For a nucleus:
Volume: \[ V = \frac{4}{3} \pi R^3 \]
Relationship for the radius:
\[ R = R_0 \left( A \right)^{1/3} \]
Substitute \( R \) in the volume equation:
\[ V = \frac{4}{3} \pi \left( R_0 (A)^{1/3} \right)^3 A \]
Simplifying:
\[ \Rightarrow \frac{V_2}{V_1} = \frac{A_2}{A_1} = 4 \]
For a nucleus, the volume \( V \) is proportional to \( A \), the mass number, given by:
\[ V = \frac{4}{3}\pi R^3, \]where the radius \( R \) of a nucleus is proportional to the cube root of its mass number \( A \):
\[ R = R_0 A^{1/3}. \]Thus, the volume \( V \) of a nucleus can be expressed as:
\[ V \propto A. \]Since \( A_2 = 4A_1 \), the ratio of volumes is:
\[ \frac{V_2}{V_1} = \frac{A_2}{A_1} = 4. \]The largest $ n \in \mathbb{N} $ such that $ 3^n $ divides 50! is:
For the thermal decomposition of \( N_2O_5(g) \) at constant volume, the following table can be formed, for the reaction mentioned below: \[ 2 N_2O_5(g) \rightarrow 2 N_2O_4(g) + O_2(g) \] Given: Rate constant for the reaction is \( 4.606 \times 10^{-2} \text{ s}^{-1} \).
