148440 Five moles of Hydrogen gas initially at STP is compressed adiabatically so that its temperature becomes $673 \mathrm{~K}$. The increase in internal energy of the gas is \(\left(\mathrm{R}=8.3 \mathrm{~J} \mathrm{~mol}^{-1} \mathrm{~K}^{-1}, \gamma=1.4\right.\) for diatomic gas)
148440 Five moles of Hydrogen gas initially at STP is compressed adiabatically so that its temperature becomes $673 \mathrm{~K}$. The increase in internal energy of the gas is \(\left(\mathrm{R}=8.3 \mathrm{~J} \mathrm{~mol}^{-1} \mathrm{~K}^{-1}, \gamma=1.4\right.\) for diatomic gas)
148440 Five moles of Hydrogen gas initially at STP is compressed adiabatically so that its temperature becomes $673 \mathrm{~K}$. The increase in internal energy of the gas is \(\left(\mathrm{R}=8.3 \mathrm{~J} \mathrm{~mol}^{-1} \mathrm{~K}^{-1}, \gamma=1.4\right.\) for diatomic gas)
148440 Five moles of Hydrogen gas initially at STP is compressed adiabatically so that its temperature becomes $673 \mathrm{~K}$. The increase in internal energy of the gas is \(\left(\mathrm{R}=8.3 \mathrm{~J} \mathrm{~mol}^{-1} \mathrm{~K}^{-1}, \gamma=1.4\right.\) for diatomic gas)
148440 Five moles of Hydrogen gas initially at STP is compressed adiabatically so that its temperature becomes $673 \mathrm{~K}$. The increase in internal energy of the gas is \(\left(\mathrm{R}=8.3 \mathrm{~J} \mathrm{~mol}^{-1} \mathrm{~K}^{-1}, \gamma=1.4\right.\) for diatomic gas)