Step 1: {Given data}
Temperature, \( T = 273 \, {K} \) Molecular mass of oxygen, \( M = 32 \times 10^{-3} \, {kg} \)
Step 2: {Calculating the speed of sound}
\[ v = \sqrt{\frac{\gamma RT}{M}} = \sqrt{\frac{1.4 \times 8.3 \times 273}{32 \times 10^{-3}}} \approx 315 \, {m/s} \] Thus, the speed of sound in oxygen at STP is approximately 315 m/s.
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:
