216 MeV
0.9 MeV
9.4 MeV
804 MeV
To calculate the total gain in binding energy when a nucleus with a mass number of 240 breaks into two fragments each with a mass number of 120, we can follow these steps:
The binding energy per nucleon for the unfragmented nucleus is given as 7.6 MeV. Therefore, the total binding energy for the nucleus with mass number 240 is:
\(E_{\text{initial}} = 240 \times 7.6 \, \text{MeV}\)
Calculating this gives:
\(E_{\text{initial}} = 1824 \, \text{MeV}\)
Each fragment has a mass number of 120 and a binding energy per nucleon of 8.5 MeV. Therefore, the total binding energy for both fragments together is:
\(E_{\text{final}} = 2 \times (120 \times 8.5 \, \text{MeV})\)
Calculating this gives:
\(E_{\text{final}} = 2 \times 1020 \, \text{MeV} = 2040 \, \text{MeV}\)
The gain in binding energy, \(\Delta E\), is given by:
\(\Delta E = E_{\text{final}} - E_{\text{initial}}\)
Substitute the values we have calculated:
\(\Delta E = 2040 \, \text{MeV} - 1824 \, \text{MeV}\)
Calculating this gives:
\(\Delta E = 216 \, \text{MeV}\)
Thus, the total gain in binding energy in this process is 216 MeV, which is the correct answer.
The electric potential at the surface of an atomic nucleus \( (z = 50) \) of radius \( 9 \times 10^{-13} \) cm is \(\_\_\_\_\_\_\_ \)\(\times 10^{6} V\).
In a nuclear fission reaction of an isotope of mass \( M \), three similar daughter nuclei of the same mass are formed. The speed of a daughter nuclei in terms of mass defect \( \Delta M \) will be: