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CHM 123-Chapter 2.7
CHM 123-Chapter 2.7

Chemistry (B) HW Chapter 25
Chemistry (B) HW Chapter 25

... a. Products that start a new reaction are released. b. Reactants that have two parts split. c. Products that are radioactive are lost. d. Radioactive reactants are deposited on control rods. ____ 38. Controlled nuclear chain reactions ____. a. take place in nuclear reactors b. are always fusion reac ...
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mass numbers

Problem Set 7 Solutions
Problem Set 7 Solutions

... Can increase fuel utilization, because the lower absorption of sodium compared to water means fewer neutrons are absorbed in the coolant. May decrease fuel utilization, as more of the absorption events happen in the resonance regions of other materials (structural, cladding, etc.) because the neutro ...
Nuclear Chem Notes - Warren County Schools
Nuclear Chem Notes - Warren County Schools

... neutron, it eventually forms the fissionable nuclide of plutonium, Pu-239, which can support a chain reaction. Plutonium is a transuranium element, meaning that it has an atomic number greater than the 92 of uranium. The fissionable plutonium produced in a uranium-fueled reactor can be used as a fue ...
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Nuclear Chemistry

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Radioactivity - Teach Nuclear

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ppt-nuclear - SandersScienceStuff

... left, divide the time passed from the half life and that will give you the amount of half lives your sample has had. You can then divide your original mass of sample by 2 as many times as you have half lives. • If you are trying to solve for the half life of your sample, take the remaining mass and ...
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30.1 Radioactivity The atom is the smallest unit of achemical

... a proton decays into a neutron it has the same charge as electron but negative charge • it has the same mass as electron • it can penetrate with few meters in air. 2 or 3 cm of wood are enough to protect oneself. 3- Gamma decay (γ) ...
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Outline Chapter 8 The Nucleus 8-1. J.J. Thompson`s Plum Pudding

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Atomic/Nuclear

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... and 2 neutrons are combined to form the helium nucleus: E = m c2 = (5·10-29 kg) · (3·108 m/s)2 = 4.5 ·10-12 J = 28 MeV Each of the four nucleons releases 28 MeV / 4 = 7 MeV ...
Energy of a nucleus
Energy of a nucleus

... Fusion in stars • Stars convert hydrogen to helium and heavier elements. When Fe and Ni are reached, fusion stops. The star has burnt its nuclear fuel and collapses under its own gravity. • In massive stars, this collapse releases a huge amount of gravitational energy that leads to a supernova.The ...
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Chapter 25 Nuclear Chemistry

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Fusion or Fission

... plants use fission to produce energy, producing a lot of radioactive byproducts as a result. 4 Conversely, in fusion reactions, the nuclei from atoms with low atomic weights combine to create heavier nuclei. This reaction does not require neutrons in order to occur. Two light nuclei must collide wit ...
< 1 ... 6 7 8 9 10 11 12 13 14 ... 19 >

Nuclear fission product

Nuclear fission products are the atomic fragments left after a large atomic nucleus undergoes nuclear fission. Typically, a large nucleus like that of uranium fissions by splitting into two smaller nuclei, along with a few neutrons, the release of heat energy (kinetic energy of the nuclei), and gamma rays. The two smaller nuclei are the fission products. (See also Fission products (by element)).About 0.2% to 0.4% of fissions are ternary fissions, producing a third light nucleus such as helium-4 (90%) or tritium (7%).The fission products themselves are often unstable and radioactive, due to being relatively neutron-rich for their atomic number, and many of them quickly undergo beta decay. This releases additional energy in the form of beta particles, antineutrinos, and gamma rays. Thus, fission events normally result in beta radiation and antineutrinos, even though these particles are not produced directly by the fission event itself.Many of these isotopes have a very short half-life, and therefore give off huge amounts of radiation. For instance, strontium-90, strontium-89 and strontium-94 are all fission products, they are produced in similar quantities, and each nucleus decays by shooting off one beta particle (electron). But Sr-90 has a 30-year half-life, Sr-89 a 50.5-day half-life, and Sr-94 a 75-second half-life. When freshly created, Sr-89 will spray beta particles 10,600 times faster than Sr-90, and Sr-94 will do so 915 million times faster. It is these short-half-life isotopes that make spent fuel so dangerous, in addition to generating much heat, immediately after the reactor itself has been shut down. The good news is that the most dangerous fade quickly; after 50 days, Sr-94 has had 58,000 half-lives and is therefore 100% gone; Sr-89 is at half its original quantity, but Sr-90 is still 99.99% there. As there are hundreds of different isotopes created, the initial high radiation fades quickly, but never fades out completely.
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