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Poor man's nuclear energy? |
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| Jan25-09, 10:13 AM | #18 |
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Poor man's nuclear energy? |
| Jan25-09, 12:27 PM | #19 |
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It's a pretty OBVIOUS thing to do. Additionally, Pu-238 production doesn't give one the recipe for a bomb. One needs fissile Pu-239 for a nuclear weapon - not radioactive Pu-238. In fact, Pu-238 is something you want to LEAVE OUT OF a nuclear weapon - the Pu-238 doesn't help in the fission reaction - and its radioactivity and heat just complicate matters. Dr. Gregory Greenman Physicist |
| Jan25-09, 12:48 PM | #20 |
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| Jan25-09, 03:13 PM | #21 |
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Actually, Pu-238 IS fissile. At room temperature 0.025 eV; Pu-238 has a (n,fission) microscopic cross section of about 15 barns. That is in comparison to about 700 - 800 barns for Pu-239. So Pu-238 is fissile - but it isn't going to help much - and the negatives are overwhelming. A nuclide can't be not "fissile" in a thermal spectrum but fissile in a fast spectrum- by definition. The word "fissile" means that the nuclide will fission with thermal neutrons. If a nuclide like U-238 that will only fission with neutrons of energy above a certain threshold - like with fast neutrons - those nuclides are termed "fissionable". U-238 is NOT "fissile" - but it is "fissionable". Dr. Gregory Greenman Physicist |
| Jan26-09, 03:07 AM | #22 |
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I just wanted to point out that a big enough lump of Pu-238 will undergo just as well a fast power excursion (if you see what I mean) as a big enough lump of Pu-239, as its k_inf value is far above 1. (which is not the case for U-238 btw). |
| Jan26-09, 08:21 AM | #23 |
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For high energy neutrons, the fission cross-sections for Pu-238 and Pu-239 are quite comparable. The problem is that you are not going to be able to get the Pu-238 to the same densities that one can with Pu-239. The problem with looking at just k-infinity is that infinite sized devices are really tough to transport to the target. Dr. Gregory Greenman Physicist |
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