Since both wires are made of the same material and have the same mass, they also have the same volume. Let \(\rho\) be the resistivity, \(A\) the cross-sectional area, \(V\) the volume, and \(\ell\) the length.
The resistance \(R\) of a wire is given by:
\[ R = \frac{\rho \ell}{A} = \frac{\rho V}{A^2}. \]
Since \(V\) is constant for both wires, we can write:
\[ \frac{R_A}{R_B} = \frac{A_B^2}{A_A^2} = \frac{r_B^4}{r_A^4}. \]
Given \(R_B = 2 \, \Omega\), \(r_B = 4 \, \text{mm}\), and \(r_A = 2 \, \text{mm}\), we substitute these values:
\[ \frac{R_A}{2} = \left(\frac{4 \times 10^{-3}}{2 \times 10^{-3}}\right)^4. \]
Simplifying this, we get:
\[ \frac{R_A}{2} = 16, \]
which gives:
\[ R_A = 32 \, \Omega. \]
In the given circuit the sliding contact is pulled outwards such that the electric current in the circuit changes at the rate of 8 A/s. At an instant when R is 12 Ω, the value of the current in the circuit will be A.
Let A be a 3 × 3 matrix such that \(\text{det}(A) = 5\). If \(\text{det}(3 \, \text{adj}(2A)) = 2^{\alpha \cdot 3^{\beta} \cdot 5^{\gamma}}\), then \( (\alpha + \beta + \gamma) \) is equal to: