Documents / Report

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//EAR AEEJGJPk WEE &••LY
inclination relative to the ecliptic, will reduce the maximum eclipse period to about one
hour. Inclusion of spacecraft batteries is then justified. Passive thermal control will be
used to keep the spacecraft electronics within 10°c of ambient temperature, and hence
will not require electric power for heating. Using such a scenario, a battery
requirement of about 2 amp-hours at 3.3 volts will allow full spacecraft functionality
during an eclipse. Twelve AA size Lithium-ion batteries meet the requirement and only
weigh 480 grams.
Circuits that have high current demands, such as thruster solenoids and fuses, need to
be augmented with components that have a lower power density than batteries, but
also have lower internal resistance. Ultra-capacitors are being explored for this
application.
Miniaturization of the power system electronics (PSE) to meet the weight and size
requirements of the nanosats is a considerable challenge. The ideal approach is to
eliminate the PSE completely, by having a fixed electrical load and batteries provide the
needed bus regulation. This yields a simplified system consisting of solar cells,
batteries, and minimal circuitry. A more immediate approach to miniaturization is to
produce hybrid modules that measure approximately 5.08 cm x 3.17 cm x 1.27 cm
and weigh 100 grams for each PSE component, namely the solar array regulator,
battery regulator, and low voltage power converter. The combination of these three
components into one module will reduce the size and weight another order of
magnitude.
THERMAL
Although an inclination change by 10° renders maximum shadows below two hours, we
evaluate the case of a maximum eight hour shadow for the purpose of generality.
Three thermal configurations are considered: (1) top and bottom of the nanosat are
insulated, the inside of the cylindrical solar array is not insulated, allowing internal heat
transfer between the internal equipment and the array; (2) the entire nanosat is
insulated, top and bottom as well as inside the solar arrays, except for a radiator on
top, sized to radiate the internal electrical dissipation; and (3) the internal equipment is
thermally isolated as well as possible from an "outside shell" with a controllable two-
phase heat transport device which can be "shut off" during Earth shadows, serving as
the only thermal coupling between the equipment and a radiator on the outside surface.
The key advantage of configuration (1) is its reliability, or robustness. Since the
temperature of the nanosat is set by a high energy balance (heat in - heat out)
dominated by the absorbed solar energy, the operational temperature of the nanosat is
relatively insensitive to top and bottom multilayer insulation (MLI) properties, or,
largely, to internal heat dissipation. However, the feature that yields the operational
reliability, i.e., the high energy balance, also results in a rapid drop in temperature
when the solar load disappears during the Earth shadow. During the maximum eight
hour eclipse used for this evaluation, it was found that internal temperatures dropped
by about 60 8
C, which would result in internal temperatures in the range of -30 8
C to
-40°C. At the same time, the solar arrays dropped to a temperature of about 60°C.
Based on past experience, these end-of-eclipse temperatures are reasonable.
6
UNCLASSIFIED//FQA: QFFIGI11J.k WEE Q•lklf

Not linked to a story yet.

About this file

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.