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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.

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and in devices such as t he gliding arc, the plasma evolves from near-equilibrium
to highly nonequilibrium during each of the periodically repeating cycles. In
shock and boundary layers during reentry, the plasma is near therma l
equ ilibrium while being diffuse. The primary reason for this behavior is that the
ionizat ion in those shock and boundary layers exists without any electric field
and thus is not subject to arcing instabilities.
Plasma Features
What feat ures or properties make weakly ionized plasmas interesting for
propu lsion and aerodynam ic applications? The most obvious feature is heating - a
consequence of Joule dissipation in an electrically conducting medium placed in
an electric field. As a heating element, plasma has important advantages
compared with conventional heaters. For example, even a surface electric
discharge can effectively heat t he gas flow much farther from the wall than a
wall-imbedded convent ional heater would. Microwave and laser beams can
create plasmas and heat the gas even far from any surfaces, and the volume and
shape of the heated region can, in principle, be adjusted. Since heated regions
can significantly alter the flow by making the gas flow mostly around them,
plasmas can form switchable, controllable, and tunable virtual bodies or
surfaces. Such virtua l surfaces can be deployed on demand for drag reduction,
aerodynamic control (when app lied asymmetrically), and optimization of engine
inlet performance, to name a few. It is the localized and transient deployment of
plasma virtual surfaces that results in the most interesting and complex
interactions with gas flows while saving energy compared with large -volume,
steady-state plasma utilization, and thus is especially promising for applications.
Another useful application of plasma heating is ignit ion . This may seem trivial;
after all, spark plugs in conventional internal combustion engines are well
developed thermal plasma devices . However, therma l plasma ignition for
scramjet eng ines is not that simple, since the ign it ion system would have to
prevent the plasma from being easily blown away by the supersonic flow, and
even if this problem is resolved, if not properly (and qu ite ingeni ously) designed,
the igniter would cause an unacceptably strong perturbation to the flow and loss
of the stagnation pressure and wou ld require extremely high power. As an
example, plasma igniters based on subcritical microwave discharges are quite
sophisticated .
Besides heating, the presence of charged particles is another obvious, and very
important, feature of plasmas. Charged particles can be act ed upon by electric
and magnetic fields, and this action can be transferred to the bu lk gas by ion
molecule collisions. Thus, magnetohydrodynamic (MHD) and
electrohydrodynamic (EHD) interactions can be ut ilized to exert forces and to
decelerate or accelerate the gas in both inviscid core flows and viscous boundary
layers. The magnitude of such interactions depends on the ionization fraction and
the magnetic or electric field strength.
MHD Interactions
The ionization fraction can be quite high in shock and boundary layers at very
high Mach numbers (such as those in reentry flight), or just downstream of
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