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Nuclear Fission - Practice Questions & MCQ

Edited By admin | Updated on Sep 18, 2023 18:34 AM | #JEE Main

Quick Facts

  • Nuclear fission is considered one the most difficult concept.

  • 9 Questions around this concept.

Solve by difficulty

In the nuclear fussion reaction, _{1}^{2}H+_{1}^{3}H\rightarrow _{2}^{4}He+n it is given that the repulsive potential energy between the two nuclei is \sim 7.7\times 10^{-14}J, then the temperature at which the gases must be heated to initiate the reaction is nearly

[ Boltzmann's constant  k=1.38\times 10^{-23}J/K]

To generate power of 3.2 MW, the number of fissions of { }^{235} \mathrm{U} per minute (Energy \, \, released \, per\, fission=200$ $\left.\mathrm{MeV}, 1 \mathrm{eV}=1.6 \times 10^{-19} \mathrm{~J}\right)

If 200 \, \mathrm{MeV} energy is released in the fission of a single \mathrm{U^{235}} nucleus, the number of fissions required per second to produce 1 kilowatt power shall be (Given \mathrm{1 \mathrm{eV}=1.6 \times 10^{-19} \mathrm{~J}})

Energy released in the fission of a single \mathrm{{ }_{92} U^{235}} nucleus is \mathrm{200 \, \mathrm{MeV}}. The fission rate of a \mathrm{{ }_{92} U^{235}} fuelled reactor operating at a power level of \mathrm{5 \mathrm{~W}} is

The number of neutrons released when \mathrm{{ }_{92} U^{235}} undergoes fission by absorbing \mathrm{{ }_0 n^1} and \mathrm{\left({ }_{56} B a^{144}+{ }_{36} K r^{89}\right)} are formed, is

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If the energy released in the fission of one nucleus is 200 MeV. Then the number of nuclei required per second in a power plant of 16 kW will be

To generate a power of 3.2 mega watt, the number of fissions of \mathrm{U^{235}} per minute is
(Energy released per fission \mathrm{=200 \, \mathrm{MeV}, 1 \mathrm{eV}=1.6 \times 10^{-19} \mathrm{~J}})

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The energy liberated on complete fission of 1 \mathrm{~kg} of \mathrm{{ }_{92} U^{235}} is (Assume \mathrm{200 \, \mathrm{MeV}} energy is liberated on fission of 1 nucleus)

Concepts Covered - 1

Nuclear fission

Nuclear fission-

The process of splitting of a heavy nucleus into two lighter nuclie of a comparable masses (after bombardment with energetic particle) with liberation of energy.

For example, on bombarding a uranium target, the nucleus broke into two nearly equal fragments and released a great amount of energy - 

                                                                  ^{1}_{0} \mathrm{n}+^{235}_{92} \mathrm{U} \rightarrow^{236}_{_{92}} \mathrm{U} \rightarrow^{144}_{56} \mathrm{Ba}+^{89}_{36} \mathrm{Kr}+3^{1}_{0} \mathrm{n}

Fission does not always produce Barium and Krypton. Here is another example:

                                                                 ^1_0 \mathrm{n}+^{235}_{92} \mathrm{U} \rightarrow^{236}_{92} \mathrm{U} \rightarrow^{133}_{51} \mathrm{Sb}+^{99}_{41} \mathrm{Nb}+4^{1}_{0} \mathrm{n}

All the fragmented nuclei produced in fission are neutron-rich and unstable. Also, they are radioactive and emit beta articles until they reach a stable end-product. So under favourable conditions, the neutron produced can cause further fission of other nuclie, producing large number of neutrons, Thus a chain of nuclear fissions is established which continues untill the whole Uranium is consumed. 

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Nuclear fission

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