TY - GEN
T1 - Preliminary study of a fuel cell powered magnetoplasma engine with e-beam ionization
AU - Parent, Bernard
AU - Jeung, In Seuck
PY - 2005
Y1 - 2005
N2 - A fuel-cell powered magnetoplasma jet engine (magjet) using electron-beam ionizers is here proposed for airbreathing flight in the supersonic/hypersonic regime. The engine consists of a fuel-cell duct containing the power source and of a high-speed duct producing most of the thrust through a magnetoplasmadynamic (MPD) accelerator. To reduce the shocks and heat loads in the fuel cells, the enthalpy of the air is extracted beforehand through a MPD generator. The power produced by the latter and by the fuel cells is then split optimally between the MPD accelerator located in the high-speed duct and one located downstream of the fuel cells. The performance is assessed through exact solutions of a quasione- dimensional model which includes the effect of ion slip, Joule heating, and heat dissipated through electron-beam ionization. The magnetic field strength as well as the mass flow rate ratio between the high-speed and fuel cell ducts are seen to affect the thrust considerably at lower Mach number, but to have a smaller impact at hypervelocities. Flight beyond Mach 6 would necessitate substantial cooling of the fuel cells due to the ion slip effect preventing sufficient enthalpy extraction, independently of the magnetic field strength. For a fuel cell efficiency of 0.6 and a mass flow rate ratio of 5, the magjet delivers a specific impulse within 15% of the one of the turbojet in the Mach number range 1-3 given a magnetic field of 8 Teslas. From Mach 3 to 5, a magnetic field strength varying between 2 and 4 Teslas is seen to be sufficient to match the performance of conventional engines.
AB - A fuel-cell powered magnetoplasma jet engine (magjet) using electron-beam ionizers is here proposed for airbreathing flight in the supersonic/hypersonic regime. The engine consists of a fuel-cell duct containing the power source and of a high-speed duct producing most of the thrust through a magnetoplasmadynamic (MPD) accelerator. To reduce the shocks and heat loads in the fuel cells, the enthalpy of the air is extracted beforehand through a MPD generator. The power produced by the latter and by the fuel cells is then split optimally between the MPD accelerator located in the high-speed duct and one located downstream of the fuel cells. The performance is assessed through exact solutions of a quasione- dimensional model which includes the effect of ion slip, Joule heating, and heat dissipated through electron-beam ionization. The magnetic field strength as well as the mass flow rate ratio between the high-speed and fuel cell ducts are seen to affect the thrust considerably at lower Mach number, but to have a smaller impact at hypervelocities. Flight beyond Mach 6 would necessitate substantial cooling of the fuel cells due to the ion slip effect preventing sufficient enthalpy extraction, independently of the magnetic field strength. For a fuel cell efficiency of 0.6 and a mass flow rate ratio of 5, the magjet delivers a specific impulse within 15% of the one of the turbojet in the Mach number range 1-3 given a magnetic field of 8 Teslas. From Mach 3 to 5, a magnetic field strength varying between 2 and 4 Teslas is seen to be sufficient to match the performance of conventional engines.
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U2 - 10.2514/6.2005-4924
DO - 10.2514/6.2005-4924
M3 - Conference contribution
AN - SCOPUS:85088722005
SN - 9781624100604
T3 - 36th AIAA Plasmadynamics and Lasers Conference
BT - 36th AIAA Plasmadynamics and Lasers Conference
PB - American Institute of Aeronautics and Astronautics Inc.
T2 - 36th AIAA Plasmadynamics and Lasers Conference
Y2 - 6 June 2005 through 9 June 2005
ER -