- ✓$1219°C$
- B$1492°C$
- C$400°C$
- D$400\, K$
How, when other terms are constant, $(R \cdot M . S) \propto \sqrt{T}$.
$\frac{(R \cdot M \cdot S)_{1}}{(R \cdot M \cdot S)_{2}}=\frac{\sqrt{T_{1}}}{\sqrt{T_{2}}}$
Here, $(R \cdot M \cdot S)_{2}=2 \cdot(R \cdot M \cdot S)_{1}$
$T_{1} =100^{\circ} C =(100+273) K =373 \; K$
$\therefore \frac{(R \cdot M \cdot S)_{1}}{2 \cdot(R \cdot M \cdot S)} =\frac{\sqrt{373}}{\sqrt{T_{2}}}$
$\sqrt{T_{2}} =2 \cdot \sqrt{373}$
$T_{2} =1492 \; K$ [squaring both sides]
Convert into celcius.,
$T_{2}=(1492-273)^{\circ} C =1219^{\circ} C$
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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
