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A fusion-driven gas core nuclear rocket

dc.contributor.authorKammash, Terry B.en_US
dc.contributor.authorGodfroy, Thomas J.en_US
dc.date.accessioned2011-11-15T16:00:41Z
dc.date.available2011-11-15T16:00:41Z
dc.date.issued1998-01-15en_US
dc.identifier.citationKammash, T.; Godfroy, T. (1998). "A fusion-driven gas core nuclear rocket." AIP Conference Proceedings 420(1): 1377-1384. <http://hdl.handle.net/2027.42/87423>en_US
dc.identifier.otherAPCPCS-420-1en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/87423
dc.description.abstractA magnetic confinement scheme is investigated as a potential propulsion device in which thrust is generated by a propellant heated by radiation emanating from a fusion plasma. The device in question is the gasdynamic mirror (GDM) machine in which a hot dense plasma is confined long enough to generate fusion energy while allowing a certain fraction of its charged particle population to go through one end to a direct converter. The energy of these particles is converted into electric power which is recirculated to sustain the steady state operation of the system. The injected power heats the plasma to thermonuclear temperatures where the resulting fusion energy appears a charged particle power, neutron power, and radiated power in the form of bremsstrahlung and synchrotron radiation. The neutron power can be converted through a thermal converter to electric power that can be combined with the direct converter power before being fed into the injector. The radiated power, on the other hand, can be used to heat a hydrogen propellant introduced into the system at a specified pressure and mass flow rate. This propellant can be pre-heated by regeneratively cooling the (mirror) nozzle or other components of the system if feasible, or by an electrothermal unit powered by portions of the recirculated power. Using a simple heat transfer model that ignores the heat flux to the wall, and assuming total absorption of radiation energy by the propellant it is shown that such a gas core rocket is capable of producing tens of kilonewtons of thrust and several thousands of seconds of specific impulse. It is also shown that the familiar Kelvin-Helmholtz instability which arises from the relative motion of the neutral hydrogen to the ionized fuel is not likely to occur in this system due to the presence of the confining magnetic field. © 1998 American Institute of Physics.en_US
dc.publisherThe American Institute of Physicsen_US
dc.rights© The American Institute of Physicsen_US
dc.titleA fusion-driven gas core nuclear rocketen_US
dc.typeArticleen_US
dc.subject.hlbsecondlevelPhysicsen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Nuclear Engineering and Radiological Sciences, The University of Michigan, Ann Arbor, Michigan 48109en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/87423/2/1377_1.pdf
dc.identifier.doi10.1063/1.54763en_US
dc.identifier.sourceSpace technology and applications international forum - 1998en_US
dc.owningcollnamePhysics, Department of


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