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AAWSAP DIRD, Advanced Space Propulsion Based on Vacuum (Spacetime Metric) Engineering, March 2010

U.S. Department of War · 2010-03-29 · 17 pages · text from the file's own layer

This Defense Intelligence Reference Document, dated 29 March 2010 and prepared by the Defense Intelligence Agency's Defense Warning Office, is one of a series of FY 2009 advanced technology reports under the Advanced Aerospace Weapon System Applications Program. It uses a metric tensor approach from general relativity to catalog the physical effects of engineering spacetime. It covers time alteration, light speed, effective mass, and warp drives. It concludes that these effects are consistent with physics, but that engineering them remains a daunting constraint.

From the source: Release of 2026-09-18 Incident: 3/29/10, Las Vegas, Nevada. Released with redactions. This document is a Defense Intelligence Reference Document (DIRD), a technical reference format used by the Defense Intelligence Agency (DIA) to capture baseline knowledge on a specific topic for later analytic use. DIRDs are best understood as reference and synthesis products rather than as original research. It is one of 38 DIRDs produced under the Advanced Aerospace Weapon System Applications Program (AAWSAP) between 2009 and 2011. Because AAWSAP’s scope permitted a broad range of supporting topics, not every DIRD in the series directly concerns aerospace systems or future threat assessment. The following summary reflects the DIRD’s scope and framing at the time of writing and should not be read as implying current validation of the concepts discussed. This DIRD examines the idea of vacuum or spacetime-metric engineering: the possibility that an unspecified future technology might alter the structure of spacetime in ways useful for propulsion, power generation, or extremely rapid long-distance travel. Using general relativity as a model-independent framework, it explores the physical effects that would theoretically follow if such metric changes could be artificially induced, including altered time rates, changes in effective mass, modified light propagation, gravity-like effects, and warp-drive propulsion. The document does not propose any mechanism for generating these effects and treats these physical consequences as an assumed result of spacetime manipulation rather than as the outcome of a practical engineering pathway. It also emphasizes that the energy requirements predicted by current theory to create such effects are far beyond existing technological capability.

UNCLASSIFIED/ /FOR OFFI@IAL 1::191!! 8HLY
Table 1. Metric Effects on Physical Processes in an Altered Spacetime as
Interpreted by a Remote (Unaltered Spacetime) Observer
Variable Typical Stellar Mass
(goo 1)
Spacetime-Engineered
Metric
(g(X) > 1, lg11 I c
Mass m= E/ c2 ➔ (-gIJ.Ji:;)m Effective mass increases Effective mass decreases
Gravitational "force"
f(g oo ,81 1) "Gravitational" "Antig ravitationa I"
Spatial Interval
Again, by considering the case typical for an altered spacetime metric in the vici nity of,
say, a stellar mass, then ~ > 1 for the radia l dimension x1 = r, as expressed by the
second term in Equation ( 4 ). Therefore, local measurements with physical rulers within
the altered spacetime yield a spatial interval ~dr > dr; thus a spatial interval dr
between two locations in an undistorted spacetime- say, remote from the mass- would
be judged by local (proper) measurement from within the altered spacetime to be
greater. From th is one can rightly infer that, relatively speaking, rulers (atom ic
spacings and so forth) within the altered spacetime are shrunken relative to their
values in unaltered spacetime. Given this result, a physical object (for example, atom ic
orbit) that possesses a measure !::.r in unaltered spacetime shrinks to !::..r ➔ t::.r/ ~
when placed with in the altered spacetime . Conversely, under conditions for which
~ < 1, objects wou ld expand-thus the fourth ent ry for the table of physical effects.
Velocity of Light in Spacetime-Altered Regions
Interior to a spacetime reg ion altered by, say, a dense mass (for example, a black
hole), the locally measured velocity of light c in, say, the x1 = r direction is given by the
ratio of locally measured (proper) distance/time intervals for a propagating light signal
( Reference 13).
; .J-g,1 dr
V = --- = C (6)
L ..{i;;dt
UNCLASSIFIED/ /FOR OFFI@IAL l::ISE OHL¥
4

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Official release, from the pursue collection. The PDF is mirrored here; the original link is above. 17 pages are in the text index: search them above, or from the library's search.