To solve the problem, we need to use the concept of Root Mean Square (RMS) speed for gases, which is derived from the kinetic theory of gases.
The RMS speed, \( v_{\text{rms}} \), of a gas is given by the formula:
\(v_{\text{rms}} = \sqrt{\frac{3kT}{m}}\)
where:
Given that the RMS speeds of \(\mathrm{H_2}\) and \(\mathrm{O_2}\) gases are the same, we have:
\(\sqrt{\frac{3kT_{\mathrm{H_2}}}{m_{\mathrm{H_2}}}} = \sqrt{\frac{3kT_{\mathrm{O_2}}}{m_{\mathrm{O_2}}}}\)
By canceling out the common terms and squaring both sides, we get:
\(\frac{T_{\mathrm{H_2}}}{m_{\mathrm{H_2}}} = \frac{T_{\mathrm{O_2}}}{m_{\mathrm{O_2}}}\)
Rearranging gives:
\(T_{\mathrm{H_2}} = T_{\mathrm{O_2}} \cdot \frac{m_{\mathrm{H_2}}}{m_{\mathrm{O_2}}}\)
Let's plug in the known values:
Substitute these values into the equation:
\(T_{\mathrm{H_2}} = 296\ \mathrm{K} \times \frac{2\ \mathrm{g/mol}}{32\ \mathrm{g/mol}}\)
Simplifying, we find:
\(T_{\mathrm{H_2}} = 296\ \mathrm{K} \times \frac{1}{16} = 18.5\ \mathrm{K}\)
Thus, the temperature of the \(\mathrm{H_2}\) gas is \(18.5\ \mathrm{K}\).

For an ideal gas, a cyclic process ABCA as shown in the P–T diagram. When represented in P–V plot, it would be 