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Friday, March 22, 2019

Fission Or Fusion :: essays research papers

Fission or Fusion     I think that right now, fission is the only way that we can get more brawn come on of a atomic reaction than we put in. First, the elan vital per fissionis genuinely large. In practical units, the fission of 1 kg (2.2 lb) of atomic number 92-235releases 18.7 million kilowatt-hours as heat. Second, the fission processinitiated by the absorption of one neutron in atomic number 92-235 releases about(predicate) 2.5neutrons, on the average, from the split nuclei. The neutrons released in thismanner quickly cause the fission of two more atoms, thereby releasing four ormore additional neutrons and initiating a self-sustaining series of nuclearfissions, or a chain reaction, which results in continuous release of nuclearenergy. Naturally occurring uranium contains only 0.71 percent uranium-235 theremainder is the non-fissile isotope uranium-238. A mass of natural uranium byitself, no matter how large, cannot sustain a chain reaction because only theuranium-235 is easily fissionable. The probability that a fission neutron withan initial energy of about 1 MeV will induce fission is rather low, however can beincreased by a factor of hundreds when the neutron is slowed bring through aseries of elastic collisions with light nuclei much(prenominal) as hydrogen, deuterium, orcarbon. This fact is the basis for the design of practical energy-producingfission reactors.     In December 1942 at the University of Chicago, the Italian physicistEnrico Fermi succeeded in producing the first nuclear chain reaction. This wasdone with an arrangement of natural uranium lumps distributed within a largestack of pure graphite, a form of carbon. In Fermis "pile," or nuclear reactor,the graphite moderator served to slow the neutrons.     Nuclear fusion was first achieved on earth in the early 1930s bybombarding a prey containing deuterium, the mass-2 isotope of hydrogen, withhigh-energy deute rons in a cyclotron. To accelerate the deuteron beam a coarsedeal of energy is required, most of which appeared as heat in the target. As aresult, no net useful energy was produced. In the mid-fifties the first large-scalebut uncontrolled release of fusion energy was demonstrated in the tests ofthermonuclear weapons by the United States, the USSR, Great Britain, and France.This was such a brief and uncontrolled release that it could not be utilize for theproduction of voltaic power.     In the fission reactions I discussed earlier, the neutron, which has noelectric charge, can easily approach and react with a fissionable core ,forexample, uranium-235. In the typical fusion reaction, however, the reactingnuclei both have a corroboratory electric charge, and the natural repulsion betweenthem, called Coulomb repulsion, must be overcome before they can join.

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