Inventions of Henry William Wallace

Additional Sources

The following items give the technical details of NASA’s ongoing work to replicate Podkletnov’s experiment. Dr. Li, mentioned elsewhere in this paper, is one of the researchers.

http://ro.com/~preavis/Delta-G/Physica-C.htm Static Test for A Gravitational Force Coupled to Type II YBCO Superconductors, Ning Li*, David Noever, Tony Robertson, Ron Koczor, and Whitt Brantley NASA Marshall Space Flight Center, Huntsville, AL 35812 and *The University of Alabama in Huntsville, Huntsville, AL, 35804. Physica C Preprint.

http://ro.com/~preavis/Delta-G/Delta-G_investig.htm High Temperature Superconductor Research (Project 96-07), Investigators: R.J. Koczor/EA01, D.A. Noever/ES76, G.A. Robertson/EP32, Ning Li/UAH.

The following items by Modanese are the most detailed theoretical analyses of the Tampere Effect given to date. Modanese’s basic idea is that the rotating superconductor is a macroscopic quantum-coherent state (Bose-Einstein condensate) which affects gravity by means of modifying Einstein’s cosmological constant term in the gravity-field equations. This mechanism appears to be different from, but possibly closely related to, the gravitomagnetic field discussed above in this article. In any case, it is plausible to think, or at least to suggest, that the unpaired nuclear spins in Wallace’s special materials also comprise a macroscopic quantum-coherent state and thus could act as proposed by Modanese’s theory.

http://xxx.lanl.gov/abs/gr-qc/9612022. Possible quantum gravity effects in a charged Bose condensate under variable e.m. field, G. Modanese, J. Schnurer.

http://xxx.lanl.gov/abs/hep-th/9601160. Role of a “Local” Cosmological Constant in Euclidean Quantum Gravity, G. Modanese. Phys.Rev. D54 (1996) 5002-5009

http://xxx.lanl.gov/abs/hep-th/9508018. General properties of the decay amplitudes for massless particles Authors: G. Fiore, G. Modanese. Nucl.Phys. B477 (1996) 623-651.

http://xxx.lanl.gov/abs/hep-th/9505094. Theoretical analysis of a reported weak gravitational shielding effect, G. Modanese. Europhys.Lett. 35 (1996) 413-418.

http://xxx.lanl.gov/abs/hep-th/9410086. Vacuum correlations at geodesic distance in quantum gravity, G. Modanese (INFN, Trento, and Max-Planck-Institut, Muenchen), report U.T.F. 332, July 94. Riv. Nuovo Cim. 17 (1994).

APPENDIX– SI (MKS) Dimensisons of the Gravitomagnetic Field.

Gravitoelectric Charge = Kg
(in purely electrical units, Kg = (Weber/Meter)(Coul/Meter)(Sec)

Gravitoelectric Field = Meter/Sec-Squared

Gravitoelectric Flux Density = Kg/Meter-Squared

Mass Current = Kg/Sec = (Weber/Meter)(Coul/Meter)

Gravitomagnetic Dipole Moment = (Kg)(Meter-Squared)/Sec
= Angular Momentum
= (Coulomb)(Weber)

Gravitoelectric Dipole Moment = (Kg)(Meter)
(You would need the equivalent of negative mass to make one of these)

Gravitomagnetic Charge = (Velocity)(Meter) = Square-Meter/Sec

Gravitomagnetic Field = (Mass Current)/Meter = Kg/Sec-Meter
= ((Kg)(Meter^2)/Sec)/Meter^3
= Spin Density = Angular Momentum/Cubic-Meter
= (Coulomb)(Weber)/Cubic-Meter

Gravitomagnetic Flux Density = (Gravitomagnetic Charge)/Meter^2
= Velocity/Meter
= 1/Sec = Angular Velocity

Gravitoelectric Scalar Potential = Joule/Kg
= (Acceleration)(Meter)
= (Gravitoelectric Field)(Meter)
= Velocity-Squared
= Meter-Squared/Second-Squared

Gravitomagnetic Vector Potential = (Gravitomagnetic Charge)/Meter
= Velocity = Meter/Sec

Gravitoelectric Permitivity = Gravitoelectric Flux per Gravitoelectric Field
= (Kg)(Second-Squared)/(Cubic Meter)
= 1/4(Pi)(G) = 1.1927E09 Kg-Sec^2/Meter^3

Gravitomagnetic Permeability = Gravitomagnetic Flux per Gravitomagnetic Field
= Meter/Kg

Assuming Transverse Gravitational Waves Propagate at Light Speed —
= 1/(c-squared)(epsilon0)
= 9.316E-27 Meter/Kg