Match Column-I with Column-II. \begin{tabular}{|l|l|c|l|} \hline \multicolumn{2}{|c|}{ Columm-I ...
0Match Column-I with Column-II.
\begin{tabular}{|l|l|c|l|}
\hline \multicolumn{2}{|c|}{ Columm-I } & \multicolumn{2}{c|}{ Columm-II } \\
\hline A. & \( \begin{array}{l}\text { Reversible isothermal } \\
\text { expansion of an ideal } \\
\text { gas. }\end{array} \) & p. & \( \begin{array}{l}\mathrm{w}=-2.303 \mathrm{nRT} \log \\
\left(\frac{\mathrm{V}_{2}}{\mathrm{~V}_{1}}\right)\end{array} \) \\
\hline B. & \( \begin{array}{l}\text { Reversible adiabatic } \\
\text { compression of an ideal } \\
\text { gas. }\end{array} \) & q. & \( \mathrm{PV} \gamma= \) constant \\
\hline C. & \( \begin{array}{l}\text { Irreversible adiabatic } \\
\text { expansion of an ideal } \\
\text { gas. }\end{array} \) & r. & \( \mathrm{w}=\frac{\mathrm{nR}}{(\gamma-1)}\left(\mathrm{T}_{2}-\mathrm{T}_{1}\right) \) \\
\hline D. & \( \begin{array}{l}\text { Irreversible isothermal } \\
\text { compression of an ideal } \\
\text { gas. }\end{array} \) & s. & \( \Delta \mathrm{H}=0 \) \\
\hline
\end{tabular}
(a) A-(p, s); B-(q, r); C-(r); D-(s)
(b) A-(p); B-(r); C-(p, r); D-(s,q)
(c) A-(p, q); B-(p, s); C-(r); D-(s)
(d) A-(s); B-(p, r); C-(p, r); D-(q, p)
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