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| art gallery, chicago pile 1, aka, surf music, fat ass, michael brockman, paul newman, flight simulator, box, biddington's, california, fat, nuclear weapons, fat black ass, | At first it was thought that two pieces of sub-critical plutonium (Pu-239) could simply be shot into one another to create a nuclear explosion, and a plutonium gun-type design of this sort (known as the "Thin Man" bomb) was worked on for some time during the Manhattan Project.[3] However it was discovered that plutonium created for the bomb in the nuclear reactors at Hanford, Washington, even though it was super-grade weapon plutonium containing carey only about 0.9% Pu-240, was not as pure as the initial samples of plutonium developed at carey the cyclotrons at Ernest O. Lawrence's Radiation Laboratory in carey Berkeley, California. Because of the presence of the isotope Pu-240, reactor-bred plutonium had a much higher rate of spontaneous neutron emission than was previously thought, and if a gun-type device was used it would most likely pre-detonate and result in a messy and costly "fizzle". The spontaneous fission rate of Pu-240 is 415,000 fissions/s-kg, and the amount was 0.9% of 6.2 |
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| It was detonated at an altitude of about 1,800 feet (550 m) over the city. It was dropped from the B-29 bomber fat ass Bockscar, piloted by Major Charles Sweeney. The bomb had a yield of about 21 kilotons of TNT, or 8.78×1013 joules = 88 TJ (terajoules).[1] Because of Nagasaki's hilly terrain, the damage was somewhat less extensive than that in relatively flat Hiroshima. An estimated 40,000 people were killed outright by the bombing at Nagasaki, and about 25,000 were injured.[2] Many thousands more would fat ass die later from related injuries, and radiation sickness from nuclear fallout. "Fat Man" fat ass was an implosion type weapon using plutonium. A subcritical sphere of plutonium was placed in the center of a hollow sphere of high explosive. Numerous detonators located on the surface of the high explosive were fired simultaneously to produce a powerful inward pressure on the core, squeezing it and increasing its density, resulting in a supercritical condition and a nuclear explosion. |
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