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NASA Chief: "We Just Built Antigravity Propulsion!”

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NASA Chief: "We Just Built Antigravity Propulsion!”

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4398 segments

0:01

I've always believed there had to be a

0:03

better way to move an object from point

0:05

A to point B. There just had to be. So,

0:07

I spent two decades looking at hidden

0:09

momentum.

0:12

>> You do think you've discovered a

0:13

propulsion mechanism that can get us

0:15

interstellar travel. I take those

0:17

lifters and I put them in a plastic box

0:19

and put on a scale. You turn it on, the

0:21

thing lifts up and the weight flat

0:22

lines. Does not move at all. Still about

0:25

200 microns of force still inside.

0:30

>> How many variations of this experiment

0:32

do you think you've tried? We are close

0:34

to 2,000

0:34

>> 2,000 instances of the experiment or

0:36

2,000

0:37

>> 2,000 variations.

0:39

>> Holy

0:39

>> Two test articles. Each one is tested

0:41

multiple times.

0:43

>> If you were to apply that to like a

0:45

satellite in space in a zero gravity

0:47

environment, it would accelerate with

0:49

the power off. Can't explain that to the

0:52

scientific community. I just can't.

0:54

>> The idea that you could just charge it

0:55

up and leave it there and it gets

0:57

thrust. Like it hurts my brain to even

0:59

imagine how is that possible.

1:01

>> These are very weird things.

1:04

>> It's like you create this thrust mode

1:06

that just keeps going.

1:07

>> I don't think I'm bending spaceime.

1:09

Maybe.

1:12

>> For over a century, humanity's journey

1:14

to the stars has been held hostage by a

1:17

simple, unyielding truth. Newton's third

1:20

law. For every action, there's an equal

1:23

and opposite reaction.

1:26

It's the law that powers every rocket,

1:29

every satellite, every probe we've ever

1:32

launched. And it's also the law that

1:34

keeps us trapped here on Earth. In order

1:38

to get to the closest habitable planet

1:40

in our very own Milky Way galaxy, a

1:42

place called Proxima Centauri B, it

1:45

would take you 50 to 80,000 years in a

1:47

chemical combustion rocket. You would

1:49

die before even getting 1% of the way

1:52

there. And if you somehow figured out a

1:54

way to live for thousands of years, by

1:57

the time you came back to Earth after a

1:59

trip like that, it would be totally

2:01

unrecognizable. You'd be playing out the

2:03

ending of the Planet of the Apes.

2:05

>> You maniac.

2:07

>> To go anywhere in space, you have to

2:10

carry fuel. Massive amounts of it. Over

2:12

90% of any rocket's mass at launch is

2:16

just propellant. pure fuel burned and

2:18

ejected out of the back to push the

2:20

remaining 10% forward. Launching a

2:23

rocket to get a satellite into space is

2:25

like flying a fully loaded 747 to

2:28

deliver a suitcase.

2:31

>> One of the challenges we have to solve

2:33

is orbital refilling where we dock on

2:35

orbit and transfer propellant.

2:36

>> The modern king of rocketry and Mr.

2:38

Occupy Mars himself, Elon Musk, has

2:41

publicly stated that Newton's laws are

2:44

the end all beall for space travel. For

2:46

some reason, he's quite adamant about

2:48

that.

2:49

>> Uh there's no way around Newton's third

2:50

law really. You you basically have to

2:53

expel mass.

2:56

>> The original godfather of American

2:58

rocketry, Jack Parsons, believed this as

3:01

well. In 1936, he and some colleagues at

3:04

Caltech began launching the first rocket

3:06

tests in western Pasadena.

3:09

But what most people don't know is that

3:11

a decade before Jack Parsons in the

3:13

1920s, there was someone else at Caltech

3:16

with some very different ideas for deep

3:19

space travel.

3:20

>> Towns and Brown.

3:21

>> Townsen Brown.

3:22

>> Towns and Brown.

3:22

>> Towns and Brown.

3:23

>> There's a guy named Towns and Brown.

3:25

>> Okay. Okay. Towns and brown. Brown had

3:27

stumbled onto something that mainstream

3:29

science still refuses to acknowledge.

3:33

A possible break in Newton's laws. A new

3:36

force or perhaps a way to manipulate

3:39

gravity itself with electromagnetism.

3:43

Unifying these two fundamental forces

3:45

has been the holy grail of physics for

3:47

the last century. What Einstein died

3:50

searching for.

3:53

Towns and Brown discovered that when you

3:54

apply a high voltage to certain

3:56

asymmetric capacitors, they produce

3:59

thrust. No fuel, no exhaust, no

4:02

propellant, just electricity converted

4:05

directly into motion. A new model for

4:08

space propulsion that could eliminate

4:09

crude chemical combustion forever.

4:14

Brown called his anti-gravity work

4:16

electrogravidics. Meanwhile, physics

4:18

textbooks called it impossible. And

4:21

because of that, he was dismissed,

4:23

ridiculed, and eventually erased from

4:25

the official story of physics.

4:29

But if you dig a bit deeper and read his

4:32

incredible biography by Paul Shatskin,

4:34

you start to piece together a very

4:37

different picture. One in which Townsen

4:39

Brown isn't easily dismissed as an

4:41

amateur quack. In fact, his work was

4:44

witnessed by the highest levels of

4:46

government and military. Now, we're

4:48

getting into some interesting territory.

4:50

People like notorious Air Force Chief of

4:52

Staff Curtis Lame, who courted Brown

4:55

constantly. People like Edward Teller,

4:57

the father of the hydrogen bomb. Bill

4:59

Lear, the founder of the first private

5:01

jet, and Agnu Bonson, founder of the

5:04

Institute of Field Physics at North

5:06

Carolina. A lieutenant colonel from

5:08

Wright Airfield who went on to become a

5:09

general named Victor Bertrandius

5:12

witnessed Brown's gravitator experiments

5:14

in Los Angeles in 1952. He was quoted as

5:17

saying, "Believe it or not, I think I

5:19

just saw a flying saucer and it

5:21

frightened me."

5:24

And if that's not all, we have audio of

5:26

a deathbed confession from French

5:29

aerospace executive Jacqu Cornon, who

5:31

witnessed Brown's successful experiments

5:34

in a vacuum chamber in 1956 in Paris,

5:37

explicitly stating he witnessed a

5:40

positive result.

5:41

>> So that was a positive result.

5:44

>> This is to go along with an 12 page

5:47

report around that specific experiment

5:49

that's widely available online today.

5:53

Nonetheless, stigma, tech protection,

5:56

and scientific suppression are all very

5:59

real. Brown's work is still likely

6:01

classified by the Navy to this day. Over

6:05

the last 70 years, Brown's experiments

6:07

never went away. They just went

6:09

underground. They've been replicated all

6:12

over the world in places as far as

6:14

Japan, but usually by persistent

6:16

hobbyist teams or aerospace engineers

6:19

stringing some funds together and

6:21

operating out of pure passion. But in

6:23

deep black American aerospace, I believe

6:26

Brown's work still exists in the form of

6:29

whispers and vital subcompartments where

6:32

it gets explored further. Okay, so

6:35

that's the backdrop. Newton has us stuck

6:37

on Earth. Industry titans like Elon

6:40

can't be bothered to explore new

6:42

propulsion modalities and towns and

6:44

Brown is a total ghost relegated to

6:46

quacky UFO circles. That is until today.

6:51

Inside a quiet lab in Florida, NASA's

6:53

lead electrostatic scientist, a man

6:56

named Dr. Charles Buer has been running

6:59

the same gravity altering tests as

7:02

Thomas Townsen Brown. When we see about

7:05

0.1 g that corresponds to about 1 mill

7:08

of thrust

7:09

>> only this time with modern instruments

7:12

more rigorous controls and decades of

7:15

electrostatics expertise from his work

7:17

at Kennedy Space Center behind him. And

7:20

what he's measuring is thrust. Real

7:23

repeatable directional thrust. No

7:26

combustion, no reaction mass. The future

7:29

of space travel. We say we have an

7:31

energy crisis. Oh my god, the energy

7:32

crisis. Well, it could be considered an

7:35

energy crisis, but it's really a force

7:37

crisis. It's a transportation crisis.

7:39

How do you get an object from here to

7:41

here?

7:43

>> At his company, Exodus Propulsion

7:45

Technologies, Beller isn't just

7:47

replicating Towns and Brown's work. He's

7:49

validating it, scaling it, showing

7:52

literal weight loss on scales due to

7:54

upward thrust. Again, Pewer is not some

7:57

mid-level guy at NASA. He's the lead

8:00

electrostatic scientist in the entire

8:03

agency.

8:04

>> And you're also, I believe, about to be

8:05

the president of the electrostatic

8:07

society, too.

8:08

>> That's correct. And he's contributed two

8:11

fundamental principles to the field of

8:13

electrostatics that are now widely

8:15

accepted. The question is no longer

8:17

whether the Bfield Brown effect is real

8:20

or not. The question is where could this

8:22

lead humanity? How can we scale this up?

8:25

And what is the theoretical physics

8:27

behind it? On this last question,

8:30

Charles goes deeper on this show than he

8:32

has in any other interview on his own

8:36

quantum electronamics based theory

8:38

around how this force works. And I

8:40

brought in my friend, a brilliant MIT

8:42

trained physicist named David Chester to

8:45

help stress test and sharpen Beller's

8:47

theory. What happens when propulsion no

8:50

longer requires fuel? When the tyranny

8:52

of rocket equations finally breaks?

8:55

Without further ado, please welcome this

8:56

week's amazing American alchemist, NASA

9:00

and Exodus Propulsion's very own Dr.

9:03

Charles Buer.

9:05

>> Ignition sequence.

9:08

>> How is this possible?

9:11

>> Nothing too unusual about that.

9:15

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12:40

I'm here with Charles Beller who uh this

12:43

is a holy grail interview for me. I'm

12:44

like a kid on Christmas because it's

12:48

been like the search for Beller. Uh ever

12:50

since uh you know we connected a couple

12:52

years ago cuz I made this Towns and

12:55

Brown documentary and as you know and my

12:57

audience knows I'm obsessed with this

12:59

mid-century inventor Thomas Towns and

13:01

Brown. I think he found a real force

13:04

that lies outside of either the four

13:06

fundamental forces might have merged

13:08

gravity and electromagnetism. I don't

13:10

quite know but something that transcends

13:14

kind of our chemical combustion

13:15

modalities that will take us

13:17

interstellar. And as soon as I came out

13:20

with that, bunch of people hit me up and

13:22

they're like, you got to talk to Charles

13:24

Beller. He's the lead electrostatic

13:27

scientist at NASA and he's been doing

13:30

this experiment, but his own kind of

13:32

version of it, his updated, better

13:34

version of it, uh, in a vacuum chamber

13:36

he's had access to for a decade plus.

13:40

And so we connected a little bit. We

13:42

kind of fell off. I'm so grateful to

13:44

have you here now. Um, it's just a total

13:46

honor. Um, and you're also, I believe,

13:49

about to be the president of the

13:50

Electrostatic Society, too. That's

13:53

correct. So you have the credentials to

13:55

say if you're saying that you we found

13:57

another force you have as good of

14:00

credentials as anybody. Is that right? I

14:03

mean you don't say

14:07

you know I think I know enough about

14:08

electrostatics to say that but we're all

14:11

we're always still learning. What's your

14:13

current job title? So I am the lead

14:16

scientist of NASA's electrostatics and

14:18

surface physics laboratory at part of

14:20

swamp works at Kennedy Space Center. So

14:23

before I go on, I have to diverse to to

14:25

make everyone aware that this is not,

14:27

you know, affiliated with NASA. Any of

14:29

this work that we're doing

14:31

>> not sanctioned by NASA and it's we are

14:32

not given any um credence to NASA in

14:35

this

14:36

>> disclaimer accepted. I think maybe it's

14:38

a little bizarre that NASA wouldn't want

14:40

to immediately kind of jump on,

14:43

>> but they're probably going to be a

14:44

customer later on. They're not um we're

14:46

not working this technology at NASA.

14:48

It's not in my laboratory. We're not.

14:50

But you are, is it safe to say you're

14:51

the lead electrostatics scientist at all

14:54

of NASA?

14:56

>> I would say that. I mean, we only have

14:57

one electrostatics lab in all of NASA

15:00

and I lead it. So,

15:00

>> and you run it.

15:03

>> So, by default, yes.

15:04

>> Yeah. Okay. So, uh again, if uh this

15:08

sort of force were attributable to basic

15:10

electrostatics, you would know.

15:13

>> Sure.

15:14

>> Let's let's back up a second. And you

15:16

know that's a really impressive cool

15:18

title. What does somebody who leads

15:21

electrostatics at NASA do?

15:25

Our lab does a lot of things. Um it was

15:28

founded about 26 years ago by Dr. Carlos

15:30

Gier, a physicist who uh spent a summer

15:33

working at Kennedy Space Center. Came

15:35

back the following year and started the

15:37

lab. Um we do electrostatics at NASA uh

15:42

at Kennedy Space Center because of

15:43

incidents that occurred in the 1960s.

15:46

So, there was an incident that trapped

15:48

11 people in a spin test facility um

15:52

where they accidentally set off a

15:53

rocket, a solid rocket and uh there were

15:57

some casualties there. So, we also had

15:58

the Apollo fire that you've heard about.

16:01

So, we've lost I think 14 people to

16:03

electrostatics at NASA. So, Kennedy

16:06

Space Center has kind of led this effort

16:08

to study this phenomena and test it. Um

16:12

and a lot of the tests that we do that

16:14

we've been doing um date to the 1960s

16:17

long before they had standardized

16:18

testing from electrostatics. So Dr.

16:20

Carlos Kai filmed or filmed he formed a

16:23

research arm of that test um about 26

16:28

years ago when aren't there also issues

16:30

with uh lunar dust you know getting

16:33

attracted to the lunar lander and

16:35

electrostatics uh sort of allowing or

16:39

removing the dust or something like

16:40

that. Is that is that a thing?

16:42

>> Yes. So when I get on the when I on the

16:45

stand and I talk about these things on

16:48

my pedestal, I always talk about the

16:50

safety and need to study electrostatics,

16:51

but no one pays us to study

16:53

electrostatics. You know, it's a case by

16:55

case thing where people will give us

16:57

funding to look at and investigate just

16:58

like any other investigation.

17:01

But doesn't pay the day, you know,

17:03

doesn't pay the bills. So what we've

17:05

done is we've understood some of the

17:07

needs for NASA that are in the

17:09

electrostatics um realm. For example,

17:12

the dust mitigation aspect. So dust is

17:16

considered one of the two greatest

17:18

challenges that have to be overcome uh

17:20

for long-term human presence on the moon

17:22

>> or Mars. The dust was uh um was very

17:27

problematic for the Apollo astronauts

17:29

where they couldn't even do a fourth

17:30

EVA. They could do three, they couldn't

17:32

do four. dust would clog the the suits

17:34

and get into the to the arms into the

17:37

helmet into the into the joints and it

17:40

just prevented uh further you know EVAs

17:44

extra vehicle activities. So the dust

17:47

mitigation is a serious one. It's taken

17:49

by NASA. I think every center is working

17:51

on it. Um but we actually have many dust

17:53

mitigation technologies that we've

17:55

developed over the years. Uh the our

17:57

primary one is the electronamic dust

17:59

shield the EDS. So, this uses a a a

18:03

surface that has embedded electrodes

18:05

inside of it that lifts and removes dust

18:07

without moving parts or gases or fluids

18:10

or anything.

18:10

>> Wow.

18:11

>> So, we can embed that into glass. We can

18:12

embed that into thermal radiators, uh,

18:14

solar panels, solar arrays, all kinds of

18:17

materials.

18:17

>> Very cool. And wasn't there recently

18:20

like a lunar dust mission?

18:21

>> That's right. So, we're almost just over

18:24

a year ago, we landed our our EDS

18:27

payload had nine EDS's on there. Uh so

18:30

there were six EDS's used to get dust

18:33

onto us so we can use our EDS to get

18:35

show that we can get it off.

18:37

>> So we tested a thermal radiator EDS and

18:39

we tested uh a glass EDS on the moon and

18:42

a camera EDS. So we tested the

18:44

technology on the lunar surface

18:46

successful.

18:48

That's amazing.

18:48

>> So you worked 25 years on something, you

18:50

finally get it to the moon and it works.

18:51

You're you're pretty happy.

18:53

>> Congratulations. Yeah, it would suck if

18:54

it didn't after 25 years. It's a lot of

18:57

sunk cost, a lot of time and uh fruit

19:00

and energy. One other very credibility

19:03

enhancing thing about you uh that I

19:05

think it's really important to note is

19:07

you've contributed to the field of

19:10

electrostatics outside of this anomalous

19:13

force that you're talking about. Is that

19:14

right? That's right. So, you know, I've

19:17

been in electrostatics for 26 years and

19:19

it's um it's been around obviously for a

19:22

very long time, but it doesn't get the

19:24

attention that the other scientific

19:26

disciplines get. I don't feel uh it

19:29

shouldn't be the case where I come in

19:31

you know as a young kid uh and I should

19:34

not be discovering phenomena in

19:35

electrostatics you know like I did with

19:37

the

19:39

showing that there's no brush discharges

19:40

in high vacuum conditions high vacuum

19:43

conditions I know obviously people don't

19:44

have access to that but it was not you

19:48

know generally accepted that this did

19:49

not happen under vacuum you know pulling

19:51

off charges from an insulator we know

19:53

that happens very well in air why

19:55

doesn't that happen in in high vacuum

19:56

when We were able to show that you

19:58

cannot get the brush discharges the way

20:00

you do in vacuum as you do air.

20:03

It's more of a gas breakdown effect,

20:05

which could be, you know, expected, but

20:07

it was never shown. So, it's a little

20:09

bit surprising.

20:10

>> And you were the first person that

20:12

showed that

20:13

>> as far as I can tell. Yeah.

20:15

>> In the literature.

20:17

>> So, and that's, you know, obviously

20:18

because I had interest to do that for

20:20

the NASA mission. Um, not a lot of

20:23

people want to do electrostatics in high

20:25

vacuum, but it's something I love to do

20:27

every day,

20:29

>> clearly.

20:29

>> Um, and the other phenomena that I

20:32

discovered, which I thought would be

20:35

child's play for sure,

20:38

>> would be the fact that if you take a vat

20:40

of particles of all the same size and

20:43

tilt them,

20:45

>> they would roll over top of each other.

20:47

And the ones that do the rolling are

20:48

positive and the ones left behind are

20:50

negative.

20:52

This is very intriguing because for

20:54

particle charging dynamics, we know that

20:57

in volcanoes and wind um cloud

21:00

formation, the larger particles will

21:02

become positive and the smaller ones

21:03

will become negative. So there's a size

21:05

difference. We don't exactly know why it

21:07

occurs. But I was the first to show it

21:10

has nothing to do with size. It has to

21:12

do with dynamics. So the part the

21:14

particles that partake in the

21:15

interactions more often

21:18

will become positive than the ones that

21:20

do not. So if you have a cloud mixture

21:22

of bigger particles, giant spheres with

21:24

small particles, the bigger ones are

21:26

getting bombarded a lot.

21:28

>> So you'll have the ability to sample

21:30

more than the smaller ones. The bigger

21:32

ones will be positive and the smaller

21:33

ones will be negative. There's some

21:36

basic band theory reasons why that might

21:39

happen, surface state theory, but no

21:41

one's ever showed that. What are the

21:43

practical implications of both of those

21:46

kind of more conventional contributions

21:48

to electrostatics?

21:49

>> Probably um maybe electrostatic

21:52

beneficiation. That's where you separate

21:53

materials. We do that a lot of times

21:55

when we separate plastics. When you

21:57

recycle them, you can chop them up and

21:59

you can tell the high density from the

22:01

low density polyethylene by tribbo

22:03

charging them together and to find

22:04

particles splitting them in a field. One

22:07

goes one way, one goes the other. So you

22:08

can separate plastics that way. There's

22:10

a lot of different uses of tribbo

22:12

charged electrostatically

22:14

charged materials um for industry.

22:18

That's one case. Obviously explains

22:20

lightning, cloud, ground lightning,

22:22

volcanoes and things of that nature. So

22:24

there's a lot of interest in in our

22:26

community on the tribal electrification

22:28

of materials especially for the moon

22:30

Mars programs. Um, how does because

22:33

you're honestly you're probably living,

22:35

you know, the dream of, you know, many

22:39

nerdy kids in their in their bedrooms

22:41

right now, you know, thinking about NASA

22:43

and uh, you know, working in, you know,

22:46

sort of uh, cool physics and and and

22:49

electrostatics doing stuff for them. H

22:52

what's the how what's your journey

22:54

there? How did how did you get hooked up

22:55

with NASA, you know? Uh, yeah, that's a

22:59

long one.

23:01

Well, essentially I've always had a

23:03

fascination

23:05

um with space as a kid. I've always have

23:08

u and that didn't end when I went to

23:10

graduate school and after I graduated.

23:12

So, you know, my PhD is in theoretical

23:16

condensed matter physics. I got that at

23:18

Florida State University while working

23:20

at the National High Field Lab. And um

23:25

after that, you know, the grad students,

23:27

we went different directions. Some

23:28

stayed in academia, somewhat went, you

23:30

know, got jobs, you know, in in industry

23:32

or whatnot. And I decided to go to NASA

23:35

and there was an opening for a posttock

23:37

and the electrostatics lab under Dr.

23:39

Carlos Kay. He's trying to start that

23:41

laboratory back in Florida. I was living

23:43

in Tennessee at the time. I said, "Oh,

23:45

it's a chance to get into NASA, see what

23:47

it's about. You know what? What was

23:50

there to learn on electrostatics?

23:51

Everything's known. It's Maxwell's

23:53

equations. There can't be anything to

23:55

learn there." And when I got there, I

23:58

realized that even the most fundamental

24:01

uh studies in electrostatics were not

24:02

complete.

24:03

>> Even understanding how you rub two

24:05

materials together and you separate

24:07

them, one's plus, one's minus, how does

24:09

that even happen?

24:10

>> They didn't even know if it was the

24:11

electrons responsible, ions, material

24:14

transfer, all the above, none of the

24:15

above. So there was a lot to learn. So I

24:18

found it to be a very interesting field

24:19

of physics that that the mainstream

24:21

community doesn't care too much about.

24:23

So I I found it as a nice way to to

24:25

learn and to learn something new. Um and

24:28

that's that's what got me excited about

24:30

electrostatics once I got there. And uh

24:32

what really got me excited is it could

24:34

help people like it solve problems.

24:36

>> That's what electrostatics does. It

24:37

solves problems.

24:39

>> And it's in involved in just about every

24:41

industry

24:42

>> whether it's um you know making the dust

24:45

masks for the uh those are made by 3M

24:47

those N95 masks fighting COVID. Those

24:50

are electric filters. So you actually

24:52

make those using electrostatics and they

24:54

actually work for eight or nine hours

24:55

because they can trap those nanometer

24:57

particles.

24:58

>> You don't know these things. You

25:00

microphones are all electrostatics

25:01

properties. That's an elect. So there's

25:03

so many different fields that

25:05

electrostatics

25:06

dives into. And it was very useful for

25:09

us to as NASA go to these electrostatics

25:12

conferences where you have um the

25:14

pharmacy industry there, the biologists

25:17

are there, chemists are there. It's a

25:19

very wide open discipline because they

25:21

all need help in electrostatics and

25:23

they're all advancing that field and so

25:25

I could use what I learned there to

25:27

apply to NASA. So whether it's the EDS

25:29

technology that came from that community

25:31

or um other technologies that we learned

25:34

from that community like the

25:35

electrostatic precipitation that's air

25:37

filtration there are so many so many uh

25:40

technologies that come out of that

25:42

field. It was originally discovered by,

25:45

you know, founded by the um the

25:47

scientists at Xerox

25:48

>> back in the 70s.

25:50

>> So it has a very rich deep history in in

25:53

America in that north uh New York area

25:56

with Cornell and or not Cornell Corning,

25:59

Kodak

26:01

>> and these companies that are, you know,

26:03

very prominent back in the 60s and 70s

26:06

formed together this electrostatic

26:07

society and they uh they share that

26:09

technology with people.

26:10

>> It's fascinating. Yeah. I always found

26:12

it interesting that Towns and Brown

26:14

along with his thruster work which you

26:17

know involved you know what he thought

26:18

would lead to interstellar travel. He

26:21

also I believe was responsible for the

26:22

patents that ended up you know Sharper

26:25

Image ended up buying them and it was

26:27

like an ion you know air filter or

26:30

something and so I found that really

26:32

fascinating. Um, at what point did you

26:36

get the idea that maybe there was

26:39

another force here that could take us to

26:42

the stars and that chemical combustion

26:45

and the rockets that you don't work

26:47

maybe directly on, but you work, you

26:49

know, around with your work at Kennedy

26:51

Space Center might not be, you know, the

26:54

frontier of space travel. I always knew

26:57

there was something else, something more

27:00

than just Newton's laws. So I kind of

27:03

tailored my career uh just to try and

27:05

understand physics enough to see if this

27:08

to see if something else could be done

27:11

just anything. So this goes way back

27:13

into high school. So I started doing

27:16

tests in high school. I started doing

27:17

tests in college. I built rigs in

27:20

graduate school. So it never really

27:22

ended. But so I continued to do it. But

27:25

it's hard to say when did it start. I've

27:28

always believed it. just a belief that

27:30

there had to be a better way to move an

27:31

object from point A to point B. There

27:33

just had to be. Uh Newton's laws is

27:35

great. Um relativity wasn't very useful

27:38

to me. Probably because I just didn't

27:40

know it. But but electricity and

27:43

magnetism seem to have

27:46

uh a nice appeal because, you know, it's

27:48

19th century. There had to be a 19th

27:50

century equivalent to it. Momentum

27:52

conservation had to be. M

27:53

>> so I spent I don't know two decades

27:55

looking at the conversion from um field

27:59

momentum to mechanical momentum

28:02

>> if you're familiar with that field so

28:04

essentially you know you can convert

28:07

momentum stored in the field into real

28:09

momentum they've done that in the 70s

28:12

with the angular momentum but the linear

28:14

analog to it was always hindered by a

28:16

third momentum called hidden momentum so

28:19

I went I went out on a limb and tried to

28:21

find systems that did not have hidden

28:23

momentum.

28:24

>> Fascinating. Well, we're going to dive

28:26

deep into that and your theories around

28:28

it, but

28:29

>> I think first just, you know, for the

28:31

the lay audience,

28:34

mass ejection is the current kind of

28:36

paradigm. And so it's yeah, it's

28:38

Newton's third law and it's just, you

28:40

know, you expel a ton of mass. You a lot

28:42

of these rockets like look at like, you

28:43

know, SpaceX's, you know, Starship, it's

28:46

mostly fuel uh in the rocket itself.

28:49

That's that's most of the um the tonnage

28:51

is just fuel. And then you obviously

28:53

have a, you know, a decently high

28:54

payload capacity on top of that, but

28:56

that's a very small percentage of the

28:58

overall rocket. And so it's very

29:00

inefficient from that standpoint. And

29:02

then because you have a limited amount

29:04

of fuel, you can't really get to like

29:07

Proxima Centauri B. And if you could, it

29:09

would take you 80,000 years with current

29:12

current speeds. And that's like the

29:13

closest habitable planet. So, I always,

29:16

you know, bring these things up because

29:18

even if Elon Musk were sitting in your

29:20

chair, there's no argument he would have

29:24

to defeat that's just physics, you know,

29:26

like there's there's nothing he could

29:27

say to that. And so, I think what you're

29:30

looking into is like the most, you know,

29:33

people can come back with first

29:34

principles arguments and say you're

29:36

wrong, but like it's the most important

29:38

thing

29:40

>> for space. It absolutely is. There's no

29:41

question cuz like you said 90 I think

29:43

it's 95% of the of a rocket's mass is

29:46

just fuel.

29:47

>> Yes.

29:47

>> And it's you expel it almost immediately

29:50

and then you're done with it. So then

29:52

you're just out using inertia to get you

29:55

wherever you need to go unless you have

29:56

a little bit of fuel to get back. But

29:58

you know just the amount of fuel it's

29:59

going to take to get to Mars, how many

30:01

starships it's going to take that have

30:03

to be fueled just to get to Mars. It's

30:06

just astounding. Just an incredible

30:08

amount of mass of fuel.

30:09

>> Yeah. I mean, just to the moon. Do you I

30:11

don't know if you know this, but the

30:13

Starship burns 9/10 of its fuel tank. It

30:16

goes into low Earth orbit. Then it does

30:18

buttto butt refueling with another

30:21

Starship that goes up, burns 9/10 of its

30:23

fuel tank, and then that gets disposed

30:25

of. So you end up with 2/10. You have to

30:28

do that eight more times. Then you have,

30:31

you know, a full tank, and then that

30:33

goes to the moon. And that's just the

30:34

moon. That's not even Mars.

30:36

>> Oh, it's it's astounding the numbers

30:38

I've seen. It's astounding.

30:40

>> It's doesn't seem rational.

30:43

>> It doesn't. And you never bet against

30:45

Elon. He all, you know, any engineering

30:48

feat. You know, people were saying

30:49

Starship itself wouldn't work. And the

30:51

the Pez dispenser flap that allowed the

30:54

Starlinks to come out was like, you

30:55

know, that was would get ripped off and

30:57

that there all these things they had and

30:59

it seems like it's starting to work. You

31:01

know, it has orbited Earth. Um, and then

31:05

there's still, you know, uh,

31:06

modifications and updates they need to

31:08

make. So, you know, not pouring cold

31:10

cold water on that engineering effort,

31:12

but again, I do think from a physics

31:16

perspective, from a pure design

31:17

perspective, if there is this other

31:19

force, we should obviously be looking

31:22

into it.

31:22

>> Sure. I mean, there's got to be a better

31:23

way. And I always believed ever since I

31:26

started studying science that there has

31:28

to be another way. So, even even as a

31:30

young kid,

31:31

>> Totally.

31:32

>> just it doesn't make sense.

31:33

>> Yeah, I agree. It

31:35

>> just doesn't make sense. So it's like so

31:36

I kind of just tailored my my career

31:38

just just understanding science what we

31:40

knew about it everything that I could.

31:43

>> So clearly you had this kind of

31:46

imagination and uh just preconceived

31:49

idea that maybe we could transcend the

31:52

limits of chemical combustion. Maybe

31:54

there was something sitting in

31:55

electromagnetism this 19th century

31:57

modality. describe and hopefully in

32:00

detail kind of in visceral detail the

32:02

first time you witnessed this force and

32:07

what it felt like.

32:10

I would say the first time I witnessed

32:12

it or a force

32:16

um based on a theory that I had um was

32:19

probably 2010. It's wild. So that was

32:23

2010 with my um brother-in-law, future

32:26

brother-in-law. We he we weren't married

32:28

then, but uh he was in the laboratory

32:30

working with me and I set up an

32:32

experiment and I had him run it.

32:35

Now, the other scientist I was working

32:37

on on another project, you know, thought

32:39

I was just full of BS, which is perfect,

32:42

fine. So, he did not help us at all. You

32:45

know, he's a seasoned physicist, you

32:48

know, very well known in in in his field

32:51

and um just thought I was just doing

32:53

garbage and that's fine. I don't care.

32:56

So, I still had, you know, my

32:58

brother-in-law Nathan do the experiment

32:59

in the in the laboratory. And we were

33:01

looking at a laser on a on a wall. So,

33:04

you can see small displacements force in

33:06

a in a chamber. It wasn't an air

33:08

chamber. It wasn't a vacuum chamber. And

33:10

he did the test and we saw the we saw

33:12

the laser move. Like, that's pretty

33:14

cool. It's supposed to do that, I

33:16

thought. And uh my colleague, Dr.

33:20

Clemens Sid stopped what he was doing,

33:23

went over to Nathan. Okay, you've done

33:25

this, you've done this. Okay, now we

33:26

gota do he just completely immersed in

33:28

that experiment after that.

33:30

>> Yeah. Wow.

33:30

>> It was like what is happening here? This

33:32

is really crazy. Something is weird. So

33:35

that was the first time that was very

33:36

very exciting for me cuz it was it's the

33:38

first time we all seen it and I happened

33:40

to be a world-class scientist there to

33:42

to help us, you know, it was actually

33:45

like wow what happened here.

33:47

>> So you kind of you converted him almost

33:49

at least into thinking it was worthy of

33:50

inquiry.

33:51

>> Didn't need to say anything else after

33:52

that.

33:53

That's amazing. Is he now a believer in

33:56

>> Oh, I I think so. He's seen it a few

33:58

times.

33:58

>> And what's his background?

34:00

>> Um, he is an electrostatics expert.

34:03

>> Okay.

34:04

>> He is my mentor.

34:05

>> And what's his name?

34:06

>> Dr. Sid Clemens.

34:07

>> Dr. Sid Clemens. Okay. So,

34:09

>> yeah, he is my mentor. So, that's where

34:10

I learned electrostatics.

34:11

>> That's wild. But he saw your experiment

34:13

and he was like, "Oh my god, there's

34:14

something else here.

34:15

>> There's something there. There's

34:16

something there." It's exciting. It was

34:17

an exciting moment.

34:18

>> That's incredibly exciting. Um, and so

34:20

you see this and what do you think is

34:23

the next step at that point? Cuz you

34:25

know, you see this little displacement,

34:27

this laser displacement based on this

34:29

possible force.

34:31

>> Do you design a new experiment right

34:32

after that?

34:34

We designed many experiments after that.

34:37

Um, it led us down many different paths.

34:41

>> And you know, that's kind of how this

34:42

goes. If you don't know exactly what's

34:43

happening, it can lead you down

34:45

different paths. Some were successful,

34:47

some were moderately successful, some

34:49

weren't. Really didn't hit too much

34:51

success

34:53

uh after that until I met Andrew.

34:55

Okay, here's the story with that if

34:58

you're interested. Very. So, we had a

35:01

colleague,

35:02

Andrew and I, a friend named Mike.

35:06

He knew about us working on this

35:07

independently for years and never told

35:10

us, never did. He wanted to see if we

35:13

can do it independently.

35:15

you know, like a race against I don't

35:18

know who. But

35:19

>> so he was playing dumb.

35:20

>> He was playing dumb.

35:21

>> He knew about this force and he was just

35:23

like, "Let's see how far they get."

35:24

>> He He knew Andrew was working on it. He

35:26

knew I was working on it. He just wanted

35:27

to see who was who would win the race.

35:29

>> Oh Jesus. That's like this like

35:31

Machavelian level.

35:33

>> It's like 4D chess going on

35:36

>> you know. And Mike his his excitement

35:38

was that you know how we were not we

35:40

were both working at NASA or as

35:41

contractors or or been at NASA and he

35:45

was just super excited that we were not

35:47

doing this at NASA. It's like well this

35:49

has a chance because once you get into

35:51

NASA and get in bureaucracy and get in

35:53

government there's a lot of a lot of

35:55

ways that can be hindered.

35:57

So he was loving that we decided to do

35:59

that outside of of work. Of course at

36:02

the time I wasn't working at NASA. was a

36:03

I was a consultant for Exxon Mobile.

36:06

But um

36:08

so we worked together cuz Andrew needed

36:10

an electrostatics guy. Andrew was knew

36:13

he was getting into the realm of

36:14

electrostatics.

36:17

>> So

36:17

>> what was Andrew's background?

36:18

>> Andrew.

36:19

>> Yeah.

36:19

>> Andrew Arjima. He is an engineer.

36:21

>> Okay.

36:22

>> He he's been an engineer for gosh 35

36:24

years or so.

36:25

>> And he goes by Drew.

36:27

>> Drew.

36:27

>> And he So he wasn't getting into this

36:31

via electrostatics. If if that's the

36:33

case, what what exactly was he doing?

36:35

>> Well, he he was using the term

36:37

electrovitics.

36:38

>> Oh, interesting. So, this is the Thomas

36:40

Townsen Brown.

36:41

>> So, he's in that he's in that it was in

36:44

that camp.

36:44

>> I love it. I'm in that camp.

36:48

>> I'm not exactly there, but

36:50

>> Yeah. Yeah. Yeah.

36:50

>> I might move there. We'll see. I don't

36:52

know. I'm still on the fence on the

36:54

gravitics part.

36:55

>> We'll we'll we'll we'll meet in the

36:56

middle. We'll figure it out.

36:57

>> Yeah. To me, it was a little bit

36:59

pretentious. It's like, okay, you're

37:01

doing gravity and with electromagnetism,

37:04

maybe.

37:05

>> So, you meet Drew and then what happens?

37:07

>> So, at the time I was working with the

37:10

the field momentum, converting it into

37:11

linear momentum stuff. I wasn't in the

37:14

gravity world. I was in the field

37:16

momentum world.

37:18

So, we go to Drew's house. I take my

37:20

wife and we spent, you know, four or

37:22

five hours looking at his setup, looking

37:25

what he's doing. Um

37:28

and um and I gave him a lot of pointers.

37:30

He could try this, try that, try this.

37:32

You know, all the things I would do in

37:33

electrostatics to help him along. His

37:36

experiment looked very different than

37:37

mine.

37:39

His was just a needle, high voltage

37:41

needle and a and a teflon casing.

37:44

Um

37:46

I said, you know, that's pretty

37:47

interesting. Um

37:51

if he's getting forces with that, that's

37:52

kind of interesting. I don't know how

37:53

you would until my wife told me as we're

37:57

leaving the driveway. My wife was like,

37:59

"Isn't that the same force you're

38:00

working on? Just manifest it

38:02

differently."

38:03

>> She's a physicist, too. She's the best.

38:05

>> Wow.

38:05

>> So, she like we go back and forth on

38:07

these things.

38:08

>> Is she at NASA as well?

38:09

>> She is.

38:10

>> Wow. What does she do there?

38:12

>> She's in the launch services program.

38:13

>> Cool.

38:14

>> So, she doesn't have her PhD in physics,

38:16

but um she's taken engineering physics

38:20

in undergrad and she's really good at

38:22

math. So if I need help with math, I

38:23

just give, hey, Janessa, help me with

38:25

this equation. Help me with this

38:26

integral. She'll have like a baby on her

38:28

arm. Okay, fine. You can't get I'll do

38:30

it for you.

38:32

>> That's awesome.

38:32

>> She'll come in and look at the

38:33

whiteboard. She's like, "This is not

38:34

right."

38:36

>> So, she's very smart. It's fun to bounce

38:38

stuff off her.

38:39

>> Um but uh no, she she was clear. She's

38:42

like, "No, you you should look at this

38:44

your force that you're trying to do with

38:46

his setup. See if you're working on the

38:48

same thing, just a different

38:49

>> twist." Mhm.

38:50

>> I said, "Well, that can't be right." So,

38:52

I went back to my lab and I made a

38:55

needle, but I did it differently using

38:57

what I thought would work. And I would,

38:59

you know, I put a there's videos of this

39:01

on our website. You put a a tube over

39:03

the end of the needle and you put scotch

39:05

tape on the tube. So, there's no way on

39:07

wind getting out and you shove the

39:09

needle in that tube. You encase the darn

39:11

tube. Then I cranked up my power supply

39:13

and that thing moved 3 4 feet in the

39:16

air. And I sent a video to Drew. says

39:18

and Drew's like, "Oh, I guess we're

39:20

working together now."

39:22

>> Wow. Um, so you have achieved how much

39:26

force roughly now with your current

39:28

experiments?

39:29

>> Additive somewhere to 5 to 10 million

39:32

range.

39:32

>> Okay. And so for people listening, if

39:36

you were to apply that to like a

39:38

satellite in space in a microgravity or

39:40

zeroravity environment, that would be

39:43

huge.

39:44

>> Sure.

39:45

>> You would be able to do

39:46

>> Yeah. initial markets. That's what we're

39:48

comfortable with. We're a space company.

39:50

We all work at the space agency at

39:53

different levels, not just NASA, but you

39:55

know, the peripherals. And this is where

39:57

we're comfortable with. There's

39:58

definitely uh when we say um when do we

40:01

hit unity? Well, we've hitten unity for

40:03

space, unity for moon, Mars, all of

40:06

these places. So, we can make flying

40:08

cars and the moon and Mars and all of

40:10

that. Um

40:12

>> so, it's a very exciting place to be

40:14

right now. Y

40:14

>> without any significantly huge

40:17

development,

40:18

>> it could theoretically lead to deep

40:19

space exploration. You could um help

40:23

maintain orbits for satellites where

40:25

there's orbital decay.

40:26

>> That's what that's what our hope is.

40:28

Sure.

40:28

>> Okay. And you can move these satellites

40:30

maybe um to other orbits as well. Like

40:34

there's a there's a company called

40:35

Impulse Space there. They're like, you

40:37

know, they do like kickstages where you

40:38

would move, you know, between orbits

40:41

where maybe you'd go up on SpaceX ride

40:44

share with another group of satellites,

40:46

but you'd want to move into a dedicated

40:48

orbit. You could use a thruster like

40:50

this to do something like that. No

40:53

doubt. That's what our goal is.

40:55

>> Super cool. And then what about like

40:58

replacing rockets? Could we ever do that

41:00

with this?

41:00

>> Well, if we get Earth unity, we won't

41:02

need rockets, right?

41:03

>> That's true. have to think about things

41:05

a little differently.

41:06

>> Um,

41:07

>> but could could the 10 millons of thrust

41:09

turn into Newtons of thrust and could we

41:12

end up launching things into space with

41:15

this, you know, Exodus method or this

41:18

other this

41:18

>> that is our our main goal to try to do

41:20

that, you know, that's where we the self

41:22

launcher we is what we call it.

41:24

>> Do you have blueprints around this self

41:26

launcher? Do you have a sense of the

41:28

energy requirements or anything like

41:29

that or

41:30

>> we we don't.

41:31

>> Okay.

41:31

>> But we're on the path. So, we know what

41:34

we need to do. We just have to go set

41:36

out and do it.

41:37

>> Have you gone up in over the 2,000

41:38

iterations? Have you gone up in millions

41:42

of thrust? Like,

41:43

>> okay.

41:44

>> So, you have a sense of the levers to

41:46

get more thrust.

41:47

>> There are levers and there are several.

41:49

>> Uhhuh.

41:49

>> And we're trying to optimize those.

41:51

>> And what are the primary levers? There's

41:54

like we've talked about voltage the

41:56

materials properties breakdown strength

41:58

of materials um the type of signals we

42:01

send

42:03

the physical limits on the materials

42:06

>> there's so many

42:07

>> what are the ideal materials for this

42:10

sort of experiment

42:11

>> well we're dealing with high voltage so

42:13

we need materials with high dialectric

42:15

breakdown strength but we also have

42:17

permitivity issues we have to contend

42:18

with uh geometry issues we have to

42:20

contend with static dissipation issues

42:22

we to contend with. There are a lot of

42:25

other issues and that's just the DC.

42:26

When you get to, you know, other

42:28

frequencies or you get to other exotic

42:31

types, you know, charge injection,

42:33

electrits, things can get even wackier.

42:36

>> Yeah.

42:36

>> So, um, we are looking at some of the

42:38

interesting materials now that have

42:40

other properties which going to keep to

42:41

ourselves for now, but something it's

42:43

very, very interesting for now. It's

42:45

just to see if it goes anywhere. It

42:46

could lead to nowhere. Yeah.

42:48

>> But, um, we're just looking at it.

42:49

>> Cool. You know, there's other things out

42:51

there.

42:51

>> In the Towns and Brown context, barerium

42:54

titanate and bismouth often come up. Are

42:57

either of those relevant to your

42:59

experience as well?

42:59

>> We have some some uh experiments with

43:02

barryium titanate a couple years ago.

43:04

It's a good high uh permitivity powder.

43:07

>> Mhm.

43:08

>> Um

43:10

I don't know what the results of those

43:11

were. There weren't uh

43:13

>> particularly interesting. What was the

43:14

other one you said?

43:15

>> Uh bismouth.

43:16

>> Oh, bismouth.

43:18

Yeah, I've seen bismouth a lot. Bismouth

43:19

looks like fun.

43:21

>> I would love to test with some Bismouth.

43:22

Um there's some cool things that they

43:24

found the arts parts materials.

43:26

>> Y

43:27

>> um which is kind of neat because they

43:29

had some weird geometries in there which

43:30

I would project that we would have

43:31

needed.

43:32

>> Mhm.

43:32

>> But to see that in real life already

43:34

made, oh that's kind of cool.

43:38

>> Can't wait to go test those exotics. But

43:40

that's down the road for us.

43:41

>> Y

43:42

>> we're going to try to stay focused and

43:43

do what we're good at right now and then

43:46

work on the more exotic stuff later, I

43:48

think. And so in doing these

43:50

experiments, uh, did you have access to

43:53

a vacuum chamber? Because I I feel like

43:55

it's been a lot of the the reason, you

43:57

know, everybody always questions me on

43:59

this. They're like, "This experiment

44:00

sounds very simple." Because I always

44:02

bring up the Towns and Brown experiment.

44:04

They're like, "Why has nobody done it

44:05

yet?" And I say, I give two reasons. I

44:09

say, people always try to explain it

44:11

away via the ion wind. And it's so

44:15

similar to the ion wind related

44:17

experiments that it's easy to do that.

44:18

It's always easy to say there's ambient

44:20

ionization in the vacuum. That's number

44:23

one. And then number two, access to an

44:25

industrialgrade vacuum chamber is pretty

44:27

limited and it's obviously very

44:29

expensive. And so did you have access uh

44:33

you know based on your kind of NASA

44:35

background?

44:36

Yes. You know Drew and I have access to

44:39

a chamber. He's got one at his house.

44:41

He's very resourceful. Amazing.

44:43

>> He funded it himself. It's a nice size

44:46

vacuum chamber. He also has a second one

44:48

that he's going to get online soon,

44:50

which is almost a walk-in size vacuum

44:52

chamber. So, very pricey, but hopefully

44:56

with some funding, we can get that thing

44:57

um up to par and running. Um, but yes,

45:01

we do have access to a high vacuum

45:02

chamber. That's where we do most of our

45:04

tests. And let me let's describe to the

45:06

audience why it's important that ion

45:09

wind can't get out because this is how

45:12

you know I learned about all this stuff

45:13

through Thomas Towns and Brown and he

45:16

used to do these experiments. So Thomas

45:18

Towns and Browns this super interesting

45:21

mysterious guy who pops up at extremely

45:24

high levels of aerospace. He was at the

45:26

Navy for a very long time. He was at

45:28

Martin Corporation the year that

45:30

Skunkworks was formed in 1942 or three.

45:34

Um there's a an FBI document um that is

45:38

circulated now and out about him uh and

45:41

says that he's the lead radar scientist

45:43

in the entire Navy. He knows more about

45:45

radar than anybody in the Navy. We have

45:47

a lot of evidence that his

45:48

electro-hydrodnamics work, you know,

45:51

this electric fields to manipulate

45:54

airflow work ended up in the B2 stealth

45:57

bomber. So you have like two out of

45:59

three things that he's talking about

46:01

definitely being legit. And then the

46:03

third thing he's saying is I've merged

46:06

electromagnetism and gravity and he

46:08

talks about electrogravidics and it's

46:09

specifically two experiments 1956 in

46:13

Paris of which we have a witness who

46:16

there's a an audio recording of a

46:18

deathbed confession in 2009. This guy

46:20

Jacqu Cornon who's a technical

46:23

consultant for Sud west which is uh you

46:26

know an aerospace corporation there. And

46:29

you know they say there is a a force

46:31

that is not only measurable in a vacuum

46:33

at 10 the -6 to but um the force exceeds

46:39

what you would ever see outside of a

46:41

vacuum. And then he does the same

46:42

experiment at the Bonson labs at the

46:44

Institute of Field Physics in North

46:46

Carolina. And it's this remarkable thing

46:49

where you have this guy two out of the

46:50

three things he's saying probably right.

46:53

you have, you know, he's dealing with

46:54

Curtis Lame and the Rand Corporation,

46:56

all these super high up people,

46:58

>> and then this Electrogravitics thing

47:01

just gets stigmatized and people just

47:03

kind of forget about it. And it almost

47:05

feels like he's trying to he has this

47:07

wounded prairie chicken routine where

47:08

he's trying to stigmatize his own work.

47:11

And so it's it's fascinating. And the

47:15

reason so this is very long-winded, but

47:17

you mentioned ion wind. The way people

47:20

write off any of these experiments,

47:22

including Thomas Towns and Browns, is

47:24

they say that uh these capacitor

47:27

experiments, especially if they take

47:29

place not in a vacuum, you end up with

47:31

ionized air. The ionized air then

47:34

bounces off of uh other air particles

47:37

and it's basically just Newton's law

47:39

taking place and then you get thrust.

47:41

And so that's very different than

47:44

showing this in a vacuum chamber or in

47:46

this case you mitigated ion ions in in

47:49

another way. Is that right?

47:51

>> Well, you kind of have to. Yeah.

47:52

Otherwise, you'll see the ion wind

47:54

thrust. So you can either cap it,

47:56

enclose it in a volume, whatever you

47:58

have to do,

47:59

>> but you don't want the ion wind to be

48:01

playing a role here.

48:02

>> Yep.

48:03

And uh one of the things that's

48:04

different about the force that we're

48:06

talking about in the iron wind force is

48:08

in terms of geometry is that the devices

48:11

will move with the wind.

48:13

>> So imagine a rocket moving in the

48:14

direction that the exhaust is.

48:15

>> That's crazy.

48:17

>> So you have to remove the eye and wind

48:20

because of the stigma from it because a

48:21

lot of scientists have tried to do these

48:23

things and they've seen the eye and wind

48:24

and

48:25

>> it's not a real force in the sense it's

48:28

not a uh propellantless force. There's

48:30

propellant there. The wind. Yep.

48:32

>> Um but the other thing is not that's a

48:34

different thing.

48:35

>> Yeah.

48:36

>> That's a completely different beast.

48:37

>> And you would be an authority in your

48:40

ability to delineate between

48:42

>> Sure. I do I do videos where I take

48:44

those um the lifters and I put them in a

48:47

in a in a plastic box and I put on a

48:49

scale.

48:49

>> Yeah.

48:50

>> And you watch the weight and you turn it

48:52

on, the thing lifts up and the weight

48:54

flat lines. Does not move at all.

48:56

>> Wow.

48:57

>> So Drew was like, "Man, I've never seen

48:58

that video before." That's conservation

49:00

momentum right there. That's what ion

49:02

wind is doing.

49:03

>> Yeah. So that's exactly like the all the

49:05

you have all these DIY videos of these

49:08

balsa wood lifters with tin foil and you

49:11

have the ions moving around the copper

49:12

coil or whatever and then you end up

49:14

with thrust. But that is not this

49:17

electrogravidic force or what you are

49:20

calling you know this this uh exodus

49:23

force or you know electrostatic

49:26

variation force whatever it is that is

49:28

different that is another force. Um so

49:31

it's important for you know any

49:32

experimental physicists who want to pour

49:35

cold water on this. And the funny thing

49:36

is Brown himself would use the

49:40

electrohydrodnamic stuff the the stuff

49:43

involving ion wind to cover for the

49:45

electrogravitics he would literally like

49:48

because it's 95% similar

49:51

>> but it's not the same thing. And again

49:52

you are in a kind of an authoritative

49:54

position in order to you know you have

49:57

the ability to delineate between those

49:58

two things. Yeah, that's important. I

50:00

>> It is really important. Yeah. Um and

50:03

it's Yeah, it's important because it's

50:04

the always the first order debunk on

50:06

this entire thing.

50:08

>> So, you do this experiment that

50:10

eliminates or controls for ion wind. I'm

50:14

assuming you since then have done a

50:16

series of experiments to control for all

50:19

sorts of other possible confounding

50:21

variables.

50:23

Yes. So, after Drew and I did these

50:26

experiments in 2016, uh I think we spent

50:28

about two years trying to package it.

50:31

Now, there's one thing to put 100,000

50:33

volts on a device and have it move

50:34

around in the room. Drew and I both knew

50:37

that was completely impractical. You

50:39

can't do anything with that cuz you have

50:40

to make something to attach it to a

50:42

vehicle, to a rocket, to something that

50:44

people have to be around.

50:46

And this this better damn well go inside

50:48

of grounded box. So, we made a lot of

50:52

effort. It took a lot of effort those

50:53

two years to get the sucker packaged up

50:54

in in a way so it can actually be

50:56

transportable and confined.

50:59

Um so that was the initial pull to to go

51:04

into to get into a system where we can

51:06

actually enclose everything. Coolant

51:08

forces are the biggest killer in vacuum

51:11

or in air. So you can you know you can

51:13

apply high voltage to something it'll

51:15

attract to the wall floors ceilings far

51:17

away. It can still do that. So you have

51:19

to make sure that everything you do is

51:21

inside a a very well-grounded Faraday

51:23

cage. So that is another one of our

51:27

our tests, checks and balances. You

51:30

know, do we have it inside of a Faraday

51:32

cage? Is it all completely housed? Is it

51:34

feels trapped within the system? Do we

51:36

spin it the other way? There's a lot of

51:37

checks and balances we have to do along

51:39

the along the along the way. So Faraday

51:41

cage would eliminate magnetic field

51:43

interference.

51:44

>> No.

51:45

>> Okay.

51:45

>> Only electric field. only electric field

51:47

interference and then you also need

51:51

vacuum chamber because is that right or

51:54

no? You don't need it. It's a lot

51:56

easier. Okay.

51:56

>> Because you get rid of the air. The gas

51:58

breaks down like like a million volts

52:01

per meter fields. So the gases start

52:03

breaking down and when they break down

52:04

they create their own charges and when

52:06

they create their own charges you can

52:08

put charges where you don't want it. You

52:10

can short. You can uh have charges

52:12

leaking around the side. It it really

52:14

messes with you. So to do things in air

52:17

is a bit more complicated than vacuum.

52:19

Vacuum you don't have to worry about

52:20

that. Moisture is the biggest killer

52:21

especially in Florida. So you want to do

52:23

stuff in in a very dry environment or

52:25

high vacuum if you can.

52:26

>> So you're saying that in a vacuum

52:28

chamber you get more thrust.

52:29

>> You could make a system work better.

52:32

Yes.

52:32

>> Interesting. Well that's Townsen Brown

52:35

also said you'd get more thrust.

52:36

>> You get more thrust because the field

52:38

limit is not 10 to the 6th anymore. It's

52:40

10 to the eth.

52:41

>> Right. So that's because it goes the

52:44

forces are related to pressure. They go

52:46

up by field squared.

52:48

>> So instead of 10 6^ squar is 10 12th 10

52:51

the 8th squar is 10 to the 16. So now

52:53

you have a much you have four orders of

52:55

magnitude potential higher thrust just

52:57

on the

52:58

>> on the exterior part of your of your uh

53:01

thrusters.

53:02

>> Yeah.

53:03

>> So there's more to draw from from the

53:04

field.

53:05

>> That's right. This is a field effect.

53:07

It's not a voltage effect.

53:09

>> It's fascinating. Yeah. It's so

53:11

interesting and it's it but it really

53:13

flies in the face of the debunkers

53:14

saying that it's attributable to ion

53:16

wind because in an environment where

53:18

there is less ion wind you are getting

53:20

more thrust and it might be due to this

53:22

field effect but still you're

53:24

controlling for the ion wind which is

53:25

what they're saying is accounting for

53:27

the thrust.

53:28

>> Yes. And you have to also when you're in

53:30

a vacuum chamber now you have a new

53:31

falsity which could be the walls of the

53:33

vacuum chamber giant metal ground. So

53:35

you want to make sure that you put your

53:37

test device, whatever it is, inside of a

53:39

Faraday cage and then you measure the

53:41

force on the Faraday cage, nothing else,

53:43

not what's inside of it. The whole box

53:45

has to move. So you got to measure that.

53:47

>> That makes sure that what you're seeing

53:49

is real. Then you got to take turn that

53:50

suck around so that you're not being

53:52

attracted to the wall through the fair

53:53

gauge. So you want to make sure you're

53:54

always going in the correct direction.

53:56

>> So describe the current kind of

53:58

state-of-the-art experimental setup on

54:00

this.

54:01

>> So that's basically what I was saying.

54:02

So we'll put it in a box. So, it'll be a

54:04

Faraday cage. A lot of ways to make

54:06

Faraday cages. Uh, ground it really,

54:08

really well.

54:09

>> Um, if you do have voltage come in from

54:11

outside or if you put the voltage

54:12

inside, you have to make sure it's

54:13

shielded really, really well. You don't

54:15

want any coolum attraction to the walls

54:16

or the housing or anything like that.

54:18

We've gotten good where we've lowered

54:20

our voltage way way down. We don't need

54:22

30 40,000 volts like we did 10 years

54:24

ago. Um, and try to keep it all

54:27

contained and then reverse it. Make sure

54:29

it works. Put it in air. See if it

54:31

works. Put it on the mass. put on the

54:33

scale, see if it works. Do the pendulum,

54:35

do the rotator, do the spinner, do

54:38

everything to make sure it's real

54:40

because we hate

54:41

>> falsities. They're they're we hate them.

54:44

We don't want them.

54:47

>> Okay. So, what we have here is a

54:49

thruster that is set on top of a scale

54:51

in room air.

54:52

>> Okay. So, what Buer is basically saying

54:54

here is that he's testing a small

54:56

experimental in-air thruster to show

54:59

that it actually works. His team puts

55:01

the thruster on a sensitive scale. Next,

55:03

they connect it to electricity, about

55:05

480 volts to be exact.

55:07

>> If you look to the bottom right of the

55:09

screen, you'll see the voltage that is

55:11

applied. You can also see the current in

55:12

the center, the electric field, and the

55:14

run time. So, this is a 42-minute video

55:16

that we sped up to 5 minutes.

55:18

>> They watch to see if the scale reading

55:20

changes as a result of the thrust.

55:22

>> We turn on the voltage here. It's about

55:23

- 480 volts.

55:24

>> When they turn the power on, the

55:26

thruster produces a tiny force. Within a

55:28

few seconds, the force starts to be

55:31

applied to the thruster, which is on top

55:32

of the scale, and it goes in the

55:34

negative direction. It's lifting up.

55:35

>> They're specifically demonstrating that

55:37

the force is real and controllable,

55:39

enough to lift about.1 g.

55:42

>> We see about 0.1 g. That corresponds to

55:45

about 1 mill of thrust.

55:46

>> When they turn the power off, the force

55:48

goes away.

55:49

>> Okay? So, we leave it on for a few

55:50

seconds and then we turn it back off.

55:52

And then you can see that it'll come

55:54

back down.

55:54

>> They repeat this to show it's not a

55:56

fluke. So what we'll do is we'll do this

55:58

again. We'll turn it back on. Get it

55:59

back up to the mill range. Let it sit

56:01

for a few seconds. So what we're showing

56:03

is that you can actually turn this force

56:04

on and off.

56:05

>> They then flip the thruster upside down

56:07

and run the test again.

56:09

>> So you'll see that here in a moment. And

56:10

the reason why we have it off the scale

56:12

itself, we do not want any attraction of

56:14

the thruster to the scale itself.

56:16

Although the fields are very very weak

56:17

and in most cases there is a Faraday

56:18

shield, we also want to make it so it's

56:20

very very far away.

56:21

>> Finally, they take full precautions to

56:23

make sure nothing else is affecting the

56:25

measurement. So, we flip the thruster,

56:26

we deionize it. Basically, we ionize the

56:29

gases. We neutralize any charge that

56:31

escapes. And then we retar the scale.

56:33

It's typical. That's what's needed for

56:35

scale testing. This thruster itself is

56:36

surrounded by ground plates. So, we try

56:38

to minimize the field that escapes. But

56:40

just in case, we neutralize it anyway.

56:42

And then we turn the voltage back on. In

56:43

this case, about 480 volts or so. Wait a

56:45

few seconds. The thrust kicks on. And

56:47

then we see the force is in the positive

56:50

direction. So, now it's being pulled

56:51

down.

56:52

>> Now, the force pushes down instead of

56:54

up. This proves that the thruster itself

56:57

is creating the force, not some outside

56:59

interference or attraction to the scale

57:02

like electrical interference or the

57:04

thruster just sticking to the scale. I

57:06

would say this video proves the force

57:08

fairly definitively to any skeptic, but

57:11

you could technically say that this

57:13

experiment requires a vacuum chamber

57:15

because open air can get ionized. Again,

57:18

ionized wind can result in thrust based

57:21

on Newton's classical laws. But 480

57:23

volts isn't nearly enough to ionize the

57:26

air. So it's kind of a moot point, but

57:28

just for good measure, here is another

57:30

variation of the experiment, also

57:32

showing thrust, this time in a vacuum

57:35

chamber.

57:36

>> What we have here is a vacuum test

57:38

highlighting actual movement in vacuum

57:40

using a dual thruster pack in the

57:42

vertical spinner orientation. And how we

57:44

measure the forces here is we have pegs

57:46

at the bottom of this stand that are

57:48

about 2 mm apart. And the deflection

57:50

once the thruster is turned on moves it

57:52

about 14 mm which corresponds to roughly

57:54

about 2.5 mtons of thrust when we turn

57:58

this device on. These devices are

58:00

actuated externally to the vacuum

58:02

chamber through a Bluetooth connection.

58:03

So they're not in contact with anything.

58:05

But the ITO walls that surround the

58:08

thruster pack shown by that clear

58:09

transparent plastic is perfectly

58:11

grounded. So that eliminates Koolom

58:13

attraction to the wall. We're also in

58:15

high vacuum so there's no ion wind

58:16

interference. Just to highlight that

58:18

these thrusters are actually developing

58:20

thrust internally not an external

58:22

effect. So power systems inside the

58:24

chamber all the high voltage is encased

58:26

uh surrounded with an indium tin oxide

58:28

sheathing and the thruster does come on

58:30

as expected and go off as expected for

58:32

these earlier versions. So that is a

58:34

nice way to show that there is actual

58:36

physical movement in high vacuum. We're

58:38

not just recording force measurements

58:40

without actually corresponding that to

58:42

real force. So, these are just two out

58:44

of the 2,000 experimental variations

58:47

from Charles Drew and the Exodus team.

58:49

If you're an experimental physicist with

58:52

a credible background, maybe you have a

58:54

PhD or you're a professor at a top 200

58:56

physics department and you're a bit

58:58

bored and interested in exotic

59:00

propulsion and you want to see one of

59:02

these experiments with me live in person

59:05

to help vet it and maybe change the

59:07

world in the process. Hit me up at

59:09

usa.alchemy@gmail.com.

59:10

alchemy@gmail.com.

59:12

Skeptics are extremely welcome. I want

59:15

people who are in good faith trying to

59:18

poke holes in the experimental setup

59:20

here.

59:22

If I were to pluck a random experimental

59:24

physicist from an elite college and

59:27

place him in front of this experiment,

59:29

the exact experiment you just described,

59:32

is there anything they could say to deny

59:35

the empirical effect that you're seeing?

59:39

I honestly don't know. I mean, as far as

59:42

we can tell in the electrostatics

59:44

community and and with my colleagues, um

59:47

because it's DC, that eliminates all the

59:50

magnetic effects.

59:51

>> So, you can get all kinds of weird stuff

59:53

happening when you have magnetics going

59:55

on, Earth's magnetic field or whatnot.

59:57

>> And DC is direct current. If you had,

59:59

are you saying if you had alternating

60:00

current, you'd have weird magnetic field

60:02

effects.

60:02

>> So, you'd have to account for any uh

60:04

fake readings with that. Yes. If you

60:07

have AC, sure.

60:08

>> Interesting.

60:09

>> AC eliminates a lot of that.

60:11

>> Yeah.

60:11

>> And then when you turn it off and it's

60:13

still there, that eliminates a lot of

60:15

that,

60:16

>> right? So now you really are scratching

60:18

your head like what is happening here?

60:20

And that's where we're at. Like what is

60:22

happening here?

60:23

>> Is there anything that they can hang

60:25

their hat on as far as being skeptical

60:27

about this actually happening or being

60:30

able to explain it away through prosaic

60:32

physics forces that are known? I mean, I

60:35

think if you look at every single

60:36

experiment, you can say, "Well, this

60:37

might be fake because of this."

60:38

>> I say, "Okay, we'll put it over here."

60:40

Oh, well, now it's maybe fake because of

60:42

this. Okay, we'll put it over here. So,

60:44

show me a rock. What about this? Okay,

60:45

now do this. Do that. So,

60:47

>> is there anything left is what I'm

60:49

trying to ask you. Like, if you had to

60:50

stress test your own

60:52

>> If there is, it's something quite exotic

60:54

that I have no idea what it what it

60:55

would be.

60:57

>> It's I I I don't know what else it would

61:00

be.

61:00

>> It's shown itself over and over again.

61:02

How many variations of this experiment

61:04

do you think you've tried sequentially

61:05

from 2010 till today?

61:07

>> We Well, since Drew and I, we've been

61:10

keeping track. We are close to 2,000

61:12

>> Oh my god. 2,000 instances of the

61:15

experiment or 2,000 variations.

61:17

>> 2,000 variations.

61:18

>> Holy

61:19

>> 2,000 test articles. Each one is tested

61:21

multiple times.

61:22

>> Wow.

61:23

>> Folders of folders. Has anybody come in

61:27

thoroughly examined your experiment and

61:30

come out skeptical? Or has everybody

61:34

that's thoroughly examined it come out

61:36

saying there's something here?

61:39

>> I would say the latter for sure. There's

61:42

something there.

61:42

>> You cannot think of one person who is

61:44

still like I spent, you know, a day plus

61:48

with the team and I still, you know,

61:50

think I can explain it with some other,

61:52

you know, force. I haven't I can't

61:56

really think of anyone.

61:57

>> Granted, there's not that been that many

61:59

people have seen it. You know, couple of

62:01

dozen or so, but

62:03

>> um but I don't think so. You know,

62:07

what's really cool though is some people

62:08

have called me up and say uh you know, I

62:11

represent an investor. I you know, I

62:13

would I would like to the investor would

62:16

like to you know, invest into your

62:18

company or whatever. I said, "Okay,

62:19

well, what you have to do is you have to

62:20

fly down. You have to see it. You put

62:22

your hands on it." Usually that's the

62:24

kind of the routine. He's, "Oh, I don't

62:26

need to do that." What do you mean? I

62:27

already built one in my garage.

62:30

I got a 1 mill. You showed us how to do

62:32

it, so I just did it.

62:33

>> Wow.

62:34

>> So, it's been the opposite. People have

62:36

been very taken into this and they're

62:37

very excited about it.

62:38

>> That's amazing.

62:39

>> So, the people with the know can do it.

62:42

And the people that have seen it, um, I

62:46

just don't know if they know what

62:47

they're seeing, but they definitely like

62:49

it. And they're probably not good enough

62:50

to vet it, I would say, because take

62:53

vetting it would take um a lot more a

62:57

lot more work. And I think it would take

62:58

a lot more expertise. We haven't had too

63:01

many, you know, other than, you know,

63:03

Dr. Clemens and there's other physicists

63:05

that have seen it that have said

63:08

anything negative about it. Um we

63:10

haven't seen any that have said it

63:11

negative, but we haven't seen it hasn't

63:13

been exposed to the entire scientific

63:14

community either. Um I think in this

63:18

field it's hard to find who are those

63:19

people like who would be interested in

63:21

it.

63:22

>> My hope is um the one thing I did want

63:24

to mention is

63:24

>> I think everybody should be interested

63:26

in it.

63:26

>> Well I think so.

63:27

>> Yeah.

63:27

>> Um

63:28

>> you know my

63:31

when we are hosting the electrostatic

63:33

society of America conference this year

63:35

my lab is um that's in Cocoa Beach

63:39

Florida and I will do a live demo of

63:41

this.

63:42

>> When is this

63:43

>> there in June? Can I come and film?

63:45

>> You can.

63:46

>> Oh, that'd be amazing. Let's go. I'm so

63:48

excited.

63:49

>> The Electrostatic Society of America is

63:50

just a the happy It's called the

63:52

Friendly Society.

63:53

>> Cool. You know, and um and this is an

63:56

electrostatic phenomena. So, you I'm

63:58

going to highlight how electrostatics is

64:00

so necessary for space

64:02

>> and propulsion is one of the things I

64:04

think it could help

64:05

>> for sure.

64:06

>> So, I'm going to mention that.

64:08

>> Why don't you submit this to peer review

64:09

and try to get it kind of academically

64:12

checked off?

64:12

>> I'm trying. Okay. It's just a very busy

64:15

person.

64:15

>> Yeah. Yeah, you're busy, but I want to

64:17

see this dstigmatized.

64:18

>> I know. I do, too. But, you know, you

64:20

know, there's the path. Um, right now

64:21

we're focused on getting the company

64:23

started so we get some funding to to

64:24

really get the forces up. That's that's

64:26

our main focus.

64:27

>> Yeah.

64:28

>> Um, the peer review and all of that.

64:30

It's going to take 20 years. So, I'm

64:31

starting that.

64:32

>> I don't know if it'll take 20 years.

64:34

>> Maybe 30.

64:35

>> What?

64:36

>> It just will. It just will. It's too

64:38

different. It's it's

64:39

>> oh because of the antibodies that

64:42

>> this is this field has been poisoned

64:44

multiple times for a century

64:46

>> you know I would say that and then I

64:49

think people are becoming more and more

64:50

open to these sorts of effects. Are you

64:53

familiar with Sunny White?

64:54

>> Sure. So, you know, he's

64:55

>> I haven't met him, but

64:56

>> he's another NASA guy, NASA Eagle Works,

64:59

and he is kind of similar to you where,

65:02

you know, he's has this kind of pretty

65:04

credentialed, impressive background, and

65:06

he's claiming to

65:08

1.5 kilovolts, you know, um powering up

65:11

a little microchip based on the Casemir

65:14

effect. Yeah. And the Casemir effect is

65:16

this long legendary kind of anomalous

65:19

effect that if you were to walk into

65:22

elite physics, you know, departments. I

65:24

don't think you'd get too many people

65:26

denying the effect itself,

65:28

>> but it's essentially two not charged but

65:31

conductive plates. And it seems like

65:33

there's some sort of maybe quantum

65:34

vacuum fluctuation thing going on

65:37

between them and the the plates attract

65:40

in this sort of anomalous interesting

65:41

way. and he's claiming to be able to tap

65:43

into that which is I hate the word zero

65:46

point energy the term you know is so

65:48

quacky but it is that and so you have

65:51

that you have beatric voral I don't know

65:53

if you're familiar with her

65:55

>> and I don't know if you're into UFO

65:57

stuff I don't want to muddy the waters

65:58

too much but um she's at Stockholm

66:01

University and she's uh you know again

66:03

like traditional astrophysics

66:06

credentials really impressive you know

66:09

uh astronomer and uh She went back and

66:13

looked at these plates from the Palomar

66:15

Observatory, which is, you know, the was

66:17

the most inuse observatory in the late

66:20

40s and early 50s. And she looked at the

66:23

plates from 49 to 57, so pre-sputnik.

66:26

And she found all these transients,

66:28

these light reflecting objects that that

66:30

are flat and uh mirrorike and uh seem to

66:35

exist somewhere probably in

66:36

geostationary orbit. So kind of like

66:38

outer, you know, Earth orbit. And these

66:40

short flashes and not streaks, they're

66:43

associated with things that are

66:45

extremely flat and extremely reflective.

66:48

>> Wow.

66:49

>> Like mirrors. And that makes it more

66:51

fun.

66:51

>> Like mirrors. And they're exactly how

66:54

all the early CIA documents would

66:56

describe UFOs. And they show up 68% more

67:00

around nuclear detonations, which is we

67:02

know UFOs are kind of attracted to

67:03

nukes. out of those 2,700 days, if

67:07

there's no nuclear test, there's a

67:09

transient on 11% of those days. But if

67:12

there's been a a nuclear test the day

67:14

before, then it's uh almost 19% of those

67:18

days have a transient. So that 11 versus

67:21

19 is about a 68% increase in risk for a

67:26

transient if you've had a nuclear test.

67:29

>> And she got that passed through peer

67:31

review. So I don't know. I think the

67:34

world is opening up to this stuff and my

67:36

hope is that uh 30 years is is a way

67:40

overestimate and I hear you. I mean the

67:42

academia is totally close-minded and

67:44

dogmatic but I think maybe sometimes you

67:47

just have to walk through the front

67:48

door, you know, you just have to like

67:49

knock and they'll let you in.

67:51

>> Well, I'm going to I'm going to be the

67:53

front door. I'm going to I'm going to be

67:54

the house that lands.

67:55

>> I love that.

67:56

>> You know, peer review in a paper, the

67:58

physics people are going to debate for

68:00

for decades.

68:01

>> Sure. I like having the the website and

68:04

and Drew and and having videos how to

68:06

make the things. Go ahead and make them.

68:07

>> Yeah.

68:07

>> If you don't believe me, go ahead and

68:08

make them in the garage.

68:09

>> Yeah. Yeah.

68:10

>> This has been very helpful. People have

68:12

done this.

68:13

>> So, you'll do this like you have like

68:14

these DIY videos where it's like go do

68:16

this at home.

68:17

>> Yeah.

68:17

>> Whoa. And where are these videos?

68:19

>> They're on our website.

68:20

>> Oh, wow. And where where is that? Is

68:22

that exoduspace.com

68:24

or what? Or

68:26

>> exoduspulsion.space.

68:28

>> Exoduspropulsion.space.

68:29

Okay. Check that out. And you've shown

68:31

your experiments with all of the

68:34

configurations that would

68:35

>> not all of them.

68:36

>> Okay.

68:36

>> We have to keep some stuff quiet.

68:38

>> Okay, cool. So, are you doing like

68:42

lateral propeller experiments or are you

68:45

doing things that involve like lifting

68:47

objects?

68:49

>> We're not lifting objects yet in Earth

68:50

gravity. Okay.

68:51

>> We're measuring the forces of these

68:52

objects.

68:53

>> Yeah.

68:54

>> And seeing how much their force can lift

68:58

as compared to Earth gravity. Got it.

69:00

So, we do have thrusters that are

69:02

theoretically capable to lift themselves

69:04

up. The the problem is all of the

69:06

hardware that goes with it, the voltages

69:09

and the powers and the wires and the

69:10

framing and all that other stuff is not

69:12

there yet. So, you have to It's like

69:15

saying your car engine um can lift the

69:18

engine, can move the engine down the

69:19

street, but no tires and no frames and

69:22

it's not very useful.

69:23

>> Sure.

69:23

>> Um but for right now, for what we have

69:25

for lunar applications, space

69:27

applications, oh, it's awesome. It would

69:29

be fantastic.

69:30

>> That's amazing. So, in microgravity or

69:32

or no gravity environments, you'll get a

69:35

ton of thrust.

69:36

>> Sure.

69:36

>> That's amazing. Um, and you're seeing

69:39

weight reduction. Is that right?

69:41

>> Well, we were saying that. Yeah. The

69:44

weight reduction would be something

69:45

we're seeing, not mass reduction. Be

69:47

careful.

69:47

>> Okay. Yeah. Yeah. Yeah. No, I I know

69:49

that gets thrown around UFO world all

69:50

the time. Like, wait, are you you're

69:52

reducing the mass of the thing?

69:54

>> It's definitely not negative mass.

69:56

>> Yeah. Yeah. Yeah. Right. But yes, you we

69:59

do those tests. We have videos. Um I can

70:01

share some with you.

70:02

>> Uh where we put stuff on a scale and we

70:04

turn it on, it gets lighter. You have

70:06

flip it over, it gets heavier. We are

70:07

going through a peer review.

70:08

>> Okay. Amazing.

70:09

>> For our second patent, the examiner's

70:12

office is doing a a thorough peer

70:14

review.

70:14

>> They're the ones uh

70:16

>> going down that path.

70:17

>> Okay, great.

70:18

>> Which is apparently equivalent to a

70:20

scientific peer review. So they're

70:21

that's what I've been told.

70:22

>> Amazing. So they're reaching out to

70:25

people that have done it, reaching out

70:26

to people have signed affidavits to say,

70:28

"Yes, I've seen it. Yes, I've reproduced

70:30

it." Blah blah blah blah. So they're

70:31

going through that process. Now,

70:32

>> what inspired you to pursue kind of more

70:34

exotic propulsion to begin with? Did you

70:36

have any childhood experiences around

70:38

this sort of stuff?

70:40

>> Yes. Yes, I did.

70:44

Um,

70:44

>> I've always had a fascination with with

70:46

UFOs. And I think it's been around a

70:48

long time, just, you know, strange

70:51

phenomena. But I think it really hit

70:52

home um I think I was 11 or 12 when we

70:56

worked our haunted house. My dad would

70:57

make haunted houses in our in our garage

71:00

in New York.

71:01

>> Really? What does that even mean? Make

71:03

haunted houses

71:06

>> built a haunted house for the um hotel

71:09

that he worked at,

71:11

>> Giant Holiday Inn, I think it was or

71:13

Hilton in uh Connecticut. And it was a

71:16

massive haunted house. And his job was

71:17

to build the whole darn thing. So he

71:19

liked that. So the next year we did it

71:21

at our house and we charged people like

71:23

50 cents to get in and go through the

71:25

haunted house and it was probably I

71:27

think it was a 9 by11

71:29

single car garage haunted house and uh

71:33

we made $1,100. That's how many people

71:35

showed up. It was crazy. It was a lot of

71:36

fun.

71:39

But you know we had haunted house and it

71:41

would go on for several weeks.

71:43

One night while I was there working it,

71:46

um, a whole bunch of cars came in the

71:48

driveway and, uh, I recognized one of

71:51

the kids getting out of the car. He

71:52

said, "Charlie, go look, look at that."

71:54

And he shows me, you know, we look up

71:56

and there's these six bright white

71:58

lights at the top of the trees just

71:59

hanging over the trees, just going over

72:01

the road, just uh, you know, not moving

72:03

very fast, just just hanging hanging out

72:06

in formation. No sound, no window,

72:08

nothing. And all these cars were

72:09

following this these lights for several

72:11

days. This happened over the course of

72:13

several days.

72:14

>> Was this like a famous UFO wave or flap

72:17

or something?

72:18

>> It was. It was in the papers and all

72:20

that jazz. Southeast New York in the mid

72:22

80s.

72:23

>> It was a lot of fun. You know, I was I

72:26

thought that was pretty cool. So, I kind

72:28

of like geared my career towards trying

72:31

to understand some of that stuff. I just

72:32

wanted to know what the heck that was.

72:34

And uh it got me interested in physics,

72:37

I think, in science in general. I was

72:38

always interested in science. Did they

72:40

look like orbs or were they were they

72:43

part of a formation or do you think they

72:44

were part of the same craft?

72:45

>> I think they were different craft. I

72:47

think they were just separate crafts.

72:50

Wow. I didn't see a solid object or

72:52

anything.

72:52

>> And so this was for days at a time. And

72:54

it

72:54

>> they would come every night. They'd come

72:55

back and they'd be in different parts of

72:57

the

72:58

>> of the city. I don't know what the heck

72:59

they were doing or why they were there,

73:01

but it was it was pretty pretty cool.

73:03

Pretty wild. It was about the same time

73:06

um

73:08

where somebody said they saw the men in

73:10

black which I thought was hysterical.

73:12

>> Wild cuz I was, you know, we were

73:14

trick-or-treating out with my friends

73:15

and we ran into another group of friends

73:17

and that group of friends said, "Hey,

73:19

these two weird guys showed up in these

73:21

1920s outfits and they said, you know,

73:26

if you see something weird, they said

73:28

just close your eyes and tell it to

73:30

land." Do you guys know what the heck

73:32

that means? I knew I knew what it was. I

73:35

said, "Where are these guys?" "They're

73:36

right over there." So, we went running

73:38

to go look for them, but I didn't find

73:39

anybody.

73:40

>> But you knew of the men.

73:41

>> I knew the phenomena. No one knew what

73:42

the men and black were from 1980s, early

73:45

' 80s. I don't think that was a a thing,

73:47

but I like to study that stuff. So, I

73:48

knew what I knew of who that was or what

73:50

that was.

73:51

>> That's fascinating.

73:52

>> So, I thought, "Oh, this is cool."

73:53

>> How How can we learn more about this UFO

73:55

flap? Does it have kind of a a name that

73:57

it's been kind of preserved by or is

74:00

there a way to search it? Or

74:02

>> you can just look at Brewster, New York.

74:03

>> Brewster, New York. Okay.

74:05

>> Probably 86 or 85, somewhere in that

74:07

range. Wild newspapers and television

74:10

almost weekly carried reports of the

74:12

sightings

74:15

from different places throughout the

74:16

area. Eyewitnesses all reported seeing

74:19

the same thing. I looked up and right

74:22

over my head virtually, it wasn't far

74:25

off. It was right over my head and very

74:26

still. Uh there was a rim of lights in

74:29

the shape of a triangle.

74:31

>> It was just a tremendous object. It was

74:33

anywhere from wing tip to wing tip about

74:35

four uh 50 or 60 yards.

74:38

>> These were very very unusual lights.

74:40

I've never seen anything like it in my

74:42

life. And so I pulled my car over and I

74:44

had to take a look.

74:46

>> But it it it was in the paper. I

74:47

remember that cuz it lasted several

74:49

days.

74:50

>> And you hinted to me that you had an

74:51

even more surreal experience.

74:53

>> That was not a surreal experience. That

74:55

was just me seeing some lights.

74:56

>> It's surreal for many people.

74:58

>> Yeah, just lights. It was lights. But

75:01

>> yeah, I had a more intense experience, I

75:05

would say,

75:07

many years later.

75:09

>> Um, my wife and I experienced this. And,

75:12

uh, this was it was pretty cool event

75:15

now that it's over. A little terrifying

75:17

at the time, but uh, we we live in Cocoa

75:20

Beach. So, we went out to the beach one

75:22

night. I would say 9:30, 10 o'clock at

75:24

night and um we're the only ones there.

75:28

It's not uncommon though back then. This

75:30

is maybe 10 years ago. And uh maybe 12

75:33

years ago.

75:35

So, we live close to the Patrick Air

75:38

Force Base.

75:38

>> Mhm.

75:39

>> Which is south of us. And uh so out in

75:42

the ocean, maybe about 3 miles outside,

75:45

south of us in the ocean. I would say

75:46

about 3 miles. We could kind of gauge

75:48

how far things are apart because we're

75:50

used to the all the rivers and they're

75:52

all three miles wide. So this is about 3

75:53

milesi out in the ocean. We see a red

75:55

light, just a beacon just bleeping.

75:59

No big deal. Just a boat.

76:02

Thousands of boats, but not that night.

76:04

There were not thousands of boats. And

76:06

uh it gets brighter and it gets

76:09

brighter. We're like, man, that's it's

76:11

getting kind of bright. What is that?

76:14

What? You know, beacons don't get that

76:16

bright. So, there's got to be a boat.

76:18

Maybe someone's in trouble. And then it

76:20

gets really bright. And then it

76:22

explodes.

76:24

So, we see this giant, I don't want to

76:27

say mushroom cloud, but it got very,

76:28

very bright.

76:31

So bright it lit up the whole beach as

76:32

far as the eye can see. Four, you know,

76:34

all the way from Cape Canaveral all the

76:35

way down. And I said, "My god, what the

76:38

heck happened there?" My wife and I were

76:40

like, "That's crazy. Clearly someone's

76:43

going to call the police and tell them

76:44

that a boat exploded. You know, we're on

76:46

the beach. We didn't have phones or

76:47

anything at the time. Like, what the

76:49

heck is that?

76:52

So, I would say 5 minutes later, wasn't

76:55

that long, 10 minutes, we see one of the

76:58

helicopters from the Air Force base go

76:59

out to it.

77:00

>> So, they get up and they they fly over

77:02

it and they hover right over it. It's

77:04

still blinking. It's not exploding. It's

77:06

still there. Still blinking. Just a nice

77:08

pace. Blink, blink, blink. helicopter

77:11

hangs over, looks at it, doesn't do

77:14

anything, goes all the way back.

77:16

So, like, well, are they going to help

77:17

the people? Are they going to, you know,

77:19

rescue them or are they going to do any

77:20

of that? Nothing. That is so weird.

77:24

That's when it got fun.

77:28

So, now as we're watching this thing,

77:30

this is about 10, 15, 20 minutes into

77:32

it, it gets closer. Still bring still

77:35

blinking. It's getting closer. It's

77:37

leaving. It's moving.

77:40

And then it gets within a mile. So is

77:42

that 3 miles to 2 miles to about a half

77:45

a mile and then somewhere at I think

77:47

about a half a mile. It's not one light

77:50

anymore. It's split into six.

77:53

And it's not just getting bright.

77:56

Um, these orange pinkish lights split

78:00

and then they started rotating

78:02

and they just started rotating like

78:04

bicycle spokes on a wheel and they kept

78:07

getting closer and they would go under

78:08

the water and come back out under the

78:10

water, come back out, under the water,

78:11

come back out like this is really weird.

78:15

And they got closer to us. So when it

78:18

got about a quarter mile or maybe a

78:19

thousand yards out, we're like, "Okay,

78:21

we're going to walk up the beach now.

78:22

This that's been fun. That's a little

78:25

bit too close." It kept following us. It

78:27

got closer. It got closer. It got

78:29

brighter. It got brighter.

78:32

And I think it was about when they got

78:34

about I wouldn't even be exaggerating if

78:36

I said 50 yards.

78:38

That close,

78:40

>> I started getting a little scared and

78:42

and I I know she was getting scared. Um

78:46

then after about 40 minutes of looking

78:48

at these lights and and trying to run

78:50

from them, but not full out sprint, but

78:52

kind of just walking super fast.

78:55

like 12 blocks.

78:57

>> It went out

79:00

and then um then we walked home

79:03

>> and it was ter it was terrifying, but it

79:05

was not super scary, but it was scary

79:09

enough cuz I didn't know what the heck

79:11

that was. That's wild. What year was

79:13

this? Probably 2013.

79:17

Okay. Somewhere in there. So, you had

79:18

already started your work on the more

79:21

exotic propulsion stuff.

79:24

>> Probably. Yeah. A couple years in by by

79:26

then for sure.

79:27

>> That's fascinating. It's so interesting.

79:29

So, you saw this thing out in the

79:31

distance and then it started to loop in

79:33

and out of the water and then and

79:36

approach you and it got to like 50

79:38

yardsish away.

79:40

>> Yeah, it got really close beyond the

79:42

waves like where the where the waves

79:43

started.

79:44

>> Did it still look like the same

79:45

amorphous light at 50 yards or could you

79:47

make out the structure?

79:48

>> There's no I couldn't see a structure.

79:50

just six or seven lights going in a

79:52

pattern. Faster, slower, faster, slower,

79:55

in and out of the water like the water

79:56

wasn't there and just it was responding

79:59

to us.

80:01

>> Really?

80:02

>> Why? So why? Cuz that's a common thing

80:04

for people to say who've had UFO

80:06

experiences.

80:06

>> It just if we went up, it went up. If we

80:09

went faster, it went faster.

80:11

>> It was mirroring it.

80:12

>> It was mirroring us. Did you get any

80:15

sort of consciousness download or feel

80:17

mentally locked in with it or anything

80:20

like that?

80:20

>> No.

80:22

>> No, I don't think so.

80:24

>> But these lights are kind of common over

80:25

there if you if you study these these

80:27

type of lights.

80:28

>> Mhm.

80:28

>> Because we live near a cruise ship, the

80:30

port. So, you'll see a lot of videos

80:31

online with these lights. Stephen Greer

80:34

takes his his group down there to that

80:36

same almost that same beach about about

80:38

40 minutes south

80:39

>> to look at and you know kind of conjure

80:43

up the lights.

80:44

>> So they and I have had other friends

80:46

since then have the same experience or

80:48

similar experience

80:49

>> which I thought was super cool cuz he

80:51

was out at the beach with his family and

80:52

they saw it late at night. They're the

80:54

only ones on the beach. They saw them

80:55

too. This is like maybe seven, eight

80:57

years later. So it's pretty weird stuff

81:00

that's happened. What do you think this

81:02

Patrick Air Force Based helicopter was

81:04

doing? Do you think it was doing recon

81:05

on this UFO or

81:07

>> I have no idea. It's so interesting.

81:10

>> The way it behaved, it was just like,

81:11

oh, it's these darn lights again. It It

81:14

didn't act.

81:15

>> But it looked like it was intentionally

81:17

dispatched from Patrick Air Force Base.

81:20

>> After that very large bright event,

81:21

which was blinding to look at is how

81:24

bright it was.

81:26

>> They addressed it and went out there and

81:28

looked at it and

81:29

>> still saw it there, you know. getting

81:31

bright, dim, bright, dim. It was very

81:33

bright still. Not blinding bright, but

81:35

it was very bright. And it just that's

81:37

good. I just went back home.

81:39

>> Do you ever get one step kookier and

81:41

say, "Why did this happen to me? Do you

81:43

Does it have something to do with the

81:45

work that I'm pursuing?"

81:47

>> You know, I don't think so. It happened

81:49

to a lot of people have seen these

81:50

things. You know, these lights, they

81:52

follow cruise ships and boats. There's a

81:54

lot of weird videos of it. So, they're

81:56

probably just chasing people. Yeah.

81:57

Yeah, if I had to guess, I don't think

81:59

I'm anything special. I'm just following

82:01

people.

82:01

>> Well, I might follow the person who's

82:04

working on interstellar propulsion a

82:06

little more disproportionately. Um, did

82:09

you know that Thomas Townsen Brown had a

82:11

very similar experience? Totally.

82:13

Catalina Island and a little orb light

82:16

approached him, literally came up to

82:18

him.

82:19

>> Towns and Brown had a UFO experience in

82:22

Catalina as a teenager. Is that right?

82:24

>> Yes. Yes. And I know the exact spot he

82:28

was where he was standing. I used to

82:30

ride my horse up that ridge. It

82:33

approached him.

82:35

It actually approached him.

82:37

>> And and he said that he learned

82:40

so much standing there with that ball of

82:43

light that he went back to his which at

82:47

what the time was he had a lab in

82:50

Pasadena that was funded by his parents.

82:53

So he had his own private lab and he

82:56

said he went to work immediately and he

82:59

worked that was that was the beginning

83:02

of his life's work and he said that

83:05

everything that he ever learned about

83:08

his work he learned instantly

83:13

>> everything.

83:14

>> Wow. So you got that's so fascinating.

83:17

>> I wish I got a download. I would have

83:18

been 10 years further ahead.

83:20

>> Yeah. Well, may maybe you've gotten a

83:21

lot of downloads and you just don't know

83:23

it. You know,

83:24

>> it's it's always interesting how, you

83:26

know, science is treated like, oh, it's

83:29

you're just figuring this out like you

83:31

figure out the last, you know, term of

83:33

an equation on a chalkboard or

83:34

something. And often if you were to

83:37

probe the scientist in many cases, I

83:39

don't know if this comports with your

83:40

experience, it's far more like

83:43

revelation. It's like, h it just hit me.

83:46

You know, it's D Rock. We were talking

83:47

about D Rock. D Rock, you know, staring

83:49

at the fire in Cambridge and just

83:51

downloading the D Rock equation or uh

83:54

Heisenberg at Elgoland uh you know,

83:57

figuring out quantum leaps and you know,

83:59

um probability matrices or whatever

84:02

around, you know, electron shells.

84:04

>> And so this is a very common experience.

84:07

I don't know if you've ever had

84:08

>> I would say yeah, some of the the math

84:10

is just very discreet. Oh, we'll try

84:12

this and big leap there and

84:14

>> Yeah. Yeah. And then months go by, oh, I

84:16

do try this. Oh, yeah, that works

84:17

better. That makes more sense,

84:19

>> whether it's experimental or

84:20

theoretical. Yeah, it doesn't it's not a

84:22

super gradual thing.

84:24

>> It it does have, you know, step

84:26

functions to it for sure.

84:27

>> I don't think if you put one of these

84:29

debunker types like Michael Shurmer or,

84:32

you know, Neil deGrasse Tyson, I don't

84:34

think if they were in front of either of

84:35

you, they would be able to beat you in

84:37

an argument. Like,

84:38

>> well, the argument to have to anyone

84:40

just go try it.

84:41

>> Go try it. Yeah.

84:42

>> Seriously, don't take my word for it.

84:44

Yes, go build this thing in your garage.

84:46

>> I think they'd be too arrogant to show

84:47

up, but I think if Neil deGrasse Tyson

84:49

were in a room with your experiment, I

84:50

don't think he could explain it. And

84:52

that seems like a really important fact

84:55

that you have one side that's like

84:57

showing an effect. You have 2,000

84:59

iterations of that effect. You are an

85:02

expert in this field. You've contributed

85:04

two, you know, really important things

85:06

to the field itself that are

85:08

conventionally now, you know, accepted.

85:11

and

85:12

you say you're getting an effect and

85:14

then you have somebody else who's just

85:16

smuggly dismissing it. Like I'm going to

85:18

go with you over the smug dismissal.

85:20

>> Well, you know, that's that's how

85:22

science works. You know, it is

85:23

inherently skeptical.

85:24

>> Yeah.

85:24

>> You got to understand everything, the

85:26

theory, the modeling, the experiment.

85:27

So, I expect it. This is why I didn't go

85:30

the peerreview route.

85:31

>> Yeah.

85:32

>> Per se. I went the other peerreview

85:33

route, which is through the

85:35

>> Well, it's a good office.

85:36

>> It's a good um that's a good attitude to

85:39

have. And uh yeah, the patent office.

85:41

There you go. Smart. Yeah. Just just

85:43

make money off it. Just commercialize

85:44

it. Just let you know. Let's just do

85:46

that.

85:47

>> And if they're wrong, there you go.

85:49

>> You win in the free market and Yeah.

85:50

Yeah. No, totally.

85:51

>> So, it's still peer-reviewed. The the

85:53

examiner's office is peer-reviewing it.

85:55

So,

85:55

>> yeah.

85:56

>> But in the meantime, I'll I'll just keep

85:58

building away. Keep chucking away.

85:59

>> Having said that, I I I like, you know,

86:01

Tom Thomas Coons talks about, you know,

86:03

in the structure of scientific

86:04

revolutions, how science moves more

86:06

around politics than it does truth. And

86:10

I do think the fact that you lead

86:12

electrostatics at NASA is this really

86:14

important thing. There is the kind of

86:17

you know uh patent you know commercial

86:21

route that you can take. You can just do

86:22

the kind of startup thing and just win

86:24

on your own. And then there's another

86:27

part of me where I'm like

86:29

you know Neil's bore didn't create the

86:32

first semiconductor company. And you

86:34

know, if you really are, you know,

86:36

contributing to fundamental physics in

86:38

the form of this new force,

86:40

I I like that you're coming on this show

86:42

and that you have videos and you're

86:44

telling people to do it at home because

86:47

it's hard to know where that even leads

86:50

and I hope you know that. Sure.

86:51

>> And so I do think um you just letting

86:54

this out in a public way I think also

86:57

will amount to a Cambrian explosion of

87:00

people working on new cool ideas. And I

87:03

think the more you let it out, the more

87:04

you become a lighthouse for like you

87:06

kind of did it first and the other high

87:08

agency people who do other variations of

87:10

what you you're doing will come to you.

87:14

And so I think it's this flywheel where

87:16

I I do think being public about it is

87:18

the really the right thing because god

87:20

forbid I mean you have like all these

87:21

other scientists that spend like uh

87:24

their lives in secrecy and then

87:26

sometimes they you know the frameworks

87:29

that they've helped establish just kind

87:31

of go away and they're still stigmatized

87:33

to this day. Towns and brown being a

87:35

great example.

87:36

>> So I agree with that. I think getting it

87:38

out there, letting people see it, this

87:41

is something that's just too important

87:42

to be bottled up completely. Let's be

87:45

fair.

87:46

>> Um, this is a new force. It's just what

87:48

it is.

87:49

>> Whether it's a gravitational force or

87:50

some other quantum mechanical effect,

87:53

um, it's too important to just say, "No,

87:55

no, no. I'm going to work on it until

87:56

I'm done, then I'll let you let you see

87:58

it at the end." That's not what this

88:00

should be.

88:01

>> Yeah.

88:01

>> You know, we need this.

88:03

>> Yeah.

88:03

>> We need it. We need it now. You know, we

88:06

we say we have an energy crisis. Oh my

88:07

god, the energy crisis. Well, it could

88:09

be considered an energy crisis, but it's

88:11

really a force crisis. It's a

88:14

transportation crisis. How do you get an

88:16

object from here to here? That is the

88:19

real problem.

88:20

>> Absolutely. And we've been flying with

88:22

Boeing 747s or equivalents uh you know

88:26

for the last 60 years. It's just crazy.

88:28

We've seen total stagnation in the world

88:31

of transportation. And so

88:33

>> so the world needs this. the world

88:35

absolutely needs.

88:36

>> If I can help, I I will.

88:37

>> Well, I I love that attitude. That's

88:39

That's awesome. Um, you mentioned a

88:42

patent, a second patent. Your first

88:44

patent, there was a national security

88:46

hold on it. Is that right?

88:47

>> We don't know.

88:48

>> Okay.

88:49

>> But it's possible.

88:51

>> What does that even mean?

88:54

Some patents apparently go through the

88:56

Department of Defense.

88:57

>> Okay.

88:57

>> Before they're released,

88:59

depending on the nature of the patent,

89:01

and some never see the light of day,

89:03

right? There's the invention secrecy act

89:05

of 1952.

89:06

>> Yeah, I believe that's that was one of

89:07

the risks that we were aware of.

89:09

>> Mhm.

89:11

>> Fascinating. Do you So this is the weird

89:13

thing about these sorts of experiments.

89:16

There is so much smoke not only from

89:18

you. I know a lot of engineers who

89:22

worked at aerospace corporations, you

89:25

know, Locky, Northrup, those sorts of

89:27

companies. And they give you a little

89:28

wink wink nudge nudge. They often can't

89:30

say that there's anything to, you know,

89:32

the Biffield Brown experiment, but you

89:35

know, it's often you're on the right

89:37

path, buddy. And there's weird things

89:39

happen with high, you know, electric

89:41

field strengths at short distances and

89:43

with, you know, big gradients or, you

89:46

know, asymmetry, you know, that of that

89:48

always comes up and it is there's

89:51

something going on. Am I am I wrong to

89:54

say this? Cuz look, a lot of the physics

89:56

is above my pay grade, but there is just

89:59

an overwhelming amount of circumstantial

90:01

evidence that there's a there there

90:03

here.

90:05

It seems like that. Have you met others

90:07

who've probably converged um across the

90:12

same force that you have? They've

90:13

they've kind of stumbled onto it.

90:16

I have to think about that. I can't

90:17

think of anyone off the top of my head.

90:20

Um

90:22

but it's possible. I to be fair I

90:24

haven't done that much research on the

90:26

electrogravitics and all those folks. I

90:28

started reading some of the books

90:29

>> and there are a lot of books on this

90:31

stuff.

90:31

>> Yeah. Yeah. Yeah. Oh there are ton ton

90:33

of these books

90:34

>> and everyone has a theory and I just try

90:36

to have to sip through that to see where

90:37

are the experiments you know cuz you

90:40

know the old adage is everyone

90:42

>> everyone has a theory but no one

90:43

believes a theory.

90:44

>> Yeah. Yeah. Yeah.

90:44

>> But the experimentter doesn't believe

90:46

his own experiments but everyone

90:47

believes the experiments. But if you

90:48

look at how science gets pushed forward

90:50

to me the experimental physics is a

90:53

bigger tell that the theory is like a

90:55

prison or something. And so I I never

90:57

like you know this can't work because

91:00

theory like I think it's

91:02

>> this worked and we have to explain it

91:05

with a new theory and it's like the

91:06

casemir effect or like some maybe the

91:08

casemir effect makes sense in quantum

91:10

electronamics. I don't know but there

91:12

are a lot of these you know what's a

91:14

good example like black body radiation

91:16

in the 1860s with Gustav Kirchov it was

91:19

should have produced this ultraviolet

91:20

catastrophe and it didn't and it was

91:24

because of you know quanta which plunk

91:27

discovered 40 years later and so there

91:29

are a lot of these sorts of examples and

91:31

you can't say the anomaly isn't right

91:34

because of the theory and there's just

91:37

so much anecdotal evidence around this

91:40

anomaly

91:41

working. Yeah. I I think there are

91:43

examples. I gave some of those in the

91:44

ape.

91:45

>> Some of the examples of what this how

91:46

this force may manifest, you don't even

91:48

know that you're seeing it

91:50

>> like momentum anomalies for spacecraft

91:52

when they go around the earth

91:53

>> and they get to the Van Allen belts.

91:55

They either speed up or they slow down

91:57

just by going through the picking up

91:59

charge as they go through the Van Allen

92:00

belts, which doesn't make a lot of

92:02

sense. So they have to actually add

92:03

extra fuel to spacecraft to account for

92:05

that. They don't know where it comes

92:06

from.

92:06

>> That's fascinating. So there's all kinds

92:08

of things like that. So those momentum

92:10

anomalies are possibly attributable to

92:13

this force.

92:14

>> I I think so. It's possible.

92:16

>> And you're calling this the Exodus force

92:18

and your company is Exodus space.

92:20

>> That's right. Okay.

92:21

>> Yeah. The force is really two forces.

92:24

>> There's a surface force and a volume

92:26

force. We call the surface force.

92:28

>> That's actually electrostatic pressure

92:29

force

92:30

>> um just because it comes from

92:31

electrostatic pressure. And then we have

92:33

a divergence in the E field force um for

92:37

the volume element because the integral

92:39

has a surface and a volume component at

92:40

least the classical version which is not

92:43

truly correct. It's close but it's

92:46

obviously you can't explain this force I

92:48

think in classical mechanics you have to

92:50

use quantum but it at least the

92:52

classical kind of steers you in the

92:55

right direction because you can actually

92:56

build something on that to test it but

92:59

to be fair it has to be a quantum

93:01

mechanical effect. It's not a classical

93:02

effect

93:03

>> what we're seeing

93:05

>> which has always always been known.

93:06

>> Why are you sure it's not a classical

93:08

effect?

93:10

>> Well, for one, we're not conserving

93:12

energy in the in the in the classical

93:16

world,

93:16

>> right?

93:17

>> You know, if we put something on the

93:18

scale and we turn it off,

93:21

>> it should go off. Um because the fields

93:24

are intact, the force remains. So now

93:26

we're dealing with something else. Uh

93:28

just like the kasmir effect,

93:30

>> it's dealing with something else. You

93:32

don't need power for the kasmir effect.

93:34

>> You can just put two plates in in space

93:36

and they will attract. You do not need

93:37

to add power for that.

93:39

>> It is an artifact of the structure of

93:40

the vacuum.

93:42

>> This might be another similar thing

93:45

>> just in a different light.

93:47

>> In um you know in the towns and brown

93:50

experiments involving electrogics, they

93:53

were capacitor experiments. So you had a

93:55

negative electrode, you had a positive

93:56

electrode, you had a high K dialectric

93:58

in between them.

94:00

>> The high K factor which is the ability

94:02

to store and discharge easily a lot of

94:05

you know high electric fields was this

94:07

really important factor for determining

94:09

the thrust in the experiment. Does that

94:13

make sense in the context of your

94:15

experiment?

94:16

>> Sure.

94:17

>> Okay. So usually if you have a high

94:19

capacitance you can store more charge,

94:20

right? So more charge, more energy. But

94:24

um we have to look at you know we look

94:27

at all the capacitances not just the

94:29

capacitance between the two plates. Um

94:32

we look at the fields and how you can

94:34

strengthen the fields. You know

94:35

sometimes high capacitance or high K

94:37

values high dilectric constants can

94:39

lower the fields.

94:40

>> So you want a high field depending on

94:43

where you're where you want the thrust

94:44

to be.

94:45

>> So you can tailor some of that with

94:46

capacitance just like Towns and Brown

94:49

did. Um but it is a field effect. So

94:53

those are the things those are some of

94:54

the knobs you have you have a lot of

94:55

knobs you have geometry knobs

94:57

capacitance knobs voltage knobs you have

95:00

a lot of things that we can do uh but

95:02

how you can explain this force

95:04

classically I I don't really know at

95:06

least with the conservation of energy

95:07

stuff is the you know brown would use DC

95:10

pulsing and like you know kind of high

95:13

climb rates of the voltage so that the

95:15

voltage would there'd be a steep climb

95:17

rate where it would you know increase

95:19

very very sharply is that also

95:22

consistent with your theory or

95:24

>> I don't really know. I mean, we try to

95:26

stay away from the AC stuff or the very

95:28

high slooh rate stuff if we can.

95:30

>> Yeah.

95:31

>> Damages to the plastics or damages to

95:33

the metals, damages to materials, too

95:35

many too much current. Um,

95:38

>> we we haven't explored all of the

95:40

different ways to actually enact it.

95:43

We're still exploring the DC versions.

95:45

We haven't explored all the different

95:47

ways you can apply different voltages

95:49

and different currents to it, which is

95:51

something we can we have a lot of room

95:53

in the future to improve upon, but we're

95:55

doing so many variations with all the

95:57

other parameters. We don't really need

95:58

to change the the slooh rates too much

96:01

yet.

96:01

>> Do you take issue with the term

96:03

anti-gravity or

96:04

>> I don't like anti-gravity.

96:05

>> Okay. Well, because that is that would

96:08

be like an opposite of gravity force or

96:11

>> Yeah. or the you like the

96:12

electrogravitics. It's very pretentious

96:14

to say that we're messing with gravity.

96:16

>> Yeah. Yeah. Yeah.

96:16

>> Uh even Drew calls this warp drive.

96:19

>> I'm not there yet,

96:20

>> you know. I'm not I'm not there yet with

96:22

the bending of spaceime.

96:24

>> Yeah.

96:24

>> There are experiments to check that.

96:26

>> You can use interferometry or something

96:27

like that. And I believe the Apex folks

96:29

are are looking into that.

96:30

>> So, we'll see what they find. M

96:32

>> but um I don't know if we need to I

96:35

don't think I'm betting space time with

96:36

my

96:38

my 2,000 volts and you know plates and

96:43

wires and needles. I I don't think I am.

96:45

Maybe I am, but I don't think I am.

96:46

>> But you do think you've discovered an

96:48

inroad towards uh propulsion mechanism

96:51

that could get us

96:53

>> into kind of interstellar travel and

96:55

actually deep space travel,

96:57

>> which that's amazing.

96:59

>> Yes. But I don't know if I'm bending

97:00

gravity for that or not. Sure.

97:02

>> I don't want to go there yet.

97:03

>> Yeah. Yeah. Yeah. Fair enough.

97:05

>> You know, cuz if if that's the case,

97:07

then you'll go down other paths, other

97:09

rabbit holes that I don't want to go

97:10

down. Like, oh, well, then you can make

97:12

a teleportation device or a wormhole or

97:14

this or all that other stuff.

97:15

>> Yeah.

97:16

>> Yeah. I don't I don't I'm not ready for

97:18

going down those paths yet either.

97:19

>> Have you looked into any of the other

97:21

kind of exotic physics world work?

97:24

People like Ning Lee or other people

97:26

who've claimed kind of uh weight

97:29

reduction. Have you heard about that?

97:31

There's a story about this Chinese

97:33

scientist that was working on

97:35

anti-gravity and then vanished.

97:39

>> Yeah. Real excited about the spinning

97:41

superconductor stuff.

97:42

>> Yeah.

97:42

>> Cuz that, you know, my PhD is in high

97:44

temperature conductivity.

97:45

>> Yeah.

97:46

>> And um I was like, "Oh, maybe that's

97:48

that's a way to shield gravity,

97:50

something like that." Um and then

97:52

someone I think NASA reproduced it and

97:54

they couldn't didn't see the effect.

97:56

>> Okay.

97:56

>> So I never did anything with it. It's a

97:59

very expensive experiment to do. Yeah,

98:00

>> something very large superconductor and

98:03

spinning it. Um, superconductors are not

98:05

cheap as they weren't in the '90s.

98:07

>> Um, but um I I I don't know. I haven't

98:13

seen anything that's definitive.

98:15

>> Yeah, there's this guy Pleenov at the

98:18

University of Tampir in Finland who

98:20

claims um weight reduction based on

98:23

spinning superconductors. And I believe

98:26

there might be a connection between him

98:27

and Victor Shawberger. this like World

98:29

War II uh Nazi I guess he was in

98:33

Austria. I don't want to call him a

98:34

Nazi. I he was just like a hless

98:35

scientist. But uh he had this whole

98:38

model for spinning superconductivity.

98:40

And I believe um uh Pleenoff's father

98:44

was like uh like Stacey guy who was

98:47

doing tech retrieval for the Soviets.

98:50

And so you know I think there's some

98:51

sort of lineage there. Nick Cook uh

98:53

describes this in his amazing book Hunt

98:55

for Zero Point. And um and then you have

98:58

Ning Lee popping up in the early 2000s.

99:01

It's a great book, right? Yeah, it's

99:03

awesome.

99:03

>> And then Ning Lee has Yeah, he's amazing

99:05

by the way. Everybody should read that

99:07

book. Nick Cook is a hard-headed

99:09

aviation journalist at Jean's Defense

99:11

Weekly in the UK and he just stumbles on

99:15

to all this gravity research in the 50s

99:17

and then realizes it just vanishes and

99:19

goes nowhere. and he looks through the

99:21

entire lineage and he comes to the very

99:24

interesting conclusion that there's so

99:25

much smoke there probably has to be some

99:27

fire but like never kind of finds a

99:29

smoking gun. Never knows exactly, you

99:32

know, what the there there is. Uh but

99:36

it's it's fascinating.

99:37

>> It is. He eventually is like it's

99:39

somewhere in America. It has something

99:40

to do with zero point.

99:41

>> That's right. That's right.

99:43

>> And that's where he ended it. So

99:44

>> do you think there that in the black

99:46

we've discovered some of this stuff? I

99:48

honestly don't know.

99:50

>> Has I I don't know. That's I just don't

99:53

know.

99:53

>> Has the DoD ever reached out to you? The

99:56

I guess the Department of War now or the

99:58

Pentagon or DARPA. Have any of these

100:00

organizations reached out to you?

100:01

>> No.

100:03

>> It's so strange. It's very sad. I was

100:05

hoping to be, you know, taken away and

100:06

work on some weird UFO project.

100:09

>> I know. Well, I mean,

100:10

>> hasn't happened.

100:12

>> I mean, if anybody should, you know,

100:13

deserves it. It's just It's so weird.

100:17

It's like it's like they already know

100:19

and are miles ahead and they're sort of

100:22

gaslighting and waiting for us to catch

100:24

up or they're brain dead and it's just

100:27

bureaucracy. And I don't know if you

100:29

lean on either.

100:31

>> Yeah, I I don't really know. Like your

100:33

last interview pointed out how few

100:35

physicists there were for the retrieval

100:36

program.

100:37

>> This can't add up. It's it's a twoline

100:39

proof. It defies the laws of physics. We

100:43

haven't made progress. We have no

100:45

physicists.

100:46

You know, I thought that was very

100:48

interesting because um my wife and I

100:50

were approached to help with the UAP.

100:52

NASA was doing their own UAP thing

100:54

>> and they finished one report and then

100:56

there was a second one, a second follow

100:58

on.

100:59

>> Really? Um I forget the name of the

101:01

gentleman who reached out to us said,

101:02

"Yeah, we're doing this investigation

101:04

again. I'd really like your help." I

101:06

said, "Oh, okay. Just put me in with all

101:07

the physicists." Oh, there are no

101:09

physicists. What? What do you mean

101:11

there's no physicists? Why am I the only

101:12

physicist? you know, um, and it's an

101:16

instruments group, so they're they're

101:18

they have advanced instruments to try to

101:19

capture these sensors or something I'm

101:22

not, you know, quite familiar with. So,

101:23

I I don't really have time to join that

101:25

group, but I was shocked by that, too.

101:27

Like, why are there no physicists here?

101:29

Maybe I'm missing something.

101:30

>> It's very bizarre. Yeah.

101:32

>> Like, you would think there would be

101:34

only physicists.

101:35

>> That was one of the most bizarre

101:36

conversations I've ever been a part of.

101:38

>> I was I had to watch that twice. I was

101:40

like, are are you serious?

101:41

>> Yeah.

101:41

>> Why Why wouldn't there not be any

101:43

physicists? I don't know. Either again

101:45

they've figured it out and they've are

101:47

sort of gaslighting us or they have this

101:49

limited hangout strategy where some of

101:52

the more popular physics frameworks like

101:54

you hit certain areas of it and then you

101:57

get sucked up or it's brain dead or the

102:01

UFO stuff is so weird and

102:02

consciousness-based that our physics is

102:05

so clearly kind of not equipped to deal

102:09

with it that it's like futile to even

102:11

deal with physicists. I don't know.

102:14

>> But it was weird. Did you you didn't see

102:16

my um Gary McKinnon interview, did you?

102:18

>> I was just a guy, normal guy, interest

102:20

in UFOs. Happened to have some IT

102:22

skills. Nothing genius level.

102:24

>> You hacked into the Army, the Navy, the

102:26

Air Force, the Department of Defense,

102:28

and NASA.

102:29

>> Do you know who that is?

102:30

>> Name sounds familiar.

102:32

>> So, this is a guy who he lives in the

102:36

UK.

102:36

>> Mhm. He was uh in 2001 he was like in

102:41

his girlfriend's aunt's basement at 4

102:44

a.m. smoking weed, had some IT skills

102:47

because he worked with a bank and was a

102:49

UFO nut, obsessed with UFOs, and so did

102:53

some like basic blank password fishing

102:57

techniques to essentially hack into

103:00

NASA, Navy, Army, CIA, DIA, like every

103:05

elite.

103:06

>> Is it the guy that's still trapped over

103:07

there?

103:07

>> He's still there. Yeah, because there's

103:09

a live arrest warrant out for him now.

103:11

Terresa May, former prime minister of

103:13

the UK, has finally given him kind of,

103:16

you know, safe harbor or whatever. So,

103:19

he's there. Um, but he can't he's not

103:21

allowed in the US. There's he's on the

103:23

Interpol red list. And he specifically

103:27

queried when he was when he got in, he

103:29

was like, "Oh my god, I'm in." And then

103:31

he queried the Johnson Space Center

103:33

because there were um there was a a UFO

103:36

whistleblower named Donna Hair who

103:38

worked there who saw basically images of

103:42

UFOs being airbrushed out in a specific

103:44

building, building 8 there. And so he

103:47

looked in and he saw a tic tac object

103:50

floating around the Earth like in

103:52

Earth's orbit.

103:53

>> And the hemisphere comes into view and

103:54

it's very blocky but it's kind of blue

103:57

and white. So I'm thinking it must be

103:59

Earth. And then suddenly there's a big

104:02

straight kind of silvery line that is

104:05

coming down. Then that's I guess what

104:07

they now call a tic tac but of what we

104:08

used to call cigar- shaped object.

104:11

>> And this was in the early 2000s before

104:13

David Fraver's sighting um at Nimttz.

104:16

Super wild um and interesting. And then

104:20

what so what for our purposes why I

104:22

think this was an interesting

104:23

conversation is he then stumbles upon a

104:26

list of non-terrestrial officers of

104:29

which there are 40 and which very

104:32

strange right cuz as of now if you look

104:34

at you know any of the you know uh

104:37

chatgbt anthropic any of these things

104:40

it'll tell you that we have like roughly

104:41

10 people in space like globally and so

104:44

40 people in space that's strange right

104:46

and it's the names of these 40 people,

104:49

non-aterrestrial officers, fleettofleet

104:52

transfers of these specific materials,

104:55

and a lot of the materials are highk

104:57

dialectrics. And there they seem like

104:59

these thinly layered materials. And then

105:01

there was like this one material, I

105:03

think it's like mulbadinium,

105:06

>> malibdum. Yeah, malibdinum. Yeah,

105:08

>> malibdum.

105:10

Malibdinum.

105:11

>> And malibdinum is good for like

105:14

alloying. And so we came to the crazy

105:18

conclusion on the spot that maybe there

105:20

is a microgravity

105:23

uh supply space supply chain for

105:26

materials for these highk dialectrics

105:28

which ironically those highk dialectrics

105:31

work well for these experiments for

105:35

these you know again the quacky word is

105:37

anti-gravity experiments for these

105:39

experiments showing this other force.

105:41

Okay. So, there's like a space supply

105:43

chain where humans are manufacturing

105:46

these exotic materials in space that you

105:48

literally couldn't uh make.

105:50

>> Not physically impossible on Earth.

105:51

>> On Earth. Yes.

105:53

>> That's fascinating. I don't think has

105:55

anybody ever explicitly tied together

105:58

your thing like this like we're doing

106:00

now or

106:00

>> No, this is fresh and unique.

106:02

>> I love this. And there there are

106:04

commercial companies trying this right

106:06

now. So, for anybody who thinks we're

106:07

crazy, like that's a thing. And and then

106:11

what would you do it with first in kind

106:13

of a more of you know like covert

106:15

setting? You would do it on things that

106:17

are of extremely high value. And you

106:20

know if you if you produce materials in

106:22

microgravity you know the uh kind of

106:24

signal to noise is much better. You know

106:26

there's less you know dust and

106:28

interference issues. And so you could do

106:31

things like you know atomic layering you

106:34

know way way easier. And so I wonder if

106:37

there's something like that that then

106:39

works into some of these experiments

106:41

being done.

106:43

>> I don't know if you have a take on that.

106:45

>> There's a lot there.

106:46

>> Yeah.

106:48

>> You mean Yeah. I mean, we're working

106:49

with high K dialectrics and

106:51

>> Yeah.

106:52

>> layering materials and different things,

106:54

but I have not heard of anything going

106:56

on in space manufacturing for that.

106:58

>> Okay.

106:59

>> Not on my end.

107:00

>> Okay.

107:02

>> But um it'd be very interesting. Space

107:04

manufacturing is something NASA is

107:05

trying to get more and more involved in

107:07

>> because of the some of the reasons you

107:09

mentioned.

107:10

>> Um,

107:11

>> but I'm not heard of any spacecraft

107:13

being manufactured in space.

107:15

>> I have to ask you while I have you,

107:17

what's your best argument for the moon

107:19

landing hoax people?

107:21

>> Um, I I would say that the uh uh the

107:23

lasers that are beaming back to Earth or

107:27

you can beam a there's reflectors. We

107:28

just put a new one on from Firefly. You

107:30

can send a laser, it'll come back. So

107:33

that's been there since the Apollo days,

107:35

>> but you could put a photo reflector up

107:38

there with the rover theoretically. So

107:40

it's not super concrete evidence.

107:42

>> That's not super concrete, but you know,

107:44

we do have a lot of the Apollo samples.

107:46

>> Yeah,

107:46

>> I have a 200 gram or so in my lab.

107:49

>> Do you have some moon rocks?

107:50

>> Not the rocks, the dust. The rocks were

107:52

given out to different countries and

107:53

stuff. I JC probably still has some

107:55

rocks. I don't have any rocks, but Okay.

107:57

>> It's vastly different

107:58

>> than the than the simulants that we play

108:00

with.

108:01

>> Yeah. It's It's got a very high um angle

108:04

of repose. Yeah. So, basically, you try

108:05

to turn try to flip it over and it

108:07

doesn't doesn't want to flip over. It's

108:09

very jagged. It's very different.

108:11

>> Um it's interesting stuff. There's no

108:13

doubt. It's not weathered. Yeah.

108:15

>> It's not seen a lot of moisture, you

108:17

know, those kinds of things. It's it's

108:19

different stuff.

108:20

>> Have there been any bad actors trying to

108:22

kind of come in and debunk in like a bad

108:25

faith way or

108:26

>> um

108:28

I don't think so.

108:29

>> Okay. I haven't seen any.

108:32

>> Okay.

108:32

>> Um,

108:35

no. Most of the people are, you know,

108:36

like the APE folks are, they're open.

108:37

They're open to everything.

108:39

>> How do you answer the question, why has

108:41

nobody done this yet? I mean, the the

108:44

other answer to that question is they

108:46

have, and we just listed some of the

108:48

people earlier who have actually pulled

108:50

off the experiment, but do you have a

108:52

good answer as to why it takes a bunch

108:54

of things to line up?

108:56

>> Okay. You have to have high voltage

108:57

experience.

108:58

>> Mhm. Because these tests can be lethal,

109:01

right? They have to be packaged up

109:03

properly,

109:04

>> put into a Faraday cage or you're going

109:05

to get fake positives, false positives.

109:08

They'd be attracted to walls or floors

109:10

or ceilings. You have to make sure

109:12

you're not doing that. You have to

109:14

prevent the ion wind, which is very

109:16

wellnown fun thing to make. Does give

109:19

you some uh forces, but they're not what

109:21

we're interested in. Um, so there's a

109:24

lot of facets there. And then you have

109:26

to have the technical savvy to, you

109:29

know, show it in many uh different ways.

109:30

Pendulums, spinners, rotators, force

109:33

measurements, scales, all of those

109:36

things. And each one of those can be

109:38

fooled. So you have to make sure that

109:39

you are do your due diligence and do

109:42

not, you know, get any false positives,

109:44

especially on the scales. Everything has

109:46

to be shielded pretty darn well.

109:48

>> Can I bring up another thing that I

109:50

think limits um our ability to to do

109:53

this? I think it's um the amount of

109:56

people who think it's possible that

109:58

there is another force outside of the

110:01

conventional forces and so you need a

110:02

hypothesis to get you know a positive

110:05

result in certain cases and I think if

110:07

you are so dogmatically you know

110:10

confined to you know very conventional

110:13

physics you would never even try this

110:15

experiment maybe and so you you have to

110:18

have the imagination to you know realize

110:21

that there might be a there there to

110:23

even try it in the first place. That's

110:25

right. That's right. You have to you try

110:27

to do something. If you believe in it,

110:30

try to do it like I did with the field

110:32

momentum, the linear momentum. I tried

110:34

that for 15, 20 years. I failed. But

110:37

that doesn't mean I had to give up. I

110:39

was still seeing a force even in that

110:41

even if it had nothing to do with that

110:42

theory. Uh so you keep trying. That's

110:46

the best thing I can say. You got to

110:48

keep trying. If you believe it, if you

110:50

keep trying, maybe you'll see something

110:52

here. That's the case, I think.

110:54

>> And you think that this vindicates the

110:56

work of Thomas Towns and Brown, too?

110:58

Maybe he didn't understand what he was

110:59

dealing with in the way that you do. But

111:01

if he says he understood the iron wind

111:02

like he said, like he said he did. I he

111:04

did things in oil.

111:05

>> Mhm.

111:06

>> Where you can't have iron wind,

111:07

>> then he's possibly came across it. He

111:09

might not be the only one.

111:10

>> Yeah.

111:11

>> People that have played with high

111:12

voltage with asymmetrical capacitors

111:14

been around a long time. So it's it's

111:17

entirely possible that

111:18

>> maybe Tesla

111:20

>> maybe I don't know if he did much as he

111:22

did a lot of energy stuff.

111:23

>> Yeah, I don't know either. But um

111:25

there's a actually you mentioned

111:26

transmission oil. There's a team in

111:28

Japan, um, I believe they came out of

111:31

Honda, and I think Musha is the

111:34

scientist's name, and he claims to,

111:37

they've submerged the capacitor in the

111:39

transmission oil, which, you know,

111:40

apparently doesn't ionize or at least

111:42

ionize very well, and they claim some

111:44

results, and they kind of have gone

111:46

silent, but like they never retracted

111:48

those results. That paper's still out

111:50

there.

111:51

>> So, there's so much of this.

111:53

>> There's another group I'm working with

111:54

in Germany who's reproducing this. So,

111:56

>> really? Yeah. So, it's coming. It's

111:59

amazing. Well, I'm really excited to get

112:02

into You have a whole theory about how

112:05

the thrust works in your Exodus

112:07

experiments and it involves quantum

112:09

electronamics. So, I asked you if I

112:11

could bring a friend of mine, David

112:12

Chester, who is quantum electronamic

112:15

specialist in a theoretical physicist.

112:18

And so, um, are you down to have a group

112:20

conversation? We can we can change sets

112:22

and, uh, sweet.

112:26

All right. So, we have David Chester

112:28

here who is a friend of mine. He, uh,

112:31

got his undergrad at MIT, uh, PhD from

112:34

UCLA, both in physics, and is, uh, kind

112:38

of specializes in general relativity as

112:40

well as quantum field theory. But I to

112:42

me you are the guy who is the kind of

112:46

intersection if you have kind of two

112:48

circles in a ven diagram of uh kind of

112:51

smartest and best credentialed who will

112:53

entertain all of the quacky stuff. And

112:56

so we've had long conversations about a

112:59

lot of this you know extended

113:00

electronamics and some of these weird

113:03

topological or experimental physics

113:04

effects and you really I think

113:07

understand kind of the lay of the land

113:08

as well as anybody. And I was speaking

113:11

with you uh Charles about doing this

113:13

interview and you were like I'm

113:14

developing this quantum electron

113:17

dynamical theory of how this actually

113:19

works and I was like I probably won't be

113:23

able to say anything about that but

113:25

David will. So I'm really excited to

113:27

have both of you and maybe we start with

113:30

you Charles if you could just kind of

113:32

present what the theory is and then you

113:35

guys can kind of go back and forth.

113:38

>> Sure. No, but this is a good opportunity

113:40

to uh talk to a real physicist about my,

113:43

you know, my proposed explanation for

113:46

the force that I'm seeing. So, um I

113:50

don't like to create stuff up. That's

113:52

kind of one of my mantras. I don't want

113:54

to do that. I want to use what's known

113:56

in the physics community to see if it

113:58

can explain what I'm seeing. I don't

114:00

want to be one of those guys, I have to

114:01

come up with a whole new theory. I don't

114:02

think that's necessary. Um so my

114:05

approach was to say what are the tools

114:07

we have now to try to explain this. Can

114:09

it be done within conventional physics

114:11

that we know just maybe one other step

114:14

further or something you know within the

114:16

realm of what we already know and we

114:18

have a lot of tools in quantum

114:20

electronamics. We have a lot of tools.

114:22

So I started from what I have in my

114:24

experiments basically two charges. So I

114:27

have a plus and a minus charge.

114:30

That's my starting point. I don't have

114:32

anything else. Not as far as I know. If

114:34

I'm bending spaceime or doing something

114:36

silly, that's beyond my knowledge. But

114:39

are there the tools available to

114:41

understand the forces in just knowing

114:43

what we know with QED with two charges?

114:46

QED is very very powerful. Um I found an

114:51

example of how QED can solve a very

114:54

simple problem which can be easily

114:56

solved with electronamics. So let's make

114:59

it infinitely more complicated with QED.

115:02

And that's what physicists do. Um it's

115:04

because it's a more fundamental theory.

115:06

So I started with QED to explain

115:07

Koulum's law, the force of attraction,

115:09

repulsion between two particles. So

115:11

that's very well explained with Kulum's

115:13

law. But in the context of QED, I found

115:15

a book that actually did this. In my

115:17

grad school, we were not trained how to

115:18

do that. It's not uncommon. There's a

115:20

lot of very remedial physics problems

115:22

that take two or three hours to solve

115:25

that are not going to cover in a class.

115:27

But I saw the QED version of it and I

115:28

said, "Ah, this is very helpful. I know

115:31

where it comes from. I know where the I

115:33

know where the momentum's come from. Um

115:35

and then you do the math appropriately,

115:37

you'll get Kulum's law coming out of it.

115:39

And Kulum's law for people not familiar,

115:42

can you describe it very basically?

115:45

>> So basically it shows that if you have

115:46

two particles, their force is related by

115:49

one over the square of the distance away

115:51

relation to the the charge the charges

115:54

that you have. very uh simple

115:57

rudimentary physics

115:58

>> and it explains things like electron

116:00

repulsion, two like forces repelling.

116:03

>> It basically explains everything that we

116:05

know about two particles, two charges,

116:07

just about everything. QED how atoms are

116:10

bound together and yeah so I did not

116:12

think we needed QC QCD quantum

116:15

chromodnamics

116:17

W particles Z particles I didn't think

116:19

we needed that. We're not looking at the

116:21

interactions between protons and

116:22

neutrons. So we're not looking at the

116:24

high energy um realm. We're just looking

116:26

at low energy kulomic charges.

116:29

>> And when you say you're explaining uh

116:31

the kulom charge with quantum

116:33

electronamics, how is it normally

116:36

explained?

116:37

>> Usually you'll do you know Maxwell's

116:39

equations or something simple to derive

116:41

Kulom's law. It's not very complicated.

116:43

F= QE, right? So we know the electric

116:46

field is point part point charge times Q

116:49

>> and Maxwell's equations govern

116:50

electromagnetism.

116:52

19th century.

116:53

>> That's right. Okay.

116:54

>> But what they don't tell you is how do

116:55

these particles interact? Like what's

116:56

causing them to repel or attract

116:59

>> you know what is the physical mechanism?

117:01

QED provides us a nice little solution.

117:03

QED says well thanks to quantum and or

117:06

fineman and schwinger they are

117:09

exchanging virtual particles.

117:11

>> So they're not real particles. You can't

117:13

see them. You can't observe them but

117:15

they're virtual. So basically you can

117:17

picture this is the cartoon that people

117:19

use. You have two ice skaters. One of

117:22

them is holding a bowling ball. They the

117:24

first one throws a bowling ball so they

117:26

recoil. The second person catches the bo

117:29

bowling ball so they fall back. Uh

117:31

except there's no bowling ball. So not

117:33

real one that you can see but you can

117:35

see the interaction between the two

117:36

particles.

117:37

>> And that's the fman diagram. And what

117:39

you do is each time you write a fman

117:41

diagram, each one of those lines in the

117:43

fman diagram represent a different term.

117:45

And you multiply them all up and you get

117:47

what's called the scattering matrix

117:48

element. And you can try to find how

117:50

these things interact. If you were to

117:52

take this particle A and shoot it at

117:54

particle B, you could see where it

117:55

deflects on a board somewhere. If you if

117:57

you actually measure that that

117:58

interaction is all described in that QED

118:02

using QED to solve for to derive Kulum's

118:05

law is very complicated. But I found a

118:07

book that did it. So I copied that,

118:09

looked at what they did. I said, "Okay,

118:11

this is a good model. Let me just do one

118:14

thing different.

118:16

I don't have

118:19

just kulum. I have something else. So

118:22

what I think it is and what I proposed

118:25

now is what would happen if I just went

118:28

to the next order. So quantum

118:30

electronamics at QED doing Kulum's law

118:33

is a second order equation on uh using

118:37

time independent perturbation theory.

118:39

Perturbation theory is the best tool

118:41

that we have in physics. I think bar

118:44

none. Perturbation theory it's awesome.

118:47

It's outstanding. It's very powerful.

118:48

>> What is perturbation theory? High level.

118:51

>> High level. So high level you can get

118:52

the energy states or the the the states

118:54

themselves using pertabbations. Just

118:56

change the thing you you change an

118:58

energy state. You add that back in. You

119:00

do another perturbation. You see how it

119:02

changes

119:03

>> with a small perturbation of the energy

119:04

in this case or the states and involves

119:08

so and there are many perturbations. So

119:11

I'm using second order perturbation

119:13

theory for that's the lowest

119:14

perturbation and I think the highest

119:16

perturbation for two charges in kulum's

119:18

law and after that I don't think

119:20

anyone's done anything after that

119:22

because you not only get a close answer

119:24

you get the exact answer

119:25

>> so I was like why go further you have

119:27

two particles they either attract or

119:29

repel what's cool is all do you need to

119:31

go further not so I'm like well this

119:35

force with um that I've seen with exodus

119:39

electrostatic pressure force

119:41

um is much much weaker than coolum saw.

119:43

There's no doubt much weaker. But I

119:47

decided well let's try the third order.

119:49

What does that give me? And when I tried

119:52

it with my math, which may not be

119:54

perfect, I'm sure I was I was seeing

119:56

three charges now. So basically, one of

119:59

the charges was weighed twice,

120:01

multiplied by itself, and then the third

120:03

order is being multiplied by the first

120:05

charge. So there's already an asymmetry

120:07

sort of in the charges even with two

120:09

charges which I thought was useful

120:12

because I wanted to try to get that with

120:13

classical um uh dynamics and you can't

120:17

derive that from classical energy three

120:19

charges but the QED was kind of nice to

120:22

show that. So I looked at that and I

120:24

said okay there's there's not there's no

120:26

longer four terms like there are in the

120:28

you know the second order.

120:29

>> What would classical electronamics give

120:31

you if not three? Basically when you try

120:33

to do um conservation of energy you

120:35

start with a kinetic energy and a

120:36

potential energy. And so for adding more

120:38

charges to a system you just keep adding

120:40

more and more charges to a system. The

120:41

superp position principle adds them all

120:43

up.

120:44

>> It doesn't multiply them all up. It adds

120:46

them all up.

120:47

>> But I need the addition. I needed the

120:49

the pressure that I'm creating working

120:51

on the charges that I'm creating.

120:53

>> So I have a pressure on one side charge

120:55

from the other. So I have a the

120:57

multiplication effect

120:58

>> experimentally. So I didn't know how to

121:00

drive that other than quantum

121:02

electronamics but classicalally it

121:04

doesn't doesn't show that but I thought

121:05

maybe QED might and it shows up there.

121:09

Um but that was the first thing and the

121:11

other thing there were 12 terms now

121:14

instead of four

121:16

because I'm I'm scattering. So what

121:17

happens in QED or or um time independent

121:21

perturbation theory you start from the

121:22

zero the state the vacuum state you

121:23

scatter to the first state then you go

121:25

from first state you scatter to the

121:26

second state and you go second state

121:27

scatter to the zero state. That's just

121:29

how it works. There's a lot of

121:30

scattering uh states and um matrices

121:33

that you have to solve for and you

121:35

multiply them together. So I have 12

121:36

terms. Now some of the terms are kind of

121:39

interesting.

121:40

Uh it looks like that when you draw the

121:43

diagrams

121:45

from those states that you looks like um

121:48

you get the same things you had in

121:49

second water perturbation theory where

121:51

you'll have a they'll exchange a photon

121:53

the other ones will absorb it vice

121:55

versa. Uh but there are some states are

121:57

a little weird. You'll have states where

122:00

they'll just absorb or just emit

122:03

>> kind of like the first order

122:05

>> which I don't talk about but the first

122:07

order is basically just a charge with

122:08

field line or not field line but with

122:10

basically a charge with a scalar photon.

122:14

So you have there's four kinds of

122:16

photons in QED. One of them is real. One

122:18

of them is observable. The other three

122:20

are not.

122:21

>> But um

122:21

>> two of them are real.

122:22

>> Two of them are real. I thought I only

122:23

read there's only one of them was real.

122:25

Well, you have uh h you have plus and

122:27

minus h bar for two different spin

122:29

states.

122:29

>> Oh, okay. Well, that's cool. Two of them

122:31

are real.

122:31

>> If it was massive, it would be three.

122:33

But since the photon's massless, you get

122:35

two state. I mean, light is polarized.

122:36

You can polarize it into

122:38

>> Okay. I didn't know that apply to

122:40

because I just remember the textbook

122:41

saying only one of them was real. Okay.

122:44

>> But anyway, so these are not real

122:46

things. But in QED

122:50

um you look at the vertices and every

122:52

time you draw a verticy you conserve

122:55

momentum at that point.

122:57

>> So if a particle comes in it's you know

122:59

we use these silly fiber diagrams

123:01

they're not cartisian coordinates at all

123:04

but they're basically a momentum vector

123:06

and then the momentum changes and when

123:08

the momentum changes another momentum is

123:10

created or absorbed and that's all it

123:13

is.

123:14

>> You can't think of it any more literal

123:15

than that. Um so that's what the that's

123:19

what I should you know I see in third

123:21

order third order are these vertices

123:23

that are even giving out these scalar

123:26

photons are absorbing them whatever

123:28

these things are in reality is how these

123:31

things seem to be conserving momentum if

123:33

this model is correct. So that's the

123:35

difference between the third order and

123:37

the second order. At least what I found

123:38

mathematically is that you don't absorb

123:41

this. You don't emit this scalar photon

123:44

and absorb it in the same pairing with

123:46

the two charges. There are cases where

123:48

the two charges emit and don't absorb or

123:52

>> absorb and don't emit.

123:54

>> And what is a scalar photon as opposed

123:55

to a photon?

123:56

>> It's a mathematical

123:58

photon. You can describe it better than

124:01

I can, but it has many names. dark

124:03

photons

124:04

>> and deals with different. Is it

124:05

different? I think it is. Anyway, I

124:07

think it's just it's a mathematical

124:09

term.

124:09

>> Okay.

124:10

>> It doesn't have the polarization that a

124:11

real photon has, right? Yeah.

124:13

>> Very different.

124:14

>> Yeah.

124:14

>> It's just a mathematical

124:16

>> term.

124:17

>> Mhm.

124:17

>> That you put inside the matrices and you

124:19

get the

124:20

>> I don't know how it works.

124:21

>> So, what are the what scalar?

124:23

>> It's a scaler. It's a scaler. No vector.

124:26

>> Yeah. So the idea of uh just emitting or

124:31

absorbing these scalar photons in this

124:34

third order perturbation,

124:37

how does that allow for this effect that

124:40

looks like this new force in

124:42

electrostatics or looks like

124:44

anti-gravity or you know what you're

124:46

kind of experiencing.

124:48

Well, what it shows is you have an

124:50

imbalance

124:52

>> and the system can be made to be

124:55

imbalanced,

124:57

>> which is weird. So, cuz you're not

124:59

enclosing I don't know what happens to

125:00

these scalar photons where they go or I

125:03

don't even know if they go anywhere.

125:04

They might terminate somewhere else in

125:05

the universe. I don't know. E- fields

125:07

don't do that. They do terminate

125:09

somewhere. But uh it does you know show

125:14

this weird kind of you know imparting

125:17

its momentum onto something that is

125:20

already asymmetric. So it's very odd.

125:23

>> So where you ever you have these

125:25

>> Yeah.

125:25

>> Wherever you have these

125:27

I think um that's where the field is non

125:32

zero where these things exist. Where

125:33

these things don't exist is where the

125:35

field is zero. So that's the difference.

125:37

And it's basically an electric field.

125:39

>> And super high level, you end up with

125:41

this kind of virtual particle transfer.

125:44

And due to conservation of momentum, you

125:45

end up with thrust.

125:48

>> I think so.

125:49

>> Okay. And what do you think, David

125:52

Chester? Well, first of all, I want to

125:54

commend you on your experimental

125:55

efforts. I think you're really brave

125:57

with what you're doing, and it's quite

125:59

amazing how much data you guys have been

126:01

collecting. However, I would just advise

126:03

you to be a little careful with some of

126:04

the theoretical claims you're making. Uh

126:07

first of all, it sounds like you're

126:09

saying you can get uh a momentum.

126:13

Yeah, you're getting a kick in momentum

126:14

in the center of mass frame. However,

126:16

typically in QED uh well momentum is

126:19

conserved and you still have

126:21

translational symmetry. So you're I mean

126:25

you're typically not able to

126:28

get virtual photons to give radiation.

126:33

That's the that's the first thing. So it

126:35

sounded like you were saying you you

126:37

believe that there's this scalar virtual

126:39

photon that is getting radiated out. Uh

126:42

there's I see two issues with that. The

126:45

first being first of all I mean the

126:47

scalar mode in QED is not physical.

126:50

Second of all, so you could say maybe

126:52

there's some virtual stuff going on in

126:54

that, but the virtual particles

126:57

typically refer to internal lines

126:59

whereas in the FMAN diagrams, whereas

127:02

the you know the radiation are the

127:04

external lines. So you can't have a

127:08

virtual radiation mode in QED.

127:12

So that seems to be

127:15

>> So what is

127:17

>> what is the uh

127:20

the equivalent, I guess.

127:21

>> I mean, I'm not exactly sure.

127:24

>> I don't know what's going I don't know

127:26

the best way to describe your experiment

127:28

if that's what you're getting at.

127:30

>> No, I'm just trying to figure out like

127:32

how would you draw the fineman diagram

127:34

for just a point charge and its field,

127:37

not the self energy, but just the

127:38

regular

127:39

>> Well, yeah. So, if you think about what

127:41

the electric field is, it's the force

127:43

that you would get if you had a test

127:45

charge located there. So you could

127:48

imagine exactly as you're saying uh you

127:51

know you it's a four-point tree level

127:54

scattering di Fman diagram where you

127:56

have two electrons going in two

127:57

electrons going out and you could have

127:59

it's a little subtle here because it's a

128:01

classical phenomenon but there is that

128:03

internal line and at first it becomes

128:06

virtual meaning it it can have complex

128:09

momentum that's offshell but there's

128:11

also momentum conservation as you were

128:12

saying so that when you do that thyon

128:15

diagram and you're integrating over the

128:17

momentum you get this delta function

128:19

from momentum conservation and that

128:21

basically conserves uh momentum such

128:24

that you know you get classical momentum

128:27

that can be transferred from one

128:28

electron to another and then they can

128:30

get forced apart and you know we should

128:34

it's worth mentioning you can also find

128:36

the electric field in classical

128:37

electronamics for as many charges as you

128:40

want it sound maybe I misheard you but

128:42

it sound like you were saying you can't

128:44

study things classically for three

128:46

charges or something but

128:48

>> not that multiplied together. I think

128:50

the superp position is an addition of

128:51

all the charges.

128:53

>> I also noticed so you mentioned that

128:55

you're doing time independent

128:57

pertubation theory which I didn't pick

129:00

that up. So perturbation theory yeah

129:02

mathematically it's kind of like a

129:04

tailor expansion. So the basic idea is

129:06

you can have polomials. So you could

129:08

have you know a constant term then a

129:10

linear term and then a quadratic term.

129:11

And the idea is if you're doing an

129:13

approximation, let's hopefully the thing

129:16

is small so the higher order terms can

129:17

be neglected. And then so perturbation

129:20

theory is this approximation scheme that

129:22

you can use uh to find solutions to

129:25

things. And there's different ways you

129:26

can apply pertabbation theory in

129:28

physics. Typically when you refer to

129:31

perturbation theory in quantum

129:32

electronamics,

129:34

it's not about time independence. It's

129:37

more about when you write down the fman

129:40

diagrams, you can have what they call

129:41

tree level diagrams and then loop level

129:43

diagrams. Typically the the tree level

129:47

the tree level diagrams correspond to

129:48

the classical interactions. And the

129:52

number of loops in the diagram is the

129:55

level of perturbation theory you're at.

129:57

So the language that I'm familiar with

129:59

is you'd have the classical theory is

130:01

essentially the zero third order term

130:04

and you can think of it as a

130:06

perturbation in H bar because H bar is

130:08

small that's a kind of way to colloquial

130:10

think colloquially think of it and so

130:13

you could have a one loop diagram that

130:15

would be a first order correction a

130:16

two-loop diagram second order so on and

130:18

so forth however I mean in quantum

130:20

mechanics before getting into quantum

130:23

field theory you could I'm pretty sure

130:25

that you you could do time independent

130:27

perturbation theory. I mean, for what

130:28

you're working with, you have a lot of

130:30

DC

130:32

is DC. So, there's no time dependence,

130:35

right? And so, you could look at the

130:37

frequency and you could say, well, it's

130:40

a really long wavelength

130:42

uh excitation. So I'm actually, you

130:45

know, I'll have to think more about what

130:47

exactly you are doing cuz I had just

130:49

assumed that you were doing the typical

130:51

perturbation theory of quantum field

130:53

theory, but now you're saying you're

130:54

mentioning time independent perturbation

130:56

theory. So

130:57

>> yeah,

130:57

>> I've I've seen some of your your notes.

130:59

Obviously, you haven't published

131:00

something yet, so I haven't,

131:02

>> you know, I I I looked through what you

131:03

were able to send me, but I I'm just

131:05

realizing now that you mentioned time

131:07

independent perturbation theory, which

131:09

wasn't what I was thinking. So maybe

131:11

that it's worth disentangling. Not

131:13

saying you have necessarily have an

131:14

error there, but um I'm just realizing

131:17

that now.

131:18

>> No, I mean I you know this is I haven't

131:21

done QED in 26 years.

131:23

>> Yeah. Yeah.

131:23

>> So could you use a refresher?

131:25

>> Yeah.

131:26

>> But um I I was just intrigued by just

131:29

doing the time independent perturbation

131:31

theory and getting something. I' love

131:33

your help translating some of that. U

131:35

the vertices that don't end. I

131:38

understand these particles don't they're

131:40

not real, right? I can't capture them,

131:42

but I pictured them more like electric

131:44

fields where you you can't pull the

131:47

field from the charge, right?

131:49

>> Have you now field line?

131:52

>> It doesn't work that way. And that's

131:53

what these things I think represent. So

131:55

that's why we have things like

131:56

reormalization, these really complicated

131:57

tools to try to address these

131:59

infinities. A lot of infinities here.

132:01

>> And that that is a nasty integral that I

132:04

have not been able to solve.

132:06

>> Yeah. Yeah. I'm I'm only looking at the

132:08

the cartoon picture trying to interpret

132:10

it. But if you want to help me with

132:12

that, that'd be awesome.

132:14

You help with the real math that some I

132:17

have five or six kids start to work on

132:19

that gamma functions, error functions.

132:21

These are not fun things.

132:22

>> Yeah, the integrals are definitely hard.

132:24

>> They are not hard. It's not a beautiful

132:25

solution like Kulum's like it's

132:28

different. Does the fact that Charles is

132:30

talking about a timeindependent

132:32

perturbation which you kind of hadn't

132:34

anticipated before the conversation does

132:36

that change anything as far as the

132:38

viability in your mind with QED or is it

132:40

is that something you have to kind of

132:42

>> well think about offline?

132:43

>> You can do you could you could do

132:45

perturbations with frequency

132:48

at the classical level. So if you're

132:51

claiming it's a quantum effect at some

132:53

point I think I believe I mean with the

132:56

five diagrams that you would have would

132:58

there be any loops in the diagrams that

133:02

you've been studying?

133:03

>> Well the zero orders are there right the

133:05

the non where they start and the end.

133:07

Yeah the self energy you're talking

133:10

about. Yeah.

133:12

>> Yeah. There

133:12

>> self energy terms. There's 12 terms and

133:14

I think half of them are not very useful

133:17

but maybe the other half are. That's the

133:20

That's what I'm proposing. Maybe they're

133:21

interesting because they don't they

133:23

don't close in like you would want them

133:25

to. You can't make the picture nice and

133:27

neat in your head. It's always it's this

133:30

is a game and I love this game because

133:32

it's like try to try to use your mind

133:34

and our brains are not good at this. If

133:37

I take two charges, we know they can

133:40

attract and we know they can repel.

133:43

But if you didn't see this one and you

133:45

see this one go there or go there, your

133:47

brain would say, "Well, I can't do that.

133:49

Or if I take two charges and I stick

133:51

them on a box, don't let them touch.

133:56

Take the electrodes away. Are they still

133:58

attracting? Damn right they are. For how

134:01

long? Forever. So that is a fundamental

134:05

property of charge fields which QD I

134:10

think explains quite well. So but is it

134:12

conserving energy? You know that's what

134:14

you have to think about. Is it

134:15

conserving energy? still there. You've

134:18

removed all your energy to get that

134:20

there.

134:21

>> Why is it still there?

134:22

>> So, there's there's a little mind games

134:24

with this. I think kind of helps. I

134:26

think this exodus is kind of a here's

134:28

another mind game for you.

134:30

>> I mean, it it is hard to imagine what is

134:33

going on there. I I have to

134:36

>> experimentally I I I don't know what's

134:38

going on. I it but it's it's curious

134:40

because we have nother's theorem which

134:42

describes energy momentum conservation

134:44

from uh space-time translation symmetry

134:47

and nother was actually studying quantum

134:50

field theory and discovered something

134:52

profound about classical mechanics about

134:54

the conservation laws but even still

134:58

things are conserved offshell so

135:01

it's hard to right as you're saying I

135:03

mean maybe there's some charges that

135:04

we're overlooking right but there there

135:07

honestly It's at the point where if it

135:11

appeared as if momentum conservation was

135:13

violated, then you would claim that

135:16

there's something else there that we

135:18

don't understand, right? There must be

135:19

something carrying that momentum.

135:21

>> Yeah.

135:22

>> I mean, that's how the nutrino was

135:24

discovered. Initially, they they had

135:26

these decay channels and they're

135:29

counting the energy. They're accounting

135:30

for the energy. It's like, wait a

135:32

second. This the bookkeeping isn't

135:33

adding up.

135:34

>> Yeah. And then isn't that how science

135:37

kind of moves forward in some ways? I

135:39

guess if you were to take your physics

135:41

hat off and just as a human being look

135:45

at all the kind of overwhelming

135:46

anecdotal evidence because I know you've

135:48

you've kind of systematically surveyed a

135:50

lot of these like weird fringe

135:52

experiments and exotic propulsion, free

135:54

energy, all sorts of things like that.

135:56

And to me, you know, with the without

135:59

the any sort of physics background, I

136:02

think you almost have to be dogmatic to

136:04

say that there isn't some sort of there

136:06

there specifically around the lineage of

136:09

the type of stuff that that Charles is

136:12

discussing. I don't know what what you

136:14

would say there. Um yeah, what what do

136:17

you think? Because clearly that is a way

136:18

often that science moves forward. You

136:20

know, if you look at, you know, Thomas

136:21

in the, you know, uh, uh, structure

136:24

of scientific revolutions, it's this

136:25

like anomaly buildup and then that sort

136:27

of breaks the dam and then the theory

136:29

often is playing catch-up on the

136:31

anomaly. Yeah, definitely. It can go

136:33

both ways as well. But I mean, certainly

136:35

out of all of these weird phenomena that

136:37

seem to not fit into conventional

136:40

theory, I mean, I would say your

136:42

experimental results are, you know, got

136:45

to be in the top 10 in terms of most

136:47

convincing things I've seen. I mean

136:49

there's other groups where they do one

136:51

experiment and they're measuring picon

136:53

newton forces right we've all heard

136:55

these stories and then people get in

136:57

debates oh is it some experimental error

137:00

>> obviously as you point out you're not

137:02

100% sure there could be some prosaic

137:04

explanation but the fact that you've

137:06

done so many different things and you're

137:08

seeing the self-consistency I mean even

137:11

as a scientist I have to say that is

137:13

encouraging and we should explore this

137:15

further it's not something we should

137:17

just sweep under the rug and forget

137:18

about what would be your best way. You

137:22

know, obviously you haven't like

137:24

rigorously

137:26

uh kind of studied the experiment

137:28

itself. You haven't been like on site

137:29

with them, but would you have any way of

137:32

explaining it away? Like if he is

137:35

controlling for and eliminating this ion

137:38

wind effect and actually showing that in

137:39

a vacuum chamber you get more thrust,

137:42

you know, that to me that feels like

137:44

pretty pretty convincing. And then

137:45

obviously this is being done in a

137:46

Faraday cage, you know, so there's no

137:48

electric field interference.

137:51

Is there any way that you could kind of

137:53

poke at it or kind of straw man it from

137:56

afar? Honestly, no. And I I've

137:59

interacted with Drew multiple times on

138:01

APE with Tim Ventura. I've had private

138:04

communications with him. I've interacted

138:07

with him publicly. I've seen these I've

138:09

seen him his iteration rate first of all

138:11

is phenomenal, right? He's just always

138:13

testing new things, trying different

138:15

stacks with different materials and

138:17

different geometries, and he's really

138:20

dialing it in. It's it's really

138:21

impressive the the innovation rate that

138:24

he's he's going at and your whole team.

138:27

And so, I mean, if if you've checked all

138:30

these things that you say you've

138:31

checked, right? I you know, I obviously

138:33

I haven't been in the lab with you, but

138:36

it is I can't think of anything to be

138:38

honest. I I I can't think of any prosaic

138:40

explanation. And I mean, if you know

138:42

there, you're right. There's not much

138:44

magnetic stuff going on. There's a lot

138:46

of electrostatics, right? Not much

138:48

charge moving. I It's just so

138:50

mind-blowing, though. I mean, the idea

138:52

that the claim is you you power it up

138:54

and then you unplug it from the wall and

138:56

then the thrust continues in

139:00

indefinitely. Well, you know, obviously

139:01

you haven't tested it for an infinite

139:03

amount of time.

139:04

>> Drew would sometimes act as if it would

139:06

last forever. I mean, my skeptical brain

139:09

is saying, well, eventually

139:11

>> wouldn't that capacitor discharge? But

139:14

still, even if it lasts

139:16

>> a day, you know, it seems like it lasts

139:18

longer than a day from what you guys

139:20

have done as far as I can tell in terms

139:22

of the claims, it's it's it's hard to

139:24

imagine how how could that be continued?

139:27

Like the fact that it's not getting

139:28

drained. You would think, okay, well,

139:31

wouldn't it require energy to get that

139:33

thrust? Wouldn't that quickly drain the

139:36

capacitor? It doesn't seem to be what

139:38

you're claiming.

139:39

>> You've tested it in so many different

139:41

ways that it's

139:43

>> it it's it's a tough challenge for

139:45

anyone to try to describe what's going

139:46

on there. It's very mysterious.

139:48

>> You're also friends with and um looked

139:52

at the experiments done by Falcon space

139:54

in this sort of area in this sort of

139:56

electrogravidic or maybe you know new

140:00

electrostatic force area. Uh they

140:03

basically tried to pull off the Biffield

140:04

Brown effect. uh what was your take on

140:07

that experiment?

140:08

>> Yeah, so it was actually interesting. It

140:11

was curious. So it was not

140:14

scientifically conclusive. We not all

140:16

the experimental errors ruled out, but

140:18

there was something interesting that was

140:20

seen where

140:22

they did the tests at not too low

140:24

pressure and they noticed it spinning in

140:26

one direction and then eventually they

140:30

kept pumping down further and further

140:32

and eventually it started spinning in

140:33

the other direction which

140:35

It's, you know, qualitative. We don't

140:37

know how strong the force is. I don't

140:39

know what the friction was. They I mean,

140:41

they had a a nice mechanism to hold it

140:44

up so it minimized the friction using

140:47

magnets, which introduces additional

140:49

potential errors. But I'm not too

140:51

worried about the magnets. But if you're

140:53

going to do a demonstration for others

140:55

that are skeptical, you should probably

140:57

maybe think do it another way. So, it

140:59

was I think it was interesting and it

141:02

was worth further study. It's suggestive

141:05

but not conclusive I would say where

141:08

more work is needed

141:09

>> because of the the magnets or what what

141:12

>> honestly so there there was this other

141:14

thing where the way the high voltage was

141:16

delivered uh to the thrusters uh on one

141:20

end it used the spiraling around the

141:22

chamber I mean that's something you

141:23

could point at and say ah let's just say

141:25

it's that honestly I doubt it would be

141:28

causing what was seen but you know it's

141:30

something to consider really to get a

141:33

confirmed term thing, it's best to do

141:35

multiple tests, right? Not just one and

141:37

do it in different ways. But really,

141:40

another issue potentially was the fact

141:43

that there were these discharges that

141:45

were observed.

141:46

>> And Tim Ventura was actually one of the

141:48

first to kind of get a little skeptical

141:51

to some degree because

141:52

>> he had worked with those ion lifters

141:55

back in the day with the triangular ones

141:58

and the tinfoil. And so he had worked

141:59

with high voltage and he was aware

142:01

because it it took me time to realize

142:03

this. You would think naively, well,

142:05

okay, there's this all this ion wind

142:07

stuff and that's because you're ionizing

142:10

the air. So you just remove the air and

142:12

do it in vacuum and I'm good, right? No

142:14

ion wind to worry about. But what if

142:16

there's ions or electrons literally

142:18

flying off the thruster itself? Or what

142:21

if the wires connecting them, we we

142:24

could see different discharges that were

142:26

occurring. So what if you're you're

142:29

you're spraying out these ions. What if

142:32

that's causing the force?

142:35

>> So it's it's something that it's it's

142:38

also amazing to look into it. It's first

142:40

of all, it's a challenge enough just to

142:41

work with high vacuum systems. Then it's

142:44

another challenge. I mean, if you're

142:45

you're well aware of this stuff to work

142:47

with high voltage.

142:48

>> Sure.

142:48

>> But then to combine the two, it's it's

142:51

remarkable

142:52

>> because you Yeah, you definitely want to

142:53

enclose everything with the can. When I

142:56

saw Mark's video, I I was worried about

142:58

the coil

142:59

because that would be, you know,

143:00

dubious. Why do you have a ground there,

143:02

but it's not a ground? I guess it's a

143:05

high voltage wire. But, um, it's

143:07

interesting that it went one way like

143:08

you would expect if it was a corona wind

143:10

and you pump it down, goes the other

143:12

way. That would be that's cool to see.

143:14

>> Yeah. So,

143:15

>> but you don't, like you say, you don't

143:16

want the discharges. You don't want the

143:18

current coming off even under high

143:20

vacuum. You'll get field emission it's

143:21

called.

143:22

>> Yeah.

143:23

>> From material. So you want to kind of

143:24

make sure you encapsulate everything. So

143:27

that would be the only thing that might

143:28

be a hiccup is the is the possibility of

143:30

field emission, but I have not seen the

143:31

experiment. So but that's easy to

143:33

prevent. You can coronadop it. You can

143:35

>> do all kinds of things to kind of

143:36

prevent that encapsulate it.

143:39

>> But yeah.

143:40

>> Yeah. So I found it encouraging, but you

143:43

got to keep studying further. I I think

143:45

you know to really get to the bottom of

143:47

it. Well, on that note, I know we went

143:49

deep into all sorts of, you know, out

143:52

there out there theories. Um, but this

143:54

was super super helpful. And if if you

143:57

were to give Charles any advice as far

143:59

as kind of fleshing out his theory or,

144:01

you know, um, places to look, what what

144:03

would it be?

144:04

>> Well, I would say, yeah, so if you if

144:06

you're doing you could consider two

144:08

different types of perturbation theory

144:10

at the same time. So you can do the time

144:12

independent one and you can do the har

144:16

the quantum corrections as well. So you

144:19

could keep track of both of those. It's

144:20

a little more complicated. You might not

144:23

even need the timeindependent

144:25

assumption. But since you're working

144:26

with electrostatics, I also see why

144:29

you're doing that. So it could make

144:31

sense to do that approximation because

144:33

it would simplify things. But then you

144:35

just got to be Yeah, I mean if it's

144:37

truly DC, yeah, it probably would be a

144:39

good approximation to do. Um yeah so I

144:42

think that would be one thing to do just

144:44

um yeah look into reormalization the

144:48

self energy uh those per perturbative

144:52

corrections can affect the electron self

144:54

energy also this is a puzzling thing if

144:57

you look at the direct spinner which is

145:00

used for electron in quantum

145:01

electronamics the spinner field those

145:05

equations of mo you can still have

145:07

classical equations of motion for a

145:09

quantum field and those equations might

145:12

have E or H bar or C. So you can get

145:14

alpha in thing in classical equations

145:17

but it's subtle because it's a quantum

145:19

field theory but you know there's a

145:21

classical limit there. So yeah I would

145:23

say I I honestly just try to learn as

145:25

much as you can keep trying to

145:27

>> you know we can we can correspond via

145:29

email and try to talk more about quantum

145:31

electronamics and

145:33

>> we'll see. I you know maybe something

145:35

more is needed but I think it's a good

145:37

effort to at least see where does

145:39

quantum electronamics

145:41

take you but also just recognize it is a

145:45

possibility that the results you're

145:47

finding can't be described by quantum

145:48

electronamics just keep that in mind

145:50

>> yeah you know the reason why we like to

145:52

use the QED we haven't mentioned it much

145:54

but um because of the alpha that shows

145:56

up experimentally

145:57

>> you know that's that's really cool some

146:00

the fine structure you know showing up

146:02

>> terms of the forces and find structure

146:04

constant squared. So it's always some

146:06

kind of function of alpha keeps showing

146:08

up experimentally. There's not too many

146:09

experiments you could do in your garage

146:11

>> to get you an alpha

146:13

>> and that points towards quantum

146:14

electronamics.

146:16

>> Quantum

146:16

>> quantum in general say no one knows

146:18

where alpha comes from. I don't think

146:20

anyone has a clue but it's there.

146:22

>> Why does the fact that a fine structure

146:24

constant is showing up point towards uh

146:27

quantum mechanical effect?

146:30

>> That's a good question. So

146:31

>> it's the coupling between fields and

146:33

charge is what alpha. So it's not too

146:35

surprising.

146:36

>> So it's like a it's like a primitive in

146:38

quantum mechanics and that keeps showing

146:40

up

146:40

>> in physics in general and it shows up

146:42

all over the place.

146:42

>> Yeah. Yeah. Yeah.

146:43

>> There's also another way to look at it

146:44

where you can kind of look at it from a

146:47

natural units perspective and just kind

146:48

of set H bar and c to one. I know a lot

146:51

of people might not like that.

146:53

>> Sorry,

146:53

>> I don't like that.

146:54

>> Yeah, I can understand why. I I get what

146:56

you're saying but I mean at the end of

146:58

the day alpha is proportional to was it

147:01

E^ squ and

147:03

>> the the interaction term between the

147:05

electron and the photon introduces a

147:07

factor of alpha. So once you you have

147:10

that fon vertex where you have an

147:13

electron positron and a photon there's

147:15

like a factor of alpha there.

147:16

>> Yeah.

147:17

>> And so if you're going to build these

147:18

loop order corrections you're going to

147:21

need more vertices. So you will require

147:25

more factors of alpha as you go out in

147:27

the you know the quantum perturbation

147:29

theory. However just remember that even

147:32

for the kulum force where it's a tree

147:34

diagram no loops there's still you could

147:38

do a unitarity cut on that photon

147:40

internal line and there's still two uh

147:44

interaction vertices alpha and alpha

147:46

that get multiplied together even for a

147:48

classical process. So certainly tracking

147:52

uh powers of alpha is helpful in

147:54

perturbation theory but just keep in

147:56

mind that it comes in at the classical

147:59

level as well.

148:00

>> It's exciting. Yeah because I've been

148:01

doing the driving the orders of

148:04

magnitude between third order I think.

148:06

Yeah I didn't go to fourth order but

148:08

yeah actually fourth order third order

148:10

second order first order and you could

148:12

see the perturbations in alpha.

148:14

>> Alpha is nice to use because it's you

148:15

know dimensionless. It's the ratio of um

148:19

the energy of two charges divided by a

148:21

photon of that same wave wavelength of

148:24

where those two how far apart those two

148:26

charges are. So that's what alpha is.

148:28

It's a ratio of two energies. That's the

148:30

best way to to describe the summerfeld

148:32

constant. So oh there was something else

148:35

I want to mention you too. You had

148:37

mentioned the term hidden momentum. So I

148:40

believe there is work certainly by the

148:42

1980s where if because in classical

148:46

electronamics the pointing vector is

148:48

what carries the momentum density and

148:50

that is proportional to E cross B. And

148:53

so there were experiments where people

148:57

part of the reason why hidden momentum

148:58

is found was in statics as well where

149:02

they had an electric field that was

149:04

static and a magnetic field that was

149:06

static and they're perpendicular. So you

149:08

get this E crossb and it was puzzling

149:12

because you would have a pointing vector

149:14

implying there's momentum but I mean I'm

149:17

pretty sure if you just take a symmetric

149:20

capacitor with an electric field going

149:22

through and then you put it inside a

149:23

solenoid with a magnetic field

149:25

perpendicular

149:27

nothing's going to thrust right and the

149:29

hidden momentum is what describes what

149:32

cancels out so that you don't get thrust

149:34

in those experiments. So that's just

149:36

another thing to look into.

149:38

>> That's where I started, right? So I

149:39

started looking at uh field momentum

149:42

being converted into linear angular or

149:45

linear momentum. Uh and the crux was

149:47

this 1970s hidden momentum which is a

149:50

relativistic effect. So even if you have

149:52

a magnetic field, a current, you can

149:53

always draw that as like a kind of a

149:55

square. And whenever there's the Faraday

149:58

field, it will accelerate charges in one

150:00

loop and decelerate them in the other

150:02

loop. So it's basically a kind of a

150:04

change of momentum physically of the

150:06

loop of the electrons hitting the walls.

150:07

That's how they describe the hidden

150:09

hidden momentum. So every time you have

150:11

a static E-crossB moved like you can't

150:13

you have a highly charged electric you

150:15

know electric charge to a bar magnet

150:17

doesn't fly across the room because of

150:18

the hidden momentum. So that can be

150:20

scaled down microscopically. So even the

150:22

magnetic moments can be pictured as

150:24

little currents and they have hidden

150:27

momentum. They're relativistic. So I

150:30

first started out for last I started

150:32

about in the 2000s to look at maybe the

150:36

conversion from field momentum to

150:37

mechanical momentum could happen like it

150:40

does in the angular case but for linear

150:43

momentum if there's no hidden momentum.

150:45

So what's the opposite of relativistic

150:47

charges moving? Electrostatics

150:50

>> keep the charges static. Do static

150:53

charges possess hidden momentum?

150:55

>> And that's my my theory was it didn't.

150:58

So that led me down that to that path

151:00

where in 2010 I saw the forces initially

151:03

could have been something else but

151:05

that's where I started and it wasn't

151:07

until after two years working with Drew

151:09

I said oh Drew's got the he's got the

151:11

conversion down from field momentum um

151:15

to mechanical momentum without static

151:17

charges. My wife pointed that out and uh

151:20

so we did the test. So for two years we

151:21

thought that's what the case. It wasn't

151:23

until 2018 where I realized that I

151:25

didn't even need the current. So I'm not

151:28

even setting up the E crossb fields

151:30

anymore. So this there's two electric

151:32

fields and one magnetic field for that

151:34

all to work. You have the E crossb and

151:36

then you you kill the B to make a second

151:38

E field called the Faraday's law field

151:41

to convert it into um mechanical

151:43

momentum. But if you don't have hidden

151:46

momentum, you should see thrust. So

151:48

that's what we thought we were seeing

151:50

until I realized

151:53

just before going on a trip that I

151:56

didn't even need a B field or a current.

151:58

So oh man, I'm in pure electrostatics

152:01

mode.

152:02

>> Whoa.

152:03

>> So I don't have any field momentum which

152:06

was good and bad. Um it led us down this

152:09

path. So okay, so now we'll have to

152:12

study that first before going back to

152:14

that which is far more complicated.

152:16

>> Super fascinating. Well, this has been a

152:18

really fun discussion. David, thank you

152:20

so much for lending your expertise here

152:22

and for uh you know, talking to Charles

152:25

uh in in a way that's clearly like not

152:27

dogmatic about the experimental results

152:30

uh uh and then kind of helping sharpen

152:32

his his blade on the quantum

152:34

electronamics. So, really appreciate you

152:36

both.

152:37

>> Thank you.

152:37

>> Thanks for having us and it's pleasure

152:39

meeting you. It

152:40

>> was pleasure meeting you too. Thank you.

152:54

Heat.

153:06

Heat.

153:14

Heat.

153:21

Hey, heat. Hey, heat.

Interactive Summary

In this video, Jesse Michels interviews Dr. Charles Buhler, NASA's lead electrostatic scientist and co-founder of Exodus Propulsion Technologies, regarding his discovery of a propellantless propulsion force. Buhler explains how his team has conducted over 2,000 experiments validating a force that appears to bypass traditional Newtonian rocket constraints, building upon the historical work of Thomas Townsend Brown's 'electrogravitics.' The discussion covers the experimental controls used to rule out ion wind and electrical interference, the inefficiencies of current chemical rockets for interstellar travel, and a deep dive into a theoretical explanation involving Quantum Electrodynamics (QED) with physicist David Chester. Buhler also shares personal UFO experiences that motivated his lifelong search for a more efficient way to move objects through space.

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