Radioisotope rocket: Difference between revisions

A '''radioisotope rocket''' or '''radioisotope thermal rocket''' is a type of [[Thermal rocket|thermal]] [[rocket engine]] that uses the heat generated by the decay of [[radioactive]] elements to heat a [[working fluid]], which is then exhausted through a rocket nozzle to produce [[thrust]]. They are similar in nature to [[Nuclear thermal rocket|nuclear thermal rockets]] such as [[NERVA]], but are considerably simpler and often have no moving parts. Alternatively, radioisotopes may be used in a '''radioisotope electric rocket''',<ref>{{cite journal |last1=Schmidt |first1=George R. |last2=Manzella |first2=David H. |last3=Kamhawi |first3=Hani |last4=Kremic |first4=Tibor |last5=Oleson |first5=Steven R. |last6=Dankanich |first6=John W. |last7=Dudzinski |first7=Leonard A. |title=Radioisotope electric propulsion (REP): A near-term approach to nuclear propulsion |journal=Acta Astronautica |date=1 February 2010 |volume=66 |issue=3 |pages=501–507 |doi=10.1016/j.actaastro.2009.07.006 |bibcode=2010AcAau..66..501S |hdl=2060/20110016114 |hdl-access=free }}</ref> in which energy from nuclear decay is used to generate the electricity used to power an [[Electrically poweredSpacecraft spacecraftelectric propulsion|electric propulsion system]].

The basic idea is a development of existing [[radioisotope thermoelectric generator]], or RTG, systems, in which the heat generated by decaying nuclear fuel is used to generate power. In the rocket application the generator is removed, and the working fluid is instead used to produce thrust directly. Temperatures of about {{cvt|1500 |to |2000&nbsp;°|C|F|-2}} are possible in this system, allowing for [[specific impulse]]s of about 700 to 800 &nbsp;seconds (7 to 8&nbsp;kN·s/kg), about double that of the best chemical engines such as the [[LH2]]-[[LOX]] [[Space Shuttle Main Engine]].

However the amount of power generated by such systems is typically fairly low. Whereas the full "active" reactor system in a [[nuclear thermal rocket]] can be expected to generate over a gigawatt, a radioisotope generator might get 5&nbsp;kW. This means that the design, while highly efficient, can produce thrust levels of perhaps {{cvt|1.3 |to |1.5&nbsp;|N|lbf}}, making them useful only for thrusters. In order to increase the power for medium-duration missions, engines would typically use fuels with a short [[half-life]] such as [[polonium|Po-210]], as opposed to the typical RTG which would use a long half-life fuel such as [[plutonium-238]] in order to produce more constant power over longer periods of time. The even shorter half-life element [[fermium]] has also been suggested.<ref>[http://pdf.aiaa.org/preview/CDReadyMSPACE06_1393/PV2006_7272.pdf AIAA meeting paper comparing fermium, polonium and plutonium as power sources]{{dead link|date=November 2017 |bot=InternetArchiveBot |fix-attempted=yes }}</ref>

[[TRW Inc.|TRW]] maintained a fairly active development program known as '''Poodle''' from 1961 to 1965, and today the systems are still often known as '''Poodle thrusters'''. The name was a play on the larger systems being developed under [[Project Rover]], which led to NERVA. In April 1965 they ran their testbed engine for 65 &nbsp;hours at about {{cvt|1500&nbsp;°|C|F|-2}}, producing a specific impulse of 650 to 700 &nbsp;seconds (6.5 to 7&nbsp;kN·s/kg).

==Photon Pressurepressure==

{{see also|nuclearNuclear photonic rocket}}