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If we split a nucleus into two smaller nuclei, with a release of energy, has the average binding energy per nucleon increased or decreased?

Short Answer

Expert verified

The binding energy per nucleon for smaller nuclei increases due to the split of the nucleus.

Step by step solution

01

Binding energy per Nucleon

The sum of the protons and neutrons in the nucleus is called the nucleons, and it is the same as the mass number of the atom. The energy required to separate each nucleon from the nuclear force of the nucleus is called the binding energy per nucleon. The binding energy per nucleon for an atom is given as:

Ebp=EbA

Here, Ebpis the binding energy per nucleon, Eb is the binding energy, and A is the mass number of atoms.

02

Whether average binding energy per nucleon of smaller nuclei increased or decreased

The repulsive force between protons in smaller nuclei becomes less due to the reduced number of protons. In contrast, the nuclear force remains the same, so the overall nuclear force increases and smaller nuclei become more stable than large nuclei. As the nuclear force for smaller nuclei increases, more energy is required to separate the nucleons of smaller nuclei, and binding energy per nucleon for smaller nuclei increases.

We can also see from the formula of binding energy per nucleon that binding energy per nucleon varies inversely with the mass number of nuclei. The mass number of smaller nuclei is small, so the binding energy per nucleon of smaller nuclei becomes more than heavier nuclei.

Therefore, the binding energy per nucleon for smaller nuclei increases due to the split of the nucleus

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Most popular questions from this chapter

A thermal neutron (with approximately zero kinetic energy) is absorbed by a238Unucleus. How much energy is transferred from mass-energy to the resulting oscillation of the nucleus? Here are some atomic masses and neutron mass.

U237237.048723uU237238.050782uU237239.054287uU237240.056585un1.008664u

Question: In a particular fission event in which U235is fissioned by slow neutrons, no neutron is emitted and one of the primary fission fragments is Ge83. (a) What is the other fragment? The disintegration energy is Q = 170 MeV. How much of this energy goes to (b) the Ge83fragment and (c) the other fragment? Just after the fission, what is the speed of (d) the Ge83fragment and (e) the other fragment?

Roughly 0.0150% of the mass of ordinary water is due to โ€œheavy water,โ€ in which one of the two hydrogens in anH2O molecule is replaced with deuterium,H2 . How much average fusion power could be obtained if we โ€œburnedโ€ all theH2 in 1.00 litre of water in 1.00 day by somehow causing the deuterium to fuse via the reactionH2+H2โ†’H3e+n ?

What is the Qof the following fusion process?

12H+11Hโ†’23He+photon

Here are some atomic masses.

12H2.014102u11H1.007825u

The isotope 235Udecays by alpha emission with a half-life of 7ร—108y. It also decays (rarely) by spontaneous fission, and if the alpha decay did not occur, its half-life due to spontaneous fission alone would be 3ร—1017y.

(a) At what rate do spontaneous fission decays occur in 1.0 g of235U ?

(b) How many 235U alpha-decay events are there for every spontaneous fission event?

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