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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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ground, sea and air launches of Lightcraft to LEO with air launch occurring at either
subsonic or hypersonic speed.
Lightcraft Ground/Sea to Space Investigation
The current Air Force Lightcraft vehicle concept has been designed for not only placing
nanosats into LEO at low cost (Figure 14), but also for performing much of the nanosat
function as well. In this concept the precision optics system that focuses ground/sea-
based laser light into the Lightcra~'s cowl area for propulsion is also used as a space
telescope for viewing military targets on Earth and in space. And structural panels on
the Lightcraft forebody are also used as solar panels that are unfurled in orbit for
generation of satellite power. Thus, the current Lightcraft's design allocates only 0.1 kg
of its 1.0 kg dry mass for exclusively nanosat functions. There is a military need for 1.0
kg to 2.0 kg nanosats with optical sensors for visual inspection of unknown objects in
space and on Earth.
Since conventional expendable rockets could conceivably be an alternative to laser-
powered Lightcraft for the rapid placement of military nanosats in LEO, a cursory
comparison of Lightcraft and conventional rockets was made by Froning and Davis [26]
to get some idea of their comparative costs. Hybrid rocket sizing and costing was
based upon tactical strategic missile sizing and costing information possessed by H. D.
Froning. This information related costs (in 1982 dollars) to rocket and payload
characteristics. Lightcraft sizing assumed a propellant mass fraction of 0.5 and 1.0 MW
of laser power per pound of payload (dry mass) placed into orbit. Costs for laser power
and refurbishment were based upon AFRL estimates (amortized over a fewer number of
flights). Although these Lightcraft and laser costs are higher (based upon much fewer
flights) than those of previous AFRL estimates, they are believed to be consistent with
the conventional rocket costs, and therefore applicable for relative cost comparisons.
More detailed future Lightcraft/conventional rocket designs and cost comparisons are,
of course, needed before a strong argument can be made for either design.
Shown in Table 2 is the estimated performance and weights (masses) for 3-stage
hybrid rocket launch vehicles and single-stage laser-powered launch vehicles that are
capable of placing nanosats of 1.0 kg, 5.0 kg, and 10 kg into LEO. And Table 3 shows
estimated costs for hybrid rockets and laser-powered Lightcraft assuming 100 flights
over a 10-year period. These estimated costs indicate that Lightcraft could boost
nanosats in the 2.0 kg to 5.0 kg range into LEO at about 1/lOth to l/5th the cost of
expendable rockets. But Lightcraft cost superiority over conventional rockets is less
overwhelming for satellites that are significantly heavier. Thus Lightcraft appear
extremely attractive for satellite delivery missions only if Lightcraft dry masses,
including the satellites being carried, are less than about 5.0 kg.
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