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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 1: Nanosatellite Technologies
OVERVIEW
Nanosats require technologies that radically reduce the mass and power of components
without compromising performance. In addition to miniaturizing components, methods
to integrate similar functions across subsystems are being evaluated. For example, all
subsystem electronics, including instruments, could be integrated within the Command
and Data Handling (C&DH) subsystem. Multifunctional solutions also offer significant
savings over traditional approaches. Technology investments are required to develop
or adapt components to accommodate the expected radiation environment. Simple,
effective methods of thermal control are essential to keep the nanosat operational
during extreme temperature variations. Autonomy is a critical technology that impacts
every subsystem. Constellations with tens to thousands of nanosats must be highly
autonomous to be practical. The nanosat ground system must be kept inexpensive,
simple, and made inter-operable with other missions.
PROPULSION
In the baseline mission, nanosat propulsion is needed for two distinct functions: 1) each
nanosat must raise its orbit apogee to the appropriate radius, 2) and it must reorient
the axis of the spinning nanosat from the velocity direction (within the orbit plane) to
its science mission attitude (perpendicular to the ecliptic plane). These maneuvers
present challenging velocity change (11v) and attitude-control (ACS) requirements.
Requirements for the /'iv Thruster:
• Total impulse: 3,000 to 7,000 N-sec.
• Thrust: 445 N maximum.
• Input power (during burn): < 1 watt.
• Specific impulse: 280 seconds.
Requirements for the ACS Thruster:
• Total impulse: s 2.4 N-sec.
• Minimum impulse bit: 0.044 N-sec.
• Response time: < 0.005 sec.
• Pulse rate: 1 Hz.
It turns out that the 11v and ACS thrusters can have independent systems. We propose
a new innovation whereby the nanosat launch vehicle propulsion system also serves
double duty as the 11v thruster system, and this can be done without having to carry the
propulsion energy source into orbit. This can only be achieved via laser propulsion in
which the laser beam energy that is used to launch a nanosat into orbit is also used to
provide '3.v thrust in orbit. This novel innovation dramatically reduces the mass, size,
cost, and complexity of nanosats because they will only need to carry minimal onboard
ACS thrusters and propellant to carry out routine, minor attitude adjustments. The
innovative nanosat laser propulsion concept is presented in Chapter 2.
3
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