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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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Chapter 5: Conclusion
To reduce mission costs, advanced technology components and a novel laser propulsion
system can make nanosats (and picosats) compact, lightweight, low power, and low
cost. By producing a large quantity of nanosats for a given mission, the per-unit cost
will be reduced to a small fraction of satellite procurements for traditional missions.
Mission operation costs will be minimized by the incorporation of both onboard and
ground autonomy, use of heuristic systems, and use of a novel laser propulsion system
to launch the nanosats into LEO. Laser propulsion is an enabling technology in which a
laser-propelled vehicle, called "Lightcraft," harnesses the energy of a high-energy laser
beam and converts it into propulsive thrust.
The laser-propelled Lightcraft is an ETO transportation system that develops quasi-
steady (airbreathing) thrust by pulsing at a variable rate along the flight trajectory to
orbit, and then when it climbs above the atmosphere it begins to operate in the thermal
rocket mode using onboard propellant to convert and expand the laser energy for
propulsion. The Lightcraft is spin-stabilized and can be launched vertically upward or
on a slant upward trajectory, hover in mid-air, and undergo powered descent and
landing. The system is single-stage-to-orbit and completely reusable with no onboard
propellant required (the reaction mass is free air), except for the small internal amount
of propellant needed for final ascent to orbit and orbital maneuvering. MEMS FEEP
thrusters could provide onboard attitude and stationkeeping propulsion. The Lightcraft
specific impulse is essentially infinite (several thousand seconds in rocket mode), while
payload mass fractions are 50% to 95%.
Laser-propelled Lightcraft systems are simple, reliable, safe, environmentally clean, and
could have a very high all azimuth on-demand launch rate. This novel propulsion
system reduces space launch costs by two to three orders of magnitude below today's
levels, with estimated launch costs of $20 per kg to $600 per kg of payload, not
including life-cycle and recurring launch operations costs. The entire Lightcraft launch
system is comprised of a ground, sea, or airborne laser beam generator consisting of a
power supply, a high-power (megawatt-class) laser beam generator/transmitter using
novel beam optics, and automated tracking, hand-off and safety systems.
The most promising military mission for laser-propelled Lightcraft is the placement of
Earth and space observing nano-/pico-satellites of up to 3 kg mass into LEO. Such
Lightcraft could also serve as a "Lightsat," because it would use the Lightcraft's laser
propulsion optics as a telescope for observing military targets on Earth and in space.
Such a Lightcraft system appears capable of reaching LEO at 1/Sth to 1/lOth the cost
required for placing a similar Lightsat system into LEO using multistage chemical rocket
systems. Other potential missions include using laser-propelled Lightcraft as
ground/sea- or airborne-launched kinetic kill weapons to shoot down enemy ballistic
missiles. Very innovative near-term missions could also include deploying Lightcraft
nano-/pico-satellites to form swarms of small spacecraft which cooperate coherently to
form a real distributed system in which the whole is more than the sum of the parts.
This would be a constellation of small spacecraft each performing its separate function,
but these functions combine to create at a central location a much larger virtual
spacecraft, or sensor aperture, that exists solely because of the cooperation of the
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