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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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0.001 duty cycle, has a helical film antenna that increases its gain and doubles as a
solar sail for infrequent stationkeeping maneuvers, and has a tether for coarse gravity
gradient stabilization. A SO km tether supports the feed, transmitter, and DGPS
reference assembly against a counterweight. The antenna lens is 2 km x 4 km.
The effective area of the array is the same as that of a SO m diameter filled aperture.
The total effective RF radiated power of the system is 3 GW peak and 3 MW average.
Although specific performance calculations have not been done for this concept, these
powers are so large that the radar should have the sensitivity from its location in GEO
for detecting and tracking many targets simultaneously and most "low observable"
targets as well because they are all designed and oriented so as to have their low
observables in near-horizontal directions. Three constellations would provide
essentially complete global coverage. The entire constellation weighs about 11,000 kg
in GEO (this could be reduced in the future to 110 kg if Buckytubes are used to
construct the system) and can be emplaced and replaced incrementally using laser-
powered Lightcraft launch vehicles or even small conventional launch vehicles. It could
even be funded incrementally.
Simple, Distributed, Hyperspectral Sensor
This concept presents an unconventional method of implementing a hyperspectral
sensor of great spectral and spatial resolution. Its implementation would allow the
detection of very many spectral intervals simultaneously, and it has a small field of view
from GEO so that the instrument can dwell on and resolve particular targets of interest.
It also has a large field of regard so that one spacecraft covers a significant fraction of a
hemisphere.
The concept uses a Fresnel zone plate, which is oriented roughly parallel to the local
horizontal just below GEO. It is supported by a tether that extends well above the GEO
altitude, and may or may not have a counterweight at the top end. The gravity
gradient causes the ensemble to remain Earth pointing along the local vertical, with its
center of mass in GEO.
The Fresnel zone plate has a long focal length, and thus the surface and ring locations
can be imprecise compared with conventional optics. In addition, the lens is a thin film
membrane and will be light and inexpensive. It is highly frequency dispersive, and thus
its focal length is a sensitive function of wavelength. Small, self-contained optical
sensor nanosats are placed on the tether at many locations with each nanosat's optics
filtered for response at only that narrow spectral region focused at its distance from the
lens. The nanosats can transmit directly to the ground or their signals can be combined
in one transceiver, also on the tether.
This system has a 100 km long tether, which weighs only a few kilograms in GEO. The
Fresnel zone plate is 100 m in diameter, has a collecting aperture equivalent to a 30 m
filled aperture, and requires only a surface accuracy of centimeters in the visible light
region. It is constructed of thin film with deposited aluminum rings and is an adaptive
piezoelectric membrane kept flat by an electron beam in response to an optical figure
sensor. MEMS FEEP thrusters are at the sensor's periphery for attitude control, with
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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.