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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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spacecraft. This creates coherent RF or optical apertures that are essentially unlimited
in size, which could offer unprecedented high-resolution radiometry, hyperspectral
imaging, radar, and RF interception (for mapping, surveying, MASINT, SIGNIT), etc.
Launching laser-propelled Lightcraft nano-/pico-satellites to LEO requires megawatt-
class lasers. TEXTRON Systems Corporation's proposed 10 MW electron gun-driven
CO2/gas mixture laser is a multi-megawatt-class system that can be implemented now
because this technology requires little or no additional R&D. This system offers realistic
near-term, low-cost Lightcraft launch capability. However, this system is large,
requires a large amount of gas propellant to fuel the laser, and the system
infrastructure will cost over $200 million.
The newly emergent bulk slab solid-state, high-power fiber, and free-electron laser
technologies being explored by the various DoD directed energy weapons programs
offer higher electrical-to-optical efficiencies and overall laser performance, compact and
portable system size, less complexity and smaller weight, all at much lower system and
infrastructure cost. These lasers are scalable to megawatt-class beam power, and so
we roughly estimate that the overall system and infrastructure cost to deploy such laser
systems to launch a Lightcraft to LEO will be from several factors to an order of
magnitude (or more) lower than for the electron gun-driven CO2/gas mixture laser
system.
Removing the waste heat produced by high-power laser systems is an important factor
driving the physical limitations of scaling up the beam output power. An innovative
matched-refractive-index liquid is used to rapidly remove the heat produced by a 150
kW bulk slab solid-state laser weapon while the very high surface area-to-volume ratio
of high-power fiber lasers allows for the rapid removal of heat from the gain medium
without the need for external cooling. Phase-change materials are being explored and
devices using such materials have recently demonstrated the ability to store very large
quantities of the waste heat produced by high-power solid-state lasers, which is a
different way of rapidly removing large amounts of heat from the solid-state gain
medium. Unlike solid-state laser systems, free-electron lasers are not affected by heat
problems while their gain medium (a vacuum) cannot be damaged.
Launching a laser-propelled Lightcraft nanosat/picosat from the ground, sea, or air into
LEO requires controlling and steering the high-energy laser beam, while at the same
time making real-time adjustments to account for platform motion, optical train and
atmospheric effects on beam propagation, so that the beam maintains high quality,
low-loss, precision contact with the Lightcraft during the entire flight. Recent technical
innovations in optical train design and other system architecture have evolved beam
control devices for high-energy laser weapons toward new implementations. New beam
control devices and high-power optical train combinations have a resulting beam line
that is considerably simpler, smaller and lighter than current architectures. Almost
every component in the beam line performs multiple functions, thereby dramatically
reducing the high-power optical component count. This approach also packages all
beam control sensors, processors and drivers into a single turret assembly.
In 2005, the AFRL/PRSP (Edwards AFB, CA) concluded their laser Lightcraft propulsion
R&DTE program before launching a Lightcraft test vehicle into LEO was demonstrated
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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.