Thermal to optical energy conversion: A multi megawatt carbon dioxide laser driven by an extremely high temperature gas cooled reactor

In the conversion of ionizing radiation into energy, the production of heat is the most common first step in energy conversion systems, but it is also possible to use ions and excited states as the first step. The difference being that nearly all of the energy content of ionizing radiation is conver...

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Veröffentlicht in:Progress in nuclear energy (New series) 2018-08, Vol.107, p.155-171
Hauptverfasser: Prelas, Mark A., White, Nathan E., Wisniewski, Denis A., Walton, Kyle L., Tchouaso, Modeste Tchakoua, Boraas, Matthew A., Aguilar, Fernando De La Torre, Kasiwattanawut, Haruetai, Knewtson, Tyler B., Schutte, Jenny R., Watermann, Matthew L.
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container_end_page 171
container_issue
container_start_page 155
container_title Progress in nuclear energy (New series)
container_volume 107
creator Prelas, Mark A.
White, Nathan E.
Wisniewski, Denis A.
Walton, Kyle L.
Tchouaso, Modeste Tchakoua
Boraas, Matthew A.
Aguilar, Fernando De La Torre
Kasiwattanawut, Haruetai
Knewtson, Tyler B.
Schutte, Jenny R.
Watermann, Matthew L.
description In the conversion of ionizing radiation into energy, the production of heat is the most common first step in energy conversion systems, but it is also possible to use ions and excited states as the first step. The difference being that nearly all of the energy content of ionizing radiation is converted to heat but only 40–50% of the energy content of ionizing radiation is converted into ions and excited states. Conversion of the energy contained in ionizing radiation into ions and excited states starts out at a considerable disadvantage. Nuclear-pumped lasers have typically depended on the conversion of ionizing radiation into ions and excited states as a first step. Among the reasons that nuclear-pumped lasers have had low system efficiencies (1–2.5%) is the considerable inefficiencies in producing ions and excited states from ionizing radiation. A nuclear-pumped laser system which uses heat produced from the energy content of ionizing radiation as the driver for the laser system is described in this paper. The conversion of heat into vibrational states in molecular nitrogen allows energy to be stored in a long lived molecular state which can then be transported spatially where its energy is collisionally conveyed to carbon dioxide molecules in a resonance transfer process to produce the carbon dioxide upper laser level. The carbon dioxide laser emits a laser beam with a wavelength centered at 10.4 μm. The nitrogen vibrational state and its resonance conversion into the carbon dioxide upper laser level is one of nature's most efficient processes in laser physics (with laser efficiencies approaching ∼20% primarily being driven by the resonance process-extremely high for a laser). The laser system described here takes advantage of this highly efficient mechanism for conversion of thermal energy to optical energy. The feasibility of using nuclear rocket core technology for the generation of high temperature gas flows to power this thermal to optical conversion process is described. This study indicates that the thermal to optical conversion process can lead to a carbon dioxide laser with efficiencies on the order of 7% or perhaps better. Such a system would have potential applications in power beaming, space propulsion, asteroid mining, asteroid deflection and potential military applications. •Conversion of thermal energy from a reactor to optical energy.•Extremely high temperature gas cooled reactor.•Thermally pumped carbon dioxide laser.•Three energy carbo
doi_str_mv 10.1016/j.pnucene.2018.04.008
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The difference being that nearly all of the energy content of ionizing radiation is converted to heat but only 40–50% of the energy content of ionizing radiation is converted into ions and excited states. Conversion of the energy contained in ionizing radiation into ions and excited states starts out at a considerable disadvantage. Nuclear-pumped lasers have typically depended on the conversion of ionizing radiation into ions and excited states as a first step. Among the reasons that nuclear-pumped lasers have had low system efficiencies (1–2.5%) is the considerable inefficiencies in producing ions and excited states from ionizing radiation. A nuclear-pumped laser system which uses heat produced from the energy content of ionizing radiation as the driver for the laser system is described in this paper. 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This study indicates that the thermal to optical conversion process can lead to a carbon dioxide laser with efficiencies on the order of 7% or perhaps better. Such a system would have potential applications in power beaming, space propulsion, asteroid mining, asteroid deflection and potential military applications. •Conversion of thermal energy from a reactor to optical energy.•Extremely high temperature gas cooled reactor.•Thermally pumped carbon dioxide laser.•Three energy carbon dioxide laser model.•Predicted system efficiency for the carbon dioxide laser of 6.7%.</abstract><cop>Oxford</cop><pub>Elsevier Ltd</pub><doi>10.1016/j.pnucene.2018.04.008</doi><tpages>17</tpages><orcidid>https://orcid.org/0000-0003-2588-2364</orcidid><orcidid>https://orcid.org/0000-0002-6507-0689</orcidid></addata></record>
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ispartof Progress in nuclear energy (New series), 2018-08, Vol.107, p.155-171
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source Elsevier ScienceDirect Journals
subjects Asteroid deflection
Asteroid mining
Carbon dioxide
Carbon dioxide laser
Carbon dioxide lasers
Energy conversion
Extremely high temperature reactor
Fusion
High temperature gas cooled reactors
High temperature gases
Ionizing radiation
Laser beams
Laser cooling
MCNP
Military applications
Nitrogen cooled pebble graphite reactor
Nuclear energy
Nuclear pumped laser
Nuclear reactors
Power beaming
Propulsion systems
Radiation
Thermal energy
Vibrational states
title Thermal to optical energy conversion: A multi megawatt carbon dioxide laser driven by an extremely high temperature gas cooled reactor
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