The total momentum before disintegration is equal to the total momentum after disintegration. Assuming the nucleus is initially at rest, the total momentum before disintegration is zero. Thus, the momenta of the two fragments after disintegration must be equal and opposite:
\[ m_1 V_1 = m_2 V_2, \]
where:
Rearranging for the velocity ratio:
\[ \frac{V_1}{V_2} = \frac{m_2}{m_1}. \]
Assuming the fragments have the same density, their masses are proportional to the cubes of their radii:
\[ \frac{m_2}{m_1} = \frac{r_2^3}{r_1^3}. \]
We are given \( \frac{r_2}{r_1} = 2^{1/3} \). Substituting this into the mass ratio equation:
\[ \frac{m_2}{m_1} = \left( \frac{r_2}{r_1} \right)^3 = \left( 2^{1/3} \right)^3 = 2. \]
Using the velocity ratio equation from Step 1:
\[ \frac{V_1}{V_2} = \frac{m_2}{m_1} = 2. \]
Therefore, \( V_1 : V_2 = n : 1 \), where \( n = 2 \).
The value of \( n \) is 2.

In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: