To solve this problem, we need to apply the formula relating the radius of a nucleus to its mass number. The radius \( R \) of a nucleus is given by the formula:
\(R = R_0 A^{1/3}\)
where \( R_0 \) is a constant (~1.2-1.3 femtometers) and \( A \) is the mass number.
We are given that the radius of the first nucleus is half of the radius of a nucleus with mass number 192, denoted as \( R_1 = \frac{1}{2} R_2 \). Let \( A_1 \) be the mass number of the first nucleus, and \( A_2 = 192 \).
Rounding 24.68 to the nearest whole number gives 24. Therefore, the mass number of the nucleus having a radius equal to half of the radius of the nucleus with mass number 192 is 24.
The radius \( R \) of a nucleus is proportional to the cube root of its mass number \( A \):
\[ R \propto A^{1/3}. \]Let \( R_1 \) and \( R_2 \) be the radii of two nuclei with mass numbers \( A_1 \) and \( A_2 \), respectively. Given:
\[ R_1 = \frac{1}{2} R_2 \quad \text{and} \quad A_2 = 192. \]Using the proportionality,
\[ \frac{R_1}{R_2} = \left( \frac{A_1}{A_2} \right)^{1/3}. \]Substitute \( R_1 = \frac{1}{2} R_2 \):
\[ \frac{1}{2} = \left( \frac{A_1}{192} \right)^{1/3}. \]Cubing both sides:
\[ \frac{1}{8} = \frac{A_1}{192}. \]Solving for \( A_1 \):
\[ A_1 = 192 \times \frac{1}{8} = 24. \]Thus, the answer is:
\[ 24. \]
Given below are two statements. One is labelled as Assertion (A) and the other is labelled as Reason (R):
Assertion (A): In an insulated container, a gas is adiabatically shrunk to half of its initial volume. The temperature of the gas decreases.
Reason (R): Free expansion of an ideal gas is an irreversible and an adiabatic process.
In the light of the above statements, choose the correct answer from the options given below:

Current passing through a wire as function of time is given as $I(t)=0.02 \mathrm{t}+0.01 \mathrm{~A}$. The charge that will flow through the wire from $t=1 \mathrm{~s}$ to $\mathrm{t}=2 \mathrm{~s}$ is: