n+ 235U → 236U→ "Sr+ 144Xe + 2n (30.5) The 235U nucleus absorbs the neutron to become 236U, but 236U is so unstable that it immediately fragments-in this case into a 90Sr nucleus, a 144Xe nucleus, and two neutrons. The less massive "Sr and 144Xe nuclei are more tightly bound than the original 235U nucleus, so a great deal of energy is released in this reaction. As we’ve seen, nuclei with lower values of Z have relatively smaller numbers of neutrons, meaning there will be neutrons "left over" after the reaction. Equation 30.5 shows some free neutrons among the reaction products, but the two nuclear fragments have "extra" neutrons as well they have too many neutrons and will be unstable. This is generally true for the products of a fission reaction. The fact that the waste products of nuclear fission are radioactive has important consequences for the use of nuclear fission as a source of energy.

Physics for Scientists and Engineers with Modern Physics
10th Edition
ISBN:9781337553292
Author:Raymond A. Serway, John W. Jewett
Publisher:Raymond A. Serway, John W. Jewett
Chapter43: Nuclear Physics
Section: Chapter Questions
Problem 58AP
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How much energy is released in the nuclear reaction as shown? If 1.0 kg of 235U were to undergo this reaction, how much energy would be released?

n+ 235U → 236U→ "Sr+ 144Xe + 2n
(30.5)
The 235U nucleus absorbs the neutron to become 236U, but 236U is so unstable that
it immediately fragments-in this case into a 90Sr nucleus, a 144Xe nucleus, and two
neutrons. The less massive "Sr and 144Xe nuclei are more tightly bound than the
original 235U nucleus, so a great deal of energy is released in this reaction. As we’ve
seen, nuclei with lower values of Z have relatively smaller numbers of neutrons,
meaning there will be neutrons "left over" after the reaction. Equation 30.5 shows
some free neutrons among the reaction products, but the two nuclear fragments have
"extra" neutrons as well they have too many neutrons and will be unstable. This is
generally true for the products of a fission reaction. The fact that the waste products
of nuclear fission are radioactive has important consequences for the use of nuclear
fission as a source of energy.
Transcribed Image Text:n+ 235U → 236U→ "Sr+ 144Xe + 2n (30.5) The 235U nucleus absorbs the neutron to become 236U, but 236U is so unstable that it immediately fragments-in this case into a 90Sr nucleus, a 144Xe nucleus, and two neutrons. The less massive "Sr and 144Xe nuclei are more tightly bound than the original 235U nucleus, so a great deal of energy is released in this reaction. As we’ve seen, nuclei with lower values of Z have relatively smaller numbers of neutrons, meaning there will be neutrons "left over" after the reaction. Equation 30.5 shows some free neutrons among the reaction products, but the two nuclear fragments have "extra" neutrons as well they have too many neutrons and will be unstable. This is generally true for the products of a fission reaction. The fact that the waste products of nuclear fission are radioactive has important consequences for the use of nuclear fission as a source of energy.
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