The radius \( R \) of a nucleus is proportional to the cube root of its mass number \( A \), described by the formula \( R = R_0 A^{1/3} \), where \( R_0 \) is a constant. We are given a nucleus with mass number \( A_2 = 192 \) and another nucleus with mass number \( A_1 \) such that its radius \( R_1 \) is half the radius \( R_2 \) of the nucleus with mass number 192, i.e., \( R_1 = \frac{1}{2} R_2 \).
Rounding to the nearest whole number, the mass number of the nucleus is 24.
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: