Given that the volume of the wire remains constant, we use the relation: \[ A_1 L_1 = A_2 L_2 \] Where: - \( A_1 \) and \( L_1 \) are the area and length of the original wire, - \( A_2 \) and \( L_2 \) are the area and length of the new wire. The volume of the wire is constant, so the area of cross-section \( A_2 \) and the length \( L_2 \) change according to the new dimensions. Since the length of the new wire is one-fourth of the original, we have: \[ A_1 L_1 = A_2 L_2 \quad \Rightarrow \quad A_2 = 4 A_1 \] For resistance \( R \), we know: \[ R = \rho \frac{L}{A} \] Thus, for the new wire: \[ R_2 = \rho \frac{L_2}{A_2} = \rho \frac{L/4}{4A} = \rho \frac{L}{16A} = \frac{1}{16} R_1 \] Substituting \( R_1 = 160 \Omega \): \[ R_2 = \frac{1}{16} \times 160 = 10 \Omega \] Thus, the new resistance is \( \boxed{10} \Omega \).
A wire of resistance $ R $ is bent into a triangular pyramid as shown in the figure, with each segment having the same length. The resistance between points $ A $ and $ B $ is $ \frac{R}{n} $. The value of $ n $ is:


\[ f(x) = \left\{ \begin{array}{ll} 1 - 2x & \text{if } x < -1 \\ \frac{1}{3}(7 + 2|x|) & \text{if } -1 \leq x \leq 2 \\ \frac{11}{18} (x-4)(x-5) & \text{if } x > 2 \end{array} \right. \]