Total binding energy of reactants = Binding energy of ${}^{235}_{92}\text{U}$ = 1800 MeV Total binding energy of products = Binding energy of ${}^{144}_{56}\text{Ba}$ + ${}^{89}_{36}\text{Kr}$ \[ = 1200 + 780 = 1980 \text{ MeV} \] The increase in binding energy (i.e., energy released) = \[ 1980 - 1800 = 180 \text{ MeV} \] This energy is carried away by 3 fast neutrons, so average energy per neutron: \[ \frac{180}{3} = 60 \text{ MeV} \] Thus, the average kinetic energy carried by each fast neutron is 60 MeV.
In a nuclear fission reaction, the total energy released is the difference between the initial and final total binding energies. The total initial binding energy is the binding energy of the \( ^{235}_{92}U \) nucleus, which is 1800 MeV. The total final binding energy is the sum of the binding energies of the fission products \( ^{144}_{56}Ba \) and \( ^{89}_{36}Kr \), which are 1200 MeV and 780 MeV, respectively. The energy released in the fission process is the difference between the initial and final binding energies: \[ \text{Energy released} = \text{Initial binding energy} - \text{Final binding energy} \] \[ \text{Energy released} = 1800 \, \text{MeV} - (1200 \, \text{MeV} + 780 \, \text{MeV}) = 1800 \, \text{MeV} - 1980 \, \text{MeV} = 180 \, \text{MeV}. \] This energy is carried away by the fast neutrons. Since 3 neutrons are emitted in the reaction, the average kinetic energy carried by each fast neutron is: \[ \text{Average kinetic energy per neutron} = \frac{180 \, \text{MeV}}{3} = 60 \, \text{MeV}. \] Thus, the average kinetic energy carried by each fast neutron is \( {60 \, \text{MeV}} \).
The velocity-time graph of an object moving along a straight line is shown in the figure. What is the distance covered by the object between \( t = 0 \) to \( t = 4s \)?