A conducting wire is stretched by applying a deforming force, so that its diameter decreases to 40% of the original value. The percentage change in its resistance will be:
Step 1: {Understanding the effect of stretching}
Since the volume of the wire remains constant, we use the relation: \[ V = A l \] where \(A\) is the cross-sectional area and \(l\) is the length.
Step 2: {Deriving the new resistance}
We use the resistance formula: \[ R = \rho \frac{l}{A} \] Since \(A\) decreases as \(d^2\) and \(l\) increases proportionally: \[ \frac{\Delta R}{R} = -4 \frac{\Delta D}{D} \] Substituting \(\Delta D = -0.4\), \[ \frac{\Delta R}{R} = -4(-0.4) = 1.6\% \] Thus, the percentage change in resistance is \(1.6\%\).
The stopping potential (\(V_0\)) versus frequency (\(\nu\)) of a graph for the photoelectric effect in a metal is given. From the graph, the Planck's constant (\(h\)) is:

In the diagram shown below, both the strings AB and CD are made of the same material and have the same cross-section. The pulleys are light and frictionless. If the speed of the wave in string AB is \( v_1 \) and in CD is \( v_2 \), then the ratio \( \frac{v_1}{v_2} \) is:
