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Defense Intelligence Reference Document Laser Lightcraft Nanosatellites

Defense Intelligence Agency · 77 pages · text from the file's own layer

This Defense Intelligence Reference Document from the Defense Intelligence Agency, dated 1 November 2010, was produced under the Advanced Aerospace Weapon System Applications (AAWSA) Program. It describes nanosatellite technologies and proposes launching nanosats into orbit with laser Lightcraft propulsion. It also covers a weapon mission selection study and multi-megawatt laser options. The author recommends that the Department of Defense and NASA bring Lightcraft R&D back to the United States and restart the X-50LR flight demonstration program.

  • p. 4 …Influence of Target Velocity and Intercept Angle on Impact Energy and Required Mass .................................................................................................. 33 Table 5…
  • p. 5 …The term "minisatellite" refers to a spacecraft with a wet mass (including onboard propellant) of 100…
  • p. 7 …Nanosatellite Technologies OVERVIEW Nanosats require technologies that radically reduce the mass and power of components without…
  • p. 8 …nanosat presents some unique challenges, with low mass (0.25 kg) and low power (0.5…
  • p. 9 …In order to develop a low mass C&DH, a lightweight and low power electronics packaging…
  • p. 11 …RF COMMUNICATIONS The onboard RF subsystem must be small, low mass, and low power. The system…
  • p. 12 …additional strain on an already challenged nanosat mass and power budget. For this reason, the concept…
  • p. 13 …The material will be selected based on mass, cost, manufacturability, ease of assembly and integration, and…
  • p. 15 …for the spacecraft because a large propellant mass and heavy energy source are not carried onboard…
  • p. 17 …Current Lightcraft designs are limited to about 60 g mass and 15 cm in diameter by…
  • p. 21 …It requires a beam power of 0.1 to 1 MW per kg of vehicle mass…
  • p. 22 …The majority of the system mass required to launch a payload to orbit is left on…
  • p. 24 …Therefore, this would allow approximately 4 kg of mass to be placed into orbit with the…
  • p. 25 …same ply-thickness) to meet Lightcraft airframe mass requirements. Another important finding in the study was…
  • p. 31 …Additional estimated mass for performing the Lightsat function is no more than about 1 kg, if…
  • p. 32 …Lightcraft takeoff masses no more than about 20 kg can be accelerated to orbital velocities by…
  • p. 33 …for missile and maneuvering aircraft interception. • Additional mass along Lightcraft centerline for hardened target penetration. LIGHTCRAFT…
  • p. 34 …Lightcraft sizing assumed a propellant mass fraction of 0.5 and 1.0 MW of laser…
  • p. 35 …Hybrid Rocket Expendible Launch Vehicle - Assumed Perfonnance and Estimated Weights Payload Mass (kg) 1.00 5…
  • p. 37 …It is therefore estimated that the air-to-space Lightcraft dry mass would be about the…
  • p. 38 …Influence of Target Velocity and Intercept Angle on Impact Energy and Required Mass 2 61. Lightcraft…
  • p. 39 …Influence of Lightcraft and Target Velocity on Impact Energy and Required Mass 261. Lightcraft Lightcraft Impact…
  • p. 40 …The lower mass also saves launch costs, so the total system costs less for the same…
  • p. 41 …many spacecraft that the economics of true mass production will come into play in space for…
  • p. 44 …the local vertical, with its center of mass in GEO. The Fresnel zone plate has a…
  • p. 46 …wall plug and optical efficiencies, cost, complexity, mass, and size. Free-electron lasers are another class…
  • p. 47 …P = 2000 Pa (or 0.02 atmospheres). • Mass flow rate, Q = 60 kg/sec per module…
  • p. 48 UNCLASSIFIED//509 AEEJCJOP 11£5 O.-blf + Total mass flow rate, Qtota1 = 240 kg/sec for…
  • p. 50 …sec, and 15 kg/sec of CD2 mass flow represents 2.053 x 1026 molecules/sec…
  • p. 51 …The 60 kg/sec mass flow requirement of the 3: 1 N2/C02 lasing gases means…
  • p. 53 …mass (not including the prime power and cooling systems) to achieve the low specific mass (5…
  • p. 65 …is the undulator period, mis the electron mass, and c is the speed of light. 'MeV…
  • p. 72 …The Lightcraft specific impulse is essentially infinite (several thousand seconds in rocket mode), while payload mass…
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push broom scanning mode for complete Earth coverage rather than only sampling
coverage.
The constellation/array implementation is similar to that of the preceding concept (High
Resolution Surface Sampling Radiometry section), except that tethers hold a receiving
array that must be 2 km long to obtain the 1,200 km instantaneous swath width with a
resolution of 100 m. It consists of a 2 km long focal surface with 12,000 printed
dipoles, shaped into a focal surface by gravity gradient forces balanced against
magnetic forces from a superconducting conductor around its periphery, acting on a
piezoelectric, electron beam-shaped, adaptive membrane substrate. The large antenna
is formed by a swarm of tiny elements making up the lens of a space-fed array.
The antenna is a 4 km x 6 km diameter, sparse, self-cohering array formed from
12,000 picosats weighing 23 grams each, rotating in relative coordinates in a plane
around a central orbit point. The picosats are similar to those of the preceding concept
(High Resolution Surface Sampling Radiometry section). Their locations are initially
selected to lie in a plane, and their spacings are pseudorandom to minimize the
sidelobe levels, with each picosat designed to loosely stationkeep inside a box 10 m on
a side. The relative positions of these picosat elements changes slowly, and only small
and infrequent stationkeeping propulsive maneuvers are needed for constellation
maintenance.
The effective collecting aperture of the array is the sum of those of the picosats, and in
this concept, equal to that of an equivalent 6 m diameter antenna at 2 GHz. However,
the coverage spot diameter is set by the total aperture diameter of 4 km x 6 km, and
thus is 100 m at 2 GHz from a 4,000 km orbit. Five constellation/arrays would produce
100% global coverage with 5 hour revisit for time critical measurements. The entire
constellation weighs 3,000 kg, but that could be reduced in the future to 30 kg if
Buckytubes are used to construct the system.
ROTATING NANOSAT SWARM DISTRIBUTED RADAR
An extremely powerful space-based radar, this concept would allow detection of most
air, land, sea, and space targets, as well as many "low observable" targets anywhere,
with one or a few constellations in GEO. A large, sparse array antenna using a swarm
of nanosats creates a space-based radar system. The constellation/array
implementation is similar to that of the preceding rotating swarm concepts, except that
it generates and radiates extremely large peak and average powers, and given the
generally high angles of viewing can detect and track many air, space, and surface
targets from GEO.
The constellation is composed of 10,000 nanosats that are self-contained repeater
spacecraft weighing about 1 kg each. Each nanosat receives the ground signal,
digitizes, delays, and retransmits it, causing it to arrive at the feeds at the same time
as a direct ray through the center of the array. The time delay of each nanosat is self
computed based on its location in the swarm, as measured by a local DGPS-like
navigation signal, to compensate for its deviation from its assigned ideal location.
Commands for beam sweep delays are superimposed on the time delays of each
nanosat. Each nanosat generates 10 W of average power and 10 kW peak power at
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39

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Report, from the dia collection. The PDF is mirrored here; the original link is under it. 77 pages are in the text index: search them above, or from the library's search.