Step $1 A$ to $B$ adiabatic compression, $V_{A}=8 \,m ^{3}, V_{B}=1 \,m ^{3}$

Step $2 B$ to $C$ isothermal expansion,

$T_{C}=T_{B}=T_{1}, V_{C}=10 \,m ^{3}$

Step $3 C$ to $D$ adiabatic expansion,

$V_{D}=80 \,m ^{3}$

Step $4 D$ to $A$ isothermal compression,

$T_{D}=T_{A}=T_{2}, V_{A}=8 \,m ^{3}$

Now, for processes $A$ to $B$,

$T_{A} V_{A}^{\gamma-1}=T_{B} V_{B}^{\gamma-1}$

Substituting values in above equation, we get

$T_{2}(8)^{\frac{5}{3}-1}=T_{1}(1)^{\frac{5}{3}-1}$

$\therefore$ For ideal monoatomic gas, $\gamma=\frac{5}{3}$

So, $\quad \frac{T_{1}}{T_{2}}=8^{\frac{2}{3}}=4$