$P V^{1.3}=K$
$W=\frac{P_2 V_2-P_1 V_1}{1-N}$
$\because N > 1$, so $W$ is negative.
Heat supplied by surrounding heat goes to do work.
$\therefore$ Down when expands.


Step $1$ It is first compressed adiabatically from volume $8.0 \,m ^{3}$ to $1.0 \,m ^{3}$.
Step $2$ Then expanded isothermally at temperature $T_{1}$ to volume $10.0 \,m ^{3}$.
Step $3$ Then expanded adiabatically to volume $80.0 \,m ^{3}$.
Step $4$ Then compressed isothermally at temperature $T_{2}$ to volume $8.0 \,m ^{3}$.
Then, $T_{1} / T_{2}$ is