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AAWSAP DIRD, MHD Air Breathing Propulsion and Power for Aerospace Applications, November 2010

U.S. Department of War · 2010-11-21 · 32 pages · text from the file's own layer

This Defense Intelligence Reference Document, dated 21 November 2010, was prepared by the Defense Intelligence Agency's Defense Warning Office under its Advanced Aerospace Weapons System Applications (AAWSA) Program. It reviews propulsion concepts that use weakly ionized plasmas and magnetohydrodynamics for hypersonic flight and spacecraft. It concludes that the Ajax MHD energy bypass concept is meaningless below Mach 12. A reverse energy bypass with a Virtual Cowl is judged potentially practical, and electric propulsion is expected to become standard for spacecraft.

From the source: Release of 2026-09-18 Incident: 11/21/10, Las Vegas, Nevada. Released with redactions. This document is a Defense Intelligence Reference Document (DIRD), a technical reference format used by the Defense Intelligence Agency (DIA) to capture baseline knowledge on a specific topic for later analytic use. DIRDs are best understood as reference and synthesis products rather than as original research. It is one of 38 DIRDs produced under the Advanced Aerospace Weapon System Applications Program (AAWSAP) between 2009 and 2011. Because AAWSAP’s scope permitted a broad range of supporting topics, not every DIRD in the series directly concerns aerospace systems or future threat assessment. The following summary reflects the DIRD’s scope and framing at the time of writing and should not be read as implying current validation of the concepts discussed. This DIRD surveys magnetohydrodynamic (MHD) and plasma-based concepts for air-breathing propulsion, onboard power generation, and aerodynamic control, arguing that such systems could in principle extend aerospace performance beyond the limits of conventional chemical propulsion and control surfaces. The report reviews concepts including MHD acceleration, flow control, inlet control, onboard power generation, drag reduction, and plasma-generated “virtual” aerodynamic surfaces, while giving particular attention to hypersonic applications such as scramjet power extraction, reentry vehicles, global-strike gliders, and aero-assisted orbital maneuvers. However, it emphasizes major practical constraints, especially extreme power requirements, system weight and complexity, and the difficulty of achieving useful ionization in colder air at lower hypersonic speeds; on that basis, it argues that Ajax-style MHD bypass concepts, in which energy is extracted from the airflow upstream and reintroduced downstream through an electromagnetic system, are not meaningful below about Mach 12, while treating the “virtual cowl” and related reentry applications as more plausible. The document presents plasma and MHD aerospace systems as a technically serious but highly demanding field whose nearer-term promise lies in specialized hypersonic control, power generation, and reentry applications rather than a fully realized air-breathing propulsion system.

UNCLASSIFIED/ /POI\ orr1e1At WSE 8Ptk¥
pressure, Pamb is the ambient/environmental pressure, Pj et is the jet-kinetic
power (thrust power) produced by the engine, and P eiect is the electrical (or other
external source) power supplied to the propulsion system. For air-breathing
systems the mass flow rate of the fuel is very small relative to the mass flow
rate of the air.
Note that an air-breathing system can never fly faster than its exhaust velocity.
Rockets, because they carry an onboard oxidizer, do not have this restriction
and, therefore, have no flight-speed limits. The jet power for high-speed air
breathing engines is larger than the equivalent jet power for a rocket due to the
inlet and is the difference of two large numbers.
Large power levels are required for aircraft and launch vehicles . For example, an
SR-71 cruising at Mach 3.2 produces a thrust of 24,700 lbf (110 kN) and a jet
power of 104 MW. Climb and maneuver thrust is much higher. Similarly, an RL10
rocket eng ine produces 15,000 lbf (66.7 kN) thrust at an l sp of 433 seconds, and
has a jet power of 142 MW. By comparison, a Nimitz class nuclear aircraft carrier
propulsion system is 194 MW, and the Hoover
dam produces about 2000 MW. Therefore, any
electric system replacing these applications must
be capable of processing a lot of power.
Spacecraft propulsion systems are typically
hundreds of watts to tens of kW. This, in addition
to powerplant weight issues, is a primary reason
why electric propulsion systems are currently
being used on spacecraft and not on aircraft.
Historically, electric thrusters for spacecraft were
available for flight decades before the power
systems. 12
Figure 1. Electrothermal Arcjet
Thruster. Photograph of a 30-kW
arcjet thruster being tested at the
Jet Propulsion Laboratory .13
UNCLASSIFIED/f8R 8ffl@lsld:. WSE 8Ptklf
7

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Official release, from the pursue collection. The PDF is mirrored here; the original link is above. 32 pages are in the text index: search them above, or from the library's search.