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Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF field Takaaki Musha INTERNATIONAL ACADEMY OF ASTRONAUTICS Missions to the outer solar system and beyond FIFTH IAA SYMPOSIUM ON REALISTIC NEAR-TERM ADVANCED SCIENTIFIC SPACE MISSIONS Aosta, Italy, July 2-4, 2007
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Page 1: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF field

Takaaki Musha

INTERNATIONAL ACADEMY OF ASTRONAUTICS

Missions to the outer solar system and beyond

FIFTH IAA SYMPOSIUM ON REALISTIC NEAR-TERM

ADVANCED SCIENTIFIC SPACE MISSIONSAosta, Italy, July 2-4, 2007

Page 2: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Contents

(1) Purpose(2) Outline of the dynamical B-B effect(3) Possibility of artificial gravity induced by

dynamical electromagnetic field(4) Electrogravitic propulsion systems(5) Conclusion

Page 3: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Purpose

• To explain the weigh reduction at the experiment by applying alternate electric field to the capacitor conducted by the research group of the HONDA R&D Institute group from the standpoint of ZPF field in a space

• To investigate the applicability of the dynamical Biefeld-Brown effect for the propulsion system

Page 4: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Outline of the dynamical B-B effect

• From the 1st of Feb. till the 1st of March in 1996, the research group of the HONDA R&D Institute conducted experiments to verify the B-B effect with an improved experimental device in 1996 to reject the influence of corona discharges and electric wind around the capacitor by setting the capacitor in the insulator oil contained within a metallic vessel. They found that the weight loss by the alternate electric field was greater than the static case .

Page 5: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Experimental set-up

t=1mm,d=170mm,W=62g

Page 6: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Electrical circuit for generating HV electric field

Page 7: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Schematic diagram of the electric circuit

8kV AC pulse, f=50Hz,

Page 8: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Histogram of weight losses observed at the experiment

gM 63.09.0 ±=∆

Page 9: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Forces generated by the ionic transfer of the momentum

)/(/2 000 giqVmM ⋅=∆

By introducing experimental values, 1682pF, 8kV, and 50Hz, into the equation, the weight reduction due to ionic winds becomes 1.3×10-3g , which is negligible small compared with the experimental result.

T.B.Bahder & C.Fazi

Page 10: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

EZEGZE rrg ⋅×−=⋅−≈ − εεπε 110 1062.84

)(002.0/1062.8 011 ggEWZM r =×=∆ − ε

22 ψµεψε SGdMGFg ==

(Musha: weak field approximation of general relativity theory)

(Ivanov: Weyl-Majumdar-Papapetrou solutions of the general Relativity theory)

Gravitational field generated by the B-B effect

gM 63.09.0 ±=∆(Experiment)

Page 11: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Possibility of artificial gravityinduced by

dynamical electromagnetic field

Page 12: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

2

2

2 cm c

πωhΓ

=

ZPF field in a space

ωπωωωρ d

cd 32

3

2)( h

=

Inertial mass is originated to theinteraction of sub-elementaryparticles with the vacuum ZPFfield

Inertial mass generated by the ZPF field

Page 13: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

(M.B.King : Tapping the zero-point energy)A slight coherence of vacuum fluctuations due

to the high potential electric field caused an alternation of inertial properties of the body with the ionic lattice of a rapidly spinning atom .

(B.Haish, A.Rueda and H.E.Puthoff)If one could somehow modify the vacuum

medium then the mass of a particle or object in it would change according to the zero-point field theory.

Page 14: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

><= 22

0

2

2A

cmeH A

23

0

2

2 cA cmeH ωπh

=′

(A) Electrodynamic Hamiltonian by P.Milonni

(B) Electromagnetic Hamiltonian corresponding Zero-point fields (B.Haisch, A.Rueda, H.E.Puthoff)

Process to derive the anti-gravity equation

Page 15: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

A=0

No Electric field Electric field Impressed

AA HH ′∆=

Initial State

0=AH

)( 0AAA HHH ′−′=′∆

Assumption to derive equation

0)( =′−∆ AA HH

Page 16: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

><−=∆ 2

02Ac

ωπωh

><ωπ

=ωω∆−=∆ 220

0/2/ Acmmh

Electrodynamic HamiltonianAA HH ′∆=

Equation of Mass Shift

2

2

2 cm c

πωhΓ

=

Page 17: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

rtNed

crcrtp

cA )(

41)/(

41

20

20

ωπεπε

=−

=&

)/(cos)( 220 crtE

mNetd

e

−−

= ωωω

A-field generated by the movement of electrons

Page 18: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

2042222

2

8220

422

4 )(4/)( E

cmGReNdvA

cGMM

e ωηωωω

επω

+−−=><=∆ ∫

ee

dηωπ

ωηωωωωω

ω 2)(2

142222

2

≈+−∫

20

2

8220

4

8/ ERN

cmGeMM

eηωεπ

−=∆

Mass reduction by the impressed electric field

mZe ee αω /2=

Page 19: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Compared result with the Honda experiment

22 3/2 mce=Γ=η

2

2131023.3/

tVRMM −×−=∆

mmRmmtkVV 1,1,8 ===1324 106,10 ×== eN ω

gM 28.1=∆

gM 63.09.0 ±=∆

(Abraham-Lorenz damping constant)

(dense hot plasma)

(Experiment)

Page 20: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Alternate external A-field

Mass shift of the dielectric material

Coupled with external forces

Net force generated

Mechanism of the Dynamical B-B effect

ZPF cutoff frequency shifted

A-fieldA-field

Capacitor

Dielectric material

Page 21: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

2

2131023.3/

tVRMM −×−=∆

αMdt

dMvdtMvdF +==

)(

2

2131023.3

tV

tRv

MM

tv

∆×=

∆∆

−= −α

Conservation of momentum

Acceleration of the moving body induced by          the electric field

Page 22: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Factors to induce a weight loss of the capacitor

• Increase the AC voltage impressed to the capacitor, nonlinear increase of the weight loss is produced.

• Increase the charge density of electric current flowing through the capacitor, the greater the weight loss

Page 23: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Electrogravitic propulsion systems

Page 24: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Electrogravitic craft by Brown

Dielectric material Core mass

Positive poleNegative pole

Electrode(Brown disc airfoil)

Page 25: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Spark generated at the Brown’s experiment

Page 26: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Brown’s experimental results

• A large thrust was associated with spark. A residual thrust existed without sparking (1956)

• A DC voltage caused a thrust when initially applied. The thrust would decay within 60 seconds. (1928)

• The thrust varies with the time of day(Both in vacuum and oil)

Page 27: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Electrogravitic craft (ARDA) by the JLN Labs

Electric field

Page 28: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

20

2

8220

4

8EvRN

cmGe

e τηωεπα

∆=

Electrogravitic propulsion system(Concept of the pulsed electric field plasma propulsion)

Thrust

[Features]•Highly acceleration capability•Low consumption of fuel

Inlet(-)

(-) (-)

(+)v(+) (+) (+)(+) (+)(+)(+) (+)(+) (+)(+) (+)(+)(+)(+)

(+)v(+) (+) (+)(+) (+)

(+)

(+) (+)(+) (+) (+) (+)(+)

(+)(+)(+)

(+)v

(+) (+)

Positively-chargedunits

HV pulse generator

Electric field

Electric field

Ion source

Plasma cloud

Electric field

To leading edge

Power supply

Charged outer hullNozzle

Grid

R: Radius of plasma cloud N: Plasma densityE0:Electric field

Page 29: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

Conclusion

• From the theoretical analysis by the zero-point field theory, it is considered that the origin of the dynamical Biefeld-Brown effect might be attributed to the interaction of zero-point vacuum fluctuations with high potential electric field impressed to the capacitor. This result suggests that the pulsed electric field applied to the capacitor may produce artificial gravity sufficient for practical application to the space propulsion technology.

Page 30: Explanation of dynamical Biefeld-Brown Effect from the ...jnaudin.free.fr/lifters/musha/Musha-Presen.pdf · Explanation of dynamical Biefeld-Brown Effect from the standpoint of ZPF

The End

INTERNATIONAL ACADEMY OF ASTRONAUTICS

Missions to the outer solar system and beyond

FIFTH IAA SYMPOSIUM ON REALISTIC NEAR-TERM

ADVANCED SCIENTIFIC SPACE MISSIONSAosta, Italy, July 2-4, 2007

If you have any question, please send me a mail [email protected]@gmail.com


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