DIRD_29-DIRD_Negative_mass_Propulsion.pdf

UNCLASSIFIED / / P@R-@FFt6ti=-VGE-OdiaGee Defense Intelligence Reference Document Ft i‘(‘CSéCés Defense Futures 03 January 2011 ICOD 30 August 2010 DIA-08-1101-023 Negative Mass Propulsion UNCLASSIFIED / /@@Re@EPiGitdeSEn0 deers

UNCLASSIFIED / / B@®-@FFIGHV6E-O2= Negative Mass Propulsion ' The Defense Intelligence Reference Document provides non-substantive but authoritative reference information related to intelligence topics or methodologies. Prepared by: (b)(3):10 USC 424 Defense Intelligence Agency Author: (b)(6) Administrative Notes: (U) COPYRIGHT WARNING: Further dissemination of the photographs in this publication is not authorized. This product is one in_a series of advanced technology reports produced in FY 2010 under the Defense Intelligence Agency, |(b)(3):10 USC 424 Advanced Aerospace Weapon System Applica…

UNCLASSIFIED / / R@R-@EEEGitinWEE- ORG Contents 1. IMtrOMUCEION occ ccc eee ener enn E een A EEE ESE EE EE EE ESET EEDA DEO SG EG EO SO TERED SEES EEE OE OR 2 2. The Theory by BOndi.......ccccccecetecctecneeeeeecateeereseteseeugereueeeuueesertantesureceeeugeueeetenes 4 3. Hund’s Nonlinear Newtonian Theory Of Gravity ....... cc cccccceceee eee eeeeeeeeeeneeneeenenaenens 6 4. The Theory of Bondi Revisited .......ccccccccccecceeceseeceeeteereeetseeeeeeeneerecrsgurerseenenneas 10 5. The Zitterbewegung Phenomenon as a Manifestation of Negative Masses .........05 10 6. Planck Aether Hypothesis .....…

UNCLASSIFIED / / EAR. OSGi SEONEYT Negative Mass Propulsion Summary It is easy to prove that there are negative masses all around us, albeit hidden behind positive masses. But their use for propulsion by reducing the inertia of matter, for example in the limit of macroscopic bodies with zero rest mass, depends on a technical solution to free them from their imprisonment by positive masses. It appears that there are basically two ways this might be achieved: 1. By the application of strong electromagnetic or gravitational fields or by high particle energies; 2. By searching for places in the un…

UNCLASSIFIED / / F@R-@FFEGE=VSE-Ontr 1. Introduction If we extend the law of gravity to negative masses, but hold onto the equivalence of inertial and gravitational masses, we have to distinguish between the following four cases, if a test particle is placed near a gravitational field producing mass (Table 1): Table 1. Interactions Gravitational field Mass of test Mation of test producing mass particle particle Under the principle of equivalence if a negative test mass particle would be placed in the gravitational field of earth, it would not fall upwards, as happens in science-fiction antigra…

UNCLASSIFIED / /§0R-OFFtGRE USE ORnteY™” If both masses are positive, we have the usual Newtonian attraction. For negative masses, the force has the same magnitude but is repulsive. A quite different situation exists if one mass is positive and the other one is negative. With both forming a mass dipole, the system becomes self-accelerating, because one mass is repelled and the other one attracted. With the two masses having opposite sign, the total energy and momentum of the combined system remains zero for all times, leaving intact the conservation laws of energy and momentum. Under its self-…

UNCLASSIFIED / /®@R-OPPfCR-USE-ONE Apart from Einstein’s purely kinematic interpretation of special relativity, being the expression of a Minkowskian space-time structure, there is an older alternative dynamic interpretation by Lorentz and Poincaré. In it space and time are absolute, but it can explain all relativistic effects as well. It assumes the existence of an aether, with all objects in absolute motion through the aether suffering a Lorentz contraction and time dilation. If this aether has a grainy structure, characterized by some smallest length (e.g., the Planck length ~ 10-33 cm), th…

UNCLASSIFIED / / 5OR-@EELGRA=GE-ONE Inserting (3-6) into Einstein’s nonlinear gravitational field equations, one obtains four nonlinear partial differential equations (K =87 y/{e4 ) given by % ldo (é@ = -Kp =-KT? =e?) -2V°94 Vo —--—— 4 | — 7 Kp =k ‘ - ? on r ano (28). +( OF 7) —KP, =—-KT| = KT; =Kp, =e"? | - leo 22) +(22) (8) 0 * r Ole \ ahh shen > leo (dg ° CQ ° _ =—KTS =e | Vo —--— 4] 1 4+ KPa STKE SE rary (2 (22) 9) —«T,, = 222 PO (10) - ORO Oe In solving these equations Bondi assumes that 9 is small, which then also implies that because of (5) and (6) o is small by the second order, reduci…