Introduction to the World of Nuclear Physics. Lidiya Strautman

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Название Introduction to the World of Nuclear Physics
Автор произведения Lidiya Strautman
Жанр Физика
Серия
Издательство Физика
Год выпуска 2013
isbn 978-601-04-0249-2



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with an excess of protons or neutrons in comparison with the stable nuclei will decay toward the stable nuclei by changing protons into neutrons or neutrons into protons, or else by shedding neutrons or protons either singly or in combination. Nuclei are also unstable if they are excited, that is, not in their lowest energy states. In this case the nucleus can decay by getting rid of its excess energy without changing Z or N by emitting a gamma ray.

      Nuclear decay processes must satisfy several conservation laws, meaning that the value of the conserved quantity after the decay, taking into account all the decay products, must equal the same quantity evaluated for the nucleus before the decay. Conserved quantities include total energy (including mass), electric charge, linear and angular momentum, number of nucleons, and lepton number (sum of the number of electrons, neutrinos, positrons and antineutrinos – with antiparticles counting as -1).

      137Ba decay data, counting numbers of decays observed in 30-second intervals. The best-fit exponential curve is shown. The points do not fall exactly because of statistical counting fluctuations

      The probability that a particular nucleus will undergo radioactive decay during a fixed length of time does not depend on the age of the nucleus or how it was created. Although the exact lifetime of one particular nucleus cannot be predicted, the mean (or average) lifetime of a sample containing many nuclei of the same isotope can be predicted and measured. A convenient way of determining the lifetime of an isotope is to measure how long it takes for one-half of the nuclei in a sample to decay – this quantity is called the half-life, t(1/2). Of the original nuclei that did not decay, half will decay if we wait another half-life, leaving one-quarter of the original sample after a total time of two half-lives. After three half-lives, one-eighth of the original sample will remain and so on. Measured half-lives vary from tiny fractions of seconds to billions of years, depending on the isotope. The number of nuclei in a sample that will decay in a given interval of time is proportional to the number of nuclei in the sample. This condition leads to radioactive decay showing itself as an exponential process, as shown above. The number N of the original nuclei remaining after a time t from an original sample of N0 nuclei is N = N0e-(t/T)

      where T is the mean lifetime of the parent nuclei. From this relation, it can be shown that t(1/2) = 0.693T.

EXERCISES

      Ex. 1 Make the following sentences negative.

      1. Nuclear radiation occurs in other forms, including the emission of protons or neutrons. 2. The number of nuclei in a sample that will decay in a given interval of time is proportional to the number of nuclei in the sample. 3. This condition leads to radioactive decay showing itself as an exponential process, as shown above. 4. The best-fit exponential curve is shown.

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