Lecture 5
Nuclear Reactions
 

Fission and Fusion Energetics

  • If we split a nucleus of mass A = 230 into two masses of A = 115. From the figure in last frame, BE/Nucleon for A=230 is 7.5MeV and the same for A=115 is 8.4 MeV. Hence the reaction will release energy equal to 0.9 x 230 = 217 MeV.
  • Thus fission process releases a large amount of energy.
  • Similarly if two light elements fuse to become a heavy element, energy would be released as the product nuclei has a higher binding energy than the reactants.
  • Though fusion energy release per reaction is less, but specific energy (energy release per unit
    mass) is high.
  • While the curve indicates possibility of energy release, ways and means have to be found
    to enable the reactions to take place.

Fission Energetics

  • Consider the following equation
  • Binding Energy of Last Neutron is (BELN) 6.6 MeV.
  • Energy necessary to be supplied to induce fission is called Critical Energy for Fission.
  • The critical energy for fission and BELN for some isotopes are summarised in the following table.
Isotope
Critical Energy for Fission (MeV)
Binding Energy of Last Neutron (MeV)
Th233
6.5
5.1
U234
4.6
6.6
U236
5.3
6.4
U239
5.5
4.9
Pu240
4.0
6.4