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Appendix: earlier setup. Our first experimental setup consisted of (a) a hexagon-shaped YBCO 1” (2.5 cm) superconducting disk, 6 mm thick; (b) a magnetic field generator producing a 600 gauss/60 Hz e.m. field; (c) a beam balance with suspended sample. The beam is made of bamboo, without any metal part, coming to a point on one end (24.6 cm long, weight 1.865 g). The sample is made as follows. A cardboard rectangle (16 mm by 10 mm by 0.13 mm) is suspended from the balance with 2.8 cm of cotton string. A polystyrene “pan” (7.2 cm by 8.7 cm by 1.7 mm) is attached with paper masking tape to the cardboard rectangle. The total sample assembly (with string, cardboard, tape) weighs 1.650 g. The balance is suspended from the end of a 150 cm wood crossbeam by ca. 30 cm of monofilament fishing line attached to the balance’s center of mass (5.5 cm from the end where the sample is attached). The other end of the crossbeam is firmly anchored by a heavy steel tripod. Thermal and e.m. isolation is provided by a glass plate (15 cm by 30 cm, 0.7 cm thick) with a brass screen attachment. This plate-and-brass-screen assembly is held about 4.5 cm below the sample by a “3-finger” ring stand clamp. A straightsided, 14 cm diameter, 25 cm deep dewar with ca. 10 cm of liquid nitrogen is used to cool the superconducting disk below its critical temperature, and is removed from the experiment area before the trial. The experimental procedure comprises the following steps. 1. The YBCO superconductor is placed in a liquid nitrogen bath and allowed to come to liquid nitrogen temperature (as indicated when the boiling of the liquid nitrogen ceases). The superconductor will remain below its critical temperature (about 90 K) for the duration of the trial (less than 20 seconds). 2. The disk is then removed from the bath and placed on a strong NdFeB magnet to induce a supercurrent. The Meissner effect is counteracted by a wooden stick. The superconducting disk has a cotton string attached to it to assist handling. 3. The disk and wooden stick assembly is placed on the AC field generator, about 33 cm below the isolation plate and about 40 cm below the sample. The AC field generator is then cycled for ca. 5 seconds with 0.75 sec equal-time on/off pulses. Prior to a run the sample is centered to be over the middle of where the disk will finally be, on the AC field generator. 20
One observes that while AC current is flowing through the generator the balance pointer dips 2.1 mm downward. When the AC field generator is pulsed with no superconductor present, there is no measurable pointer deflection. Also air flows do not cause any measurable deflection. The whole procedure is well reproducible. The weight difference required to raise the sample by 2.1 mm was then found to be 0.089 g. This was measured taking advantage of the fact that the suspension wire produces a small torque on the balance beam toward the equilibrium position: the balance pointer was found to raise 2.1 mm upward when a weight of 0.089 g was placed above the sample. 21
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was highly questioned Copyright© 1
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EXPLORATION OF ANOMALOUS GRAVITY EF
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As aerospace engineers we deal more
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( DxB) ∂ fH = , (2) ∂t where D
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d φ = KG (8) c dM The sensitivity
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non-EM modulated tests on the masse
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BREAKTHROUGH PROPULSION PHYSICS RES
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PROGRAM PRIORITIES To simultaneousl
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STATUS AND DIRECTION A government s
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REPORT DOCUMENTATION PAGE Public re
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Recent calculations have indicated
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Casimir force has only been compute
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Cavity width 125 nm Cavity wall 245
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Also shown for comparison, is the c
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AIAA-2001-3906 SEARCH FOR EFFECTS O
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AIAA-2001-3906 Experiment 2 - Time-
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AIAA-2001-3906 Resonance - 0 flow R
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AIAA-2001-3906 Einstein Rocket -- E
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Tests of Mach's Principle with a Me
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we note that Woodward [4] has made
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and their tensioning mechanism. Ele
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Conclusion The test of Mach’s pri
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velocity of the “front” that mu
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Fortunately, recent advances in non
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The time difference between two wel
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impinging at normal incident on a m
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sooner than his challenger. Interes
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non-empty space¯time with a horizo
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metric of S-1 takes the form ds 2 =
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L. Hui Astrophys. J. 519 (1999), p.
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consistent with the boundary condit
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classical behaviour is recovered fo
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Heisenberg's equations for the posi
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(2K) Fig. 1. Behaviour of Q(t) for
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5. N.A. Lemos J. Math. Phys. 37 (19
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arXiv:cond-mat/9701074 v3 16 Sep 19
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technology involved in the construc
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3 Operation of the apparatus. Two i
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following: in a field gradient of 0
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inner edge of the toroid (5-7 mm fr
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7 Discussion. The interaction of a
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8.1 Acknowledgments. The author is
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High T c materials, fabrication |ge
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Supporting solenoids |general, fig.
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Rotating solenoids |general, fig. 3
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Cryogenic system |general, fig. 51/
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Disk braking system |general, fig.
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In two recent experiments [1, 2], P
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true, must then consist of some kin
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constant turns Eintein gravity into
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[2] E. Podkletnov and A.D. Levit, G
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Proposal for the Experimental Detec
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Non-detection of the effect would a
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system of units to another rather t
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is not SC, and is composed of norma
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the rest of the SC). This would sho
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cylinder has its long axis oriented
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(24) s = Iω where ω is the spin a
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established. For ease of experiment
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lowered into the chamber, alternati
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T < Tc n n T > Tc n 0 Table 1: Inte
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a gravitational BCS type theory is
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III Gravitational London Equations
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VI Conclusion More significant than
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UTF-367/96 Jan 1996 arXiv:supr-con/
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2 Introduction The discovery of sup
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4 depressed by a magnetic field [12
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6 symmetry for the cuprates. Surpri
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8 metallic ρ(Τ) α T n with n > 1
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10 pseudogap, two dimensional (2D)
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12 the hole-doped and electron-dope
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14 An example of recent progress in
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16 crystals of these materials [104
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18 Acknowledgments Assistance in pr
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20 [22] M. T. Béal-Monod and K. Ma
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22 [59] A. V. Puchkov, P. Fournier,
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24 [94] A. G. Sun, A. Truscott, A.
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26 Table caption Table 1. (a) Some
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28 Fig. 8. Schematic phase diagram
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30 Table 1. (a) Some important clas
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Gravitation shielding properties of
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unaffected by an inch-thick steel p
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Polarizable-Vacuum (PV) representat
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A. Velocity of Light in a Vacuum of
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From the reciprocal of Eq. (10) we
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III. CLASSICAL EXPERIMENTAL TESTS O
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⎡ v L ≈ c ⎢ 1 − 2GM 1 ⎣
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IV. COUPLED MATTER-FIELD EQUATIONS
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Emerging Possibilities for Space Pr
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RS Electrogravitic References RS El
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Electrogravitics Systems: An examin
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ELECTROGRAVITICS SYSTEMS REPORTS ON
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CONTENTS Foreword 4 Elizabeth Rausc
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Accelerator Center, Stanford, CA wi
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Introduction, as well as copies of
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ELECTROGRAVITICS SYSTEMS An examina
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DISCUSSION Electrogravitics might b
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particles - that is to say those th
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interrelationship is a difficulty a
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electrogravitics. This is one line
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In 1955 the number of technicians e
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existence and collisions that give
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and counterbary. Counterbary is the
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ANTI-GRAVITATION RESEARCH The basic
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towards realization of a manned veh
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ELECTRO-GRAVITIC PROPULSION SITUATI
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investment is likely to be necessar
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to its present pitch. Beyond the th
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ELECTRO-GRAVITICS EFFORT WIDENING C
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ELECTROSTATIC MOTORS 40
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THE GRAVITICS SITUATION December 19
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that no new breakthroughs are neede
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equipotentials can be made less con
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laboratory man-hours is necessary o
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But aviation business is understand
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HI i GLOSSARY Gravithermals: Thermi
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Magnetogravitics : Boson Fields: Fe
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N. Schein, D.M. Haskin and R.G. Cla
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similar and allied forces the two e
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This movement is practically linear
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an assembly of the gravitator cells
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space were suddenly filled with man
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and utilizing it in the constructio
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APPENDIX ffl GRAVITY EFFECTS The or
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APPENDIX IV A LINK BETWEEN GRAVITAT
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APPENDIX VI WEIGHT-MASS ANOMALY The
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ABSTRACT Based on the asymmetry of
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do not favor such transitions, and
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THE U.S. ANTIGRAVITY SQUADRON by Pa
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Clearly, the overseers of black R &
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The saucers made by Brown have no p
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supersonic velocities. Also, in his
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Figure 5. A version of the flying d
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dielectrics are a likely choice for
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Figure 7. A side view of the B-2 sh
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which provides the electrostatic en
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for linearly accelerating negative
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Unit, London, February 1956. (Libra
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100
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Larry Deavenport is a hobbyist in e
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various levels and special notice w
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The Antigravity Research of T. Town
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Book Review Electrogravitics System
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The Hunt for Zero Point
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THE HUNT FOR ZERO POINT. Copyright
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Author's Note and Acknowledgments N
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Prologue The dust devils swirled ar
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Prologue xi The troops had been par
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Chapter 1 From the heavy-handed sty
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NICK COOK 3 Martin Aircraft Company
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NICK COOK 5 In the course of a deca
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NICK COOK 7 "negative weight"—a r
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NICK COOK 9 process, giving somethi
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NICK COOK 11 also levitate paper cl
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Chapter 2 In 1667, Newton mathemati
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NICK COOK 15 I had no direct eviden
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NICK COOK 17 cupped the receiver, b
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NICK COOK 19 Electrogravitics Syste
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NICK COOK 21 dismiss anything that
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NICK COOK 23 the following year swi
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NICK COOK 25 In this, according to
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NICK COOK 27 "degaussed" the brains
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NICK COOK 29 man responsible for so
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NICK COOK 31 Valone seemed quite un
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NICK COOK 33 model flying saucers b
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NICK COOK 35 trying to put the piec
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NICK COOK 37
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Chapter 4 History doesn't relate th
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NICK COOK 41 something—anything
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NICK COOK 43 Park, Maryland. What w
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NICK COOK 45 integral to most moder
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NICK COOK 47 the most baffling myst
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NICK COOK 49 Lusty files were old a
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NICK COOK 51 In the spring of 1941,
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NICK COOK 53 near Breslau under the
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NICK COOK 55 flying bomb designed t
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NICK COOK 57 his death in November
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NICK COOK 59 had developed a revolu
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NICK COOK 61 If there was any sense
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NICK COOK 63 A year after the war e
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NICK COOK 65 yet kicked in and my b
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NICK COOK 67 microfilmed documentat
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NICK COOK 69 reports made by aircre
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NICK COOK 71
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NICK COOK 73 What had I actually le
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NICK COOK 75 contract with the Avro
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NICK COOK 77 been built, but flight
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NICK COOK 79 inaccessible to more t
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NICK COOK 81 an antigravity effect
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NICK COOK 83 down the aircraft's la
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NICK COOK 85 principally to see if
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NICK COOK 87 It was then that I rea
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NICK COOK 89 started talking about
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NICK COOK 91 don't really have a ta
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Chapter 9 A larger-than-life depict
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NICK COOK 95 But ASTP did not end t
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NICK COOK 97 questions churned, as
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NICK COOK 99 He paused and rubbed t
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NICK COOK 101 propulsive antigravit
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NICK COOK 103 down. He was abandone
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NICK COOK 105 * * * On the flight d
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NICK COOK 107 reaction to the Podkl
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NICK COOK 109 Cleveland and, believ
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NICK COOK 111 These vibrating field
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NICK COOK 113 Union, using nothing
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Chapter 11 If antigravity had been
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NICK COOK 117 Stealth had the power
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NICK COOK 119 missions in the late
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NICK COOK 121 disclosure, however,
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Chapter 12 I'd been aware of rumors
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NICK COOK 125 Fellow of the Royal A
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NICK COOK 127 accurate total budget
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NICK COOK 129 F-l 17 A, composed of
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Below: Alleged photograph of Rudolp
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Left: John Frost. Below: A cutaway
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Above: British Aerospace's concept
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Above: The Northrop Grumman B-2 Ste
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Above: Map showing key California-b
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Below: SS General Hans Kammler - th
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Left: Bob Widmer, chief designer of
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Metal ingots 'disrupted' by the Hut
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132 The Hunt for Zero Point could s
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134 The Hunt for Zero Point impossi
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136 The Hunt for Zero Point Lockhee
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138 The Hunt for Zero Point The man
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140 The Hunt for Zero Point deduced
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142 The Hunt for Zero Point Brown's
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144 The Hunt for Zero Point Soviet
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Chapter 14 There were two final way
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148 The Hunt for Zero Point all our
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150 The Hunt for Zero Point encoura
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152 The Hunt for Zero Point Just as
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154 The Hunt for Zero Point the A-4
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156 The Hunt for Zero Point done an
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158 The Hunt for Zero Point as offe
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Chapter 16 According to Agoston, Ka
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162 The Hunt for Zero Point not, th
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164 The Hunt for Zero Point from Ka
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166 The Hunt for Zero Point mountai
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168 The Hunt for Zero Point service
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Chapter 17 I entered the complex fr
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172 The Hunt for Zero Point had spa
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174 The Hunt for Zero Point signed
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176 The Hunt for Zero Point and int
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178 The Hunt for Zero Point have ig
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180 The Hunt for Zero Point radiati
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182 The Hunt for Zero Point to use
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184 The Hunt for Zero Point "And th
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186 The Hunt for Zero Point activit
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188 The Hunt for Zero Point the rea
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190 The Hunt for Zero Point untimel
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192 The Hunt for Zero Point violet
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194 The Hunt for Zero Point There w
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196 The Hunt for Zero Point Even th
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198 The Hunt for Zero Point That ni
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200 The Hunt for Zero Point impenet
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Chapter 21 The next day, I was back
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204 The Hunt for Zero Point Many of
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206 The Hunt for Zero Point appeare
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208 The Hunt for Zero Point One suc
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210 The Hunt for Zero Point natural
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212 The Hunt for Zero Point
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214 The Hunt for Zero Point notion,
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216 The Hunt for Zero Point is busi
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218 The Hunt for Zero Point during
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220 The Hunt for Zero Point Via Sch
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222 The Hunt for Zero Point compres
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224 The Hunt for Zero Point detaile
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226 The Hunt for Zero Point U.S. si
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228 The Hunt for Zero Point the bes
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Chapter 23 Viewed from the back of
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232 The Hunt for Zero Point The ide
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234 The Hunt for Zero Point It was
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236 The Hunt for Zero Point spin-of
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238 The Hunt for Zero Point metal p
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240 The Hunt for Zero Point Martin,
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Chapter 24 The flight was several h
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244 The Hunt for Zero Point morning
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246 The Hunt for Zero Point I was i
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248 The Hunt for Zero Point was one
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250 The Hunt for Zero Point not, as
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252 The Hunt for Zero Point science
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254 The Hunt for Zero Point confirm
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256 The Hunt for Zero Point Einstei
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258 The Hunt for Zero Point had bel
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260 The Hunt for Zero Point theory
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262 The Hunt for Zero Point Hutchis
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264 The Hunt for Zero Point later,
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266 The Hunt for Zero Point Hutchis
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268 The Hunt for Zero Point objects
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270 The Hunt for Zero Point "When y
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272 The Hunt for Zero Point I could
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274 The Hunt for Zero Point that wo
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276 The Hunt for Zero Point orbitin
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278 The Hunt for Zero Point enough
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280 The Hunt for Zero Point Lucas,
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Index Page numbers of illustrations
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284 Index Brown, Thomas Townsend (c
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286 Index Gunston, Bill, 124-25 Gyr
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288 Index NASA (cont'd) Marshall Sp
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290 Index Tesla, Nikola, 258-60 Tun
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ABOUT THE AUTHOR Nick Cook is the A
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