Given that both wires share identical material composition and mass, their volumes are also equal. Let \(\rho\) denote resistivity, \(A\) represent the cross-sectional area, \(V\) denote volume, and \(\ell\) signify length.
The resistance \(R\) of a wire is defined as:
\[ R = \frac{\rho \ell}{A} = \frac{\rho V}{A^2}. \]
As \(V\) remains constant for both wires, the ratio of their resistances can be expressed as:
\[ \frac{R_A}{R_B} = \frac{A_B^2}{A_A^2} = \frac{r_B^4}{r_A^4}. \]
Substituting the given values \(R_B = 2 \, \Omega\), \(r_B = 4 \, \text{mm}\), and \(r_A = 2 \, \text{mm}\):
\[ \frac{R_A}{2} = \left(\frac{4 \times 10^{-3}}{2 \times 10^{-3}}\right)^4. \]
Simplification yields:
\[ \frac{R_A}{2} = 16, \]
resulting in:
\[ R_A = 32 \, \Omega. \]
