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HHRG-118-GO06-20230726-SD005.pdf
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UNCLASSIFIED/, .... %J... Defense Intelligence Reference Document Acquisition Threat Support 29 March 2010 ICOD: 1 December 2009 DIA-08-1003-015 Advanced Space Propulsion Based on Vacuum (Spacetime Metric) Engineering UNCLASSIFIED/ frPer*.PFbeterhad
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UNCLASSIFIED//m° nr"CT I "Cr " Advanced Space Propulsion based on Vacuum (Spacetime Metric) Engineering Prepared by: (b)(3):10 USC 424 Defense Intelligence Agency Author: (b)(6) Administrative Note 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 2009 under the Defense Intelligence Agency, (b)(3) USC 424 Advanced Aerospace Weapon System Applications (AAWSA) Program. Comments or questions pertaining to this document should be addressed to (b)(3) 10 U…
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UNCLASSIFIED/ /P011•01FRIGkoplmW&FQIIM‘m. Contents Advanced Space Propulsion Based on Vacuum (Spacetime Metric) Engineering iii Preface and Introduction iii I. Spacetime Modification - Metric Tensor Approach 1 II. Physical Effects as a Function of Metric Tensor Coefficients 2 Time Interval, Frequency, Energy 3 Spatial Interval 4 Velocity of Light in Spacetime-Altered Regions 4 Refractive Index Modeling 5 Effective Mass in Spacetime-Altered Regions 6 Gravity/Antigravity "Forces" 6 III. Significance of Physical Effects Applicable to Advanced Aerospace Craft …
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UNCLASSIFIED/ /a1‘91FRIGial Advanced Space Propulsion Based on Vacuum (Spacetime Metric) Engineering Preface and Introduction A theme that has come to the fore in advanced planning for long-range space exploration in the future is the concept that empty space itself (the quantum vacuum, or spacetime metric) might be engineered to provide energy/thrust for future space vehicles. Although far reaching, such a proposal is solidly grounded in modern physical theory, and therefore the possibility that matter/vacuum interactions might be engineered for spaceflight applications is not a pri…
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UNCLASSIFIED components of potential utility involve very-small-wavelength, high-frequency field structures and thus resist facile engineering solutions. With regard to perturbation of the spacetime metric, the required energy densities predicted by present theory exceed by many orders of magnitude values achievable with existing engineering techniques. Nonetheless, one can examine the possibilities and implications under the expectation that as science and its attendant derivative technologies mature, felicitous means may yet be found that permit the exploitation of the enormous, as-y…
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UNCLASSIFIED/)TM'ell•PieNe&tle&OPSW I. Spacetime Modification - Metric Tensor Approach Despite the daunting energy requirements to restructure the spacetime metric to a significant degree, one can investigate the forms that such restructuring would take to be useful for spaceflight applications and determine their corollary attributes and consequences. Thus we embark on a "Blue Sky," general-relativity-for-engineers approach, as it were. As a mathematical evaluation tool, the metric tensor that describes the measurement of spacetime intervals is used. Such an approach, well known from …
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UNCLASSIFIED/ / rOR ornimm-/ with the metric tensor coefficients modifying the Minkowski flat-spacetime intervals dt, dr, , and so forth, accordingly. As another example of spacetime alteration, in a spacetime altered by the presence of a charged spherical mass distribution (Q,m)at the origin (Reissner-Nordstrom-type solution), the above can be transformed into (Reference 11) Q 2G zlirece4 1+ Gm/ rc2 r 2 +Gmi rc 2 )1 —(1+ Gm/ rcl r 2 08' + sin' 041 d.s? = -[ Q2G AZ60(4 2 (1 Gm/rc2 ) 2 - G11 C 2 1+ Gm rc (5) with the metric tensor coefficients g again changed accordingly…
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UNCLASSIFIED/ friM~PPItl~defrieffitaF TIME INTERVAL, FREQUENCY, ENERGY Begin by considering the case where Vg< I, typical for an altered spacetime metric in the vicinity of, say, a stellar mass, as expressed by the leading term in Equation (4). Local measurements with physical clocks within the altered spacetime yield a time interval igtmdt <di ; thus an interval of time dt between two events in an undistorted spacetime remotel from the mass—say, 10 seconds—would be judged by local (proper) measurement from within the altered spacetime to occur in a lesser time interval, Vgoodt<dt —say…
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