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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…
UNCLASSIFIED/ ,,roAt OFFIQI.Ctk WliEii ·••LY
propulsion requires a modest 0.1 to 10 MW of total beam power. The ground-based
megawatt-class laser beam generator is state-of-the-art technology. The cost of
generating electrical power for the ground-based laser beam generator is ~ $0.10/kWh,
which translates to< $2/kg of payload. An SDIO study [10, 11] showed that all launch
to orbit conditions for a Lightcraft could be satisfied by a single, high-power ground-
based laser - with or without the aid of a low altitude laser relay mirror or space-based
laser beam generator system. The majority of the system mass required to launch a
payload to orbit is left on the ground in the form of the beam generators and their
electrical power sources. The dry spacecraft mass can be further reduced by two
orders of magnitude, and thus the operating costs reduced by a factor of 10 (to <
$2/kg of payload), if Buckytubes are used to construct the vehicle and its subsystems.
LIGHTCRAFT NANOSATELLITE CONFIGURATION
As shown in Figure 7, the Lightcraft nanosat configuration consists of: 1) a conically
shaped "forebody" for lift and aerodynamic compression of ingested airflow (prior to its
detonation by laser heating during atmospheric flight); 2) an annular "cowl" or "shroud"
within which air detonation or propellant ablation (by intense laser heating) occurs; and
3) a parabola-shaped "afterbody" whose mirrored surface focuses beamed laser energy
into regions of sufficient smallness for intense air or propellant heating to occur. And as
shown in Figure 8, the vehicle is powered by laser airbreathing propulsion (by
detonation of air) until hypersonic speed within the sensible atmosphere is reached;
and then the vehicle is powered by laser rocket propulsion (by heating of propellant)
during flight above the sensible atmosphere, until cut-off velocity for orbital flight is
reached.
Shroud (Cowl):
within which Laser
Heating of Airflow
and Propellant
Occurs
I
IForebody: for Lift
and Compression
of Airflow during
Atmospheric Flight
Figure 7. Lightcraft Concept [261.
18
---
• Laser Airbreathing Flight
from Zero Velocity to
Hypersonic Speed
--- --- ---
Afterbody: with
Mirrored Surface
for Focusing Laser
Energy into the
Shroud (Cowl) Laser
Beam
·----------- j\ --------- -
\Axi-Symmetric Body
• Laser Rocket Flight from
Hypersonic to Orbital
Speed
UNCLASSIFIED/ /f81il 8ffl@Itltt ""I! one I

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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.