148170
Two moles of helium gas $\left(\gamma=\frac{5}{3}\right)$ at $27^{\circ} \mathrm{C}$ is
expanded at constant pressures until its volume is doubled. Then it undergoes an adiabatic changes until the temperatures returns to its initial value. The work done during adiabatic process is
(universal gas constant $=8.3 \mathrm{j} \mathrm{mol}^{-1} \mathrm{~K}^{-1}$ )
148170
Two moles of helium gas $\left(\gamma=\frac{5}{3}\right)$ at $27^{\circ} \mathrm{C}$ is
expanded at constant pressures until its volume is doubled. Then it undergoes an adiabatic changes until the temperatures returns to its initial value. The work done during adiabatic process is
(universal gas constant $=8.3 \mathrm{j} \mathrm{mol}^{-1} \mathrm{~K}^{-1}$ )
148170
Two moles of helium gas $\left(\gamma=\frac{5}{3}\right)$ at $27^{\circ} \mathrm{C}$ is
expanded at constant pressures until its volume is doubled. Then it undergoes an adiabatic changes until the temperatures returns to its initial value. The work done during adiabatic process is
(universal gas constant $=8.3 \mathrm{j} \mathrm{mol}^{-1} \mathrm{~K}^{-1}$ )
148170
Two moles of helium gas $\left(\gamma=\frac{5}{3}\right)$ at $27^{\circ} \mathrm{C}$ is
expanded at constant pressures until its volume is doubled. Then it undergoes an adiabatic changes until the temperatures returns to its initial value. The work done during adiabatic process is
(universal gas constant $=8.3 \mathrm{j} \mathrm{mol}^{-1} \mathrm{~K}^{-1}$ )
148170
Two moles of helium gas $\left(\gamma=\frac{5}{3}\right)$ at $27^{\circ} \mathrm{C}$ is
expanded at constant pressures until its volume is doubled. Then it undergoes an adiabatic changes until the temperatures returns to its initial value. The work done during adiabatic process is
(universal gas constant $=8.3 \mathrm{j} \mathrm{mol}^{-1} \mathrm{~K}^{-1}$ )