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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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An outline of the conceptual design features of the proposed 10 MW electron gun-driven
CO2/gas mixture laser is [29]:
• Scalability of total beam output power, beam combining concept.
• Power oscillator or master oscillator-power amplifier (MOPA) design.
• Unstable optical resonator cavity with grating and rotating mirrors beam-combine
techniques.
• Flow and gas handling system with blow down and exhaust to the atmosphere.
• Acoustics suppression with expansion horn downstream and anode muffler.
In this concept there are four separate laser transmitters each generating 2.5 MW
output beams that are combined into a single 10 MW output beam. The oscillator
parameters for each beam transmitter are [29]:
• Energy loading, Ep: Ep = 300 J (higher loadings at reduced gas temperature);
gain volume = 0.27 m 3 (x 4 lasers); A to K = 0.3 m; gain length = 3 m.
• Specific laser output = 65 J/1.
• Estimated extraction efficiency = 20%.
• Pulse repetition rate: 125 Hz@ 20μs.
• Laser power, P = 2.5 MW/beam x 4 beams = 10 MW.
• Laser energy per pulse = 18 kJ/beam x 4 beams = 72 kJ.
• Output wavelengths: 10.6 ~tm, 10.2 ~tm, 9.6 ~tm, and 9.3 μm (mixed).
• Gas mixture ratio (for N2:CO2:H2): 3:1:0.08.
• Gas pressure = 1.013 x 10 5 Pa (or 1 atmosphere).
• Flash factor= 1.3.
The optical resonator cavity and optical components specifications are [29]:
• Resonator type: confocal unstable with rotating mirrors beam combining.
• Magnification, M = 4.
• Cavity length, L = 36.5 m.
• Equivalent Fresnel number = 3.4.
• Cavity end mirrors radius of curvature: RMirror1 = 97.3 m (concave), RM1rror2 = 24.3
m (convex).
• Gain cell: volume= 0.3 x 0.3 x 3.0 m 3 , length= 3 m.
• Beam combine mirrors: 75 x 75 cm 2 flat (30 x 30 cm 2 apertures) @ f. = 10.59
~Lm.
• Low pressure hot cell: 0.3 to 0.5 GHz suppression near line center.
• Output scraper mirror: D = 0.075 m (taped).
See Figure 16 and Figure 17 for schematics of the power oscillator optics and the MOPA.
The laser operation requirements for the gas flow system are (see Figure 18) [29]:
• Flow System: blow down.
• Gain Section
• Cross-section, A= 0.3 m x 3.0 m = 0.9 m 2 .
• Volume, V = 0.3 m x 0.3 m x 3.0 m = 0.27 m 3 .
• Flow speed, u = SO m/sec (@ 125 Hz & flash factor= 1.3).
• Dynamic pressure, !'..P = 2000 Pa (or 0.02 atmospheres).
• Mass flow rate, Q = 60 kg/sec per module ( 45 m 3/sec std).
• Run time, t = 300 seconds
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