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/ /1"91t 91'fll!lit.l! l!llili ,nu,,,
plasma, creating downward thrust expansion. Multiple laser pulses and an atmospheric
refresh of breakdown air generate the flight. This airbreathing pulsed-detonation
engine concept owes its origins to the German V-1 "Buzz Bomb" of WW II which ran on
aviation fuel.
For the purpose of this report, we envision a Lightcraft Earth-to-Orbit (ETD)
transportation system that operates according to the following scenario. The
airbreathing engine mode develops quasi-steady thrust by pulsing at a variable rate
that depends on the Mach number and altitude flown along the flight trajectory to orbit.
Once the Lightcraft reaches very high altitude and 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 ground-based laser beam generator
system consists of the following: 1) power supply; 2) high-power (megawatt-class)
laser beam generator/transmitter using novel beam optics; and 3) automated tracking,
hand-off and safety systems.
HISTORY OF THE LIGHTCRAFT TECHNOLOGY DEMONSTRATION
PROGRAM
The laser Lightcraft project originally grew out of the Lightcraft Technology
Demonstration Program funded by the Strategic Defense Initiative Organization (SDID)
Laser Propulsion Program in the late 1980's. In the 1990's, a joint program involving
the NASA-Marshall Space Flight Center and the Propulsion Sciences and Advanced
Concepts Division of the AFRL Propulsion Directorate developed and tested an
experiment to determine the feasibility of using high-power pulsed lasers to launch a
spacecraft into orbit. Successful tests at the White Sands Missile Range (WSMR) High
Energy Laser Systems Test Facility (HELSTF) demonstrated the first passively controlled
vertical free flight of an object that was propelled by the U.S. Army's 10 kW Pulsed
Laser Vulnerability Test System (PLVTS) infrared CO2 laser. Laser boost capability was
demonstrated at the HELSTF with a Lightcraft reaching 43 m vertically in 2-second
gyroscopically stabilized free flights, which was followed by horizontal guide-wire flights
of 121.9 m lasting 10 to 20 seconds (see Figure 2 through Figure 6). A subsequent
series of test flights achieved an altitude of 38. 7 m. L. Myrabo (private communication,
Rensselaer Polytechnic Inst., Troy, NY, 2009) recently reported vertical Lightcraft test
flights achieving 68 m altitude.
This achievement can be compared to the first successful flights of Robert Goddard's
liquid propellant chemical rocket, which attained a height of 12.5 m after a 2.5 second
burn in March 1926. In sharp contrast with Goddard's rockets, there is absolutely no
fuel on board the prototype Lightcraft, which has a diameter of 10 cm, mass of 20 to 40
g, and is machined from a solid block of 6061-T6 aluminum. Five different Lightcraft
designs have been flight-tested using the pointing and tracking system on the PLVTS
laser. Current Lightcraft designs are limited to about 60 g mass and 15 cm in diameter
by the PLVTS laser. A megawatt-class laser will be necessary for a larger kilo-class
Lightcraft to reach orbit and components for these lasers exist, which would
demonstrate the feasibility of this technology for low cost access to space.
13
UNCLASSIFIED/ /P81il 8PPI@Itlit 1!181!!! e,•t\f

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.