
$p = {p_0} - \frac{{2{P_0}}}{{{V_0}}}\left( {V - 2{V_0}} \right)$
using=$PV=nRT$
Temperature,$T = \frac{{{P_0}V - \frac{{2{P_0}{V^2}}}{{{V_0}}} + 4{P_0}V}}{{1 \times R}}$
$\left( {n = 1\,mole\,given} \right)$
$T = \frac{{{P_0}}}{R}\left[ {5V - \frac{{2{V^2}}}{{{V_0}}}} \right]$
$\frac{{dT}}{{dV}} = 0 \Rightarrow 5 - \frac{{4V}}{{{V_0}}} = 0 \Rightarrow V = \frac{5}{4}{V_0}$
$T = \frac{{{P_0}}}{R}\left[ {5 \times \frac{{5{V_0}}}{4} - \frac{2}{{{V_0}}} \times \frac{{25}}{{16}}V_0^2} \right] = \frac{{25}}{8}\frac{{{P_0}{V_0}.}}{R}$

$S1:$ The efficiency of a heat engine can be $1,$ but the coefficient of performance of a refrigerator can never be infinity.
$S2:$ The first law of thermodynamics is basically the principle of conservation of energy.
$S3:$ The second law of thermodynamics does not allow several phenomena consistent with the first law.
$S4:$ A process,whose only result is to transfer heat from a colder to a hotter object, is impossible.


