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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…
UNCLASSIFIED/,, OK 01 I ICIAE 652 one I
These array functions can be made coherent over very great distances. RF antennas
with sizes of hundreds of kilometers and optical telescopes of hundreds of meters
diameter can be formed. These systems can enable new capabilities not possible with
single spacecraft either acting alone, as a proliferated but non-coherent constellation,
or as relays for each other. Formed of nanosats and picosats, such swarms will contain
so many spacecraft that the economics of true mass production will come into play in
space for the first time, greatly reducing the cost of producing the system. In addition,
these systems feature the advantages of truly distributed satellite systems, including
fault tolerance, robustness, survivability, reconfigurability by software, and the ability
to be incrementally emplaced and upgraded as budgets are available.
These swarms can be implemented in a cost effective manner using laser propulsion for
both launch and orbital insertion. However, the system designs described in the
following sections are flexible enough to allow for the use of alternative conventional
launch vehicle technologies. The technologies to produce these swarms and their
constituent nanosats or picosats probably can be demonstrated by 2015 and deployed
in space by 2020.
The following concepts were provided via the voluminous research notes, lectures, and
briefings provided courtesy of I. Bekey.
ROTATING PICOSAT SWARM ARRAY RADIO FREQUENCY COLLECTOR
An unconventional, large sparse antenna array RF collector spacecraft with a small
surface footprint even when deployed in geosynchronous Earth orbit (GEO) separates
different sources in proximity and also detects weak signals. Its implementation would
result in a highly desirable, long dwell RF emitter detection capability.
At the heart of this system is a large antenna that is formed by a swarm of tiny
elements that make up the lens of a space-fed array with no structure. The antenna is
a sparse, self-cohering array formed from a large number of picosats rotating (in
relative coordinates) in a plane around a central orbital point in GEO. The picosats are
self-contained repeater spacecraft. Each one receives the ground signal, delays it, and
retransmits the signal so that it arrives at the feeds at the same time as a direct ray
through the center of the array. The time delay of each picosat is self computed based
on its location in the swarm, as measured by a local differential global positioning
system (DGPS)-like navigation signal, to compensate for its deviation from its assigned
ideal location. Each picosat digitizes, delays, frequency shifts, and retransmits its
received signals independently, causing an in-phase composite signal from the ground
to be received at the feeds.
The relative positions of these picosat elements change slowly, and only small and
infrequent propulsive maneuvers are needed for constellation maintenance. A tether
along the local vertical at the central point holds the receivers and DGPS-like reference
at the focus against a counterweight. A pseudorandom distribution of the picosats
suppresses the antenna grating lobes, and intensive computation greatly reduces much
of the remaining sidelobes, creates multiple beams, and steers the ensemble of the
individual beams anywhere on Earth. The antenna system will function with far fewer
elements as a more sparse array, though with limited sensitivity. This system can be
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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.