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Hydrogen bomb
Dátum pridania: | 13.01.2002 | Oznámkuj: | 12345 |
Autor referátu: | exar | ||
Jazyk: | Počet slov: | 688 | |
Referát vhodný pre: | Stredná odborná škola | Počet A4: | 2.3 |
Priemerná známka: | 2.97 | Rýchle čítanie: | 3m 50s |
Pomalé čítanie: | 5m 45s |
Enough neutrons are produced in the fusion reactions to produce further fission in the core and to initiate fission in the tamper.
Since the fusion reaction produces mostly neutrons and very little that is radioactive, the concept of a "clean bomb has resulted: one having a small atomic trigger, a less fissionable tamper, and therefore less radioactive fallout. Carrying this progression further would result in the suggested neutron bomb, which would have a minimum trigger and a nonfissionable tamper; there would be blast effects and a hail of lethal neutrons but almost no radioactive fallout; this theoretically would cause minimal physical damage to buildings and equipment but kill most living things. The theorized cobalt bomb is, on the contrary, a radioactively "dirty bomb having a cobalt tamper. Instead of generating additional explosive force from fission of the uranium, the cobalt is transmuted into cobalt-60, which has a half-life of 5.26 years and produces energetic (and thus penetrating) gamma rays. The half-life of Co-60 is just long enough so that airborne particles will settle and coat the earth's surface before significant decay has occurred, thus making it impractical to hide in shelters. This prompted physicist Leo Szilard to call it a "doomsday device since it was capable of wiping out life on earth.
Like other types of nuclear explosion, the explosion of a hydrogen bomb creates an extremely hot zone near its center. In this zone, because of the high temperature, nearly all of the matter present is vaporized to form a gas at extremely high pressure. A sudden overpressure, i.e., a pressure far in excess of atmospheric pressure, propagates away from the center of the explosion as a shock wave, decreasing in strength as it travels. It is this wave, containing most of the energy released, that is responsible for the major part of the destructive mechanical effects of a nuclear explosion. The details of shock wave propagation and its effects vary depending on whether the burst is in the air, underwater, or underground.
R. Rhodes, Dark Sun: The Making of the Hydrogen Bomb (1995).