To find the final temperature of the gas after an adiabatic expansion, we use the formula for adiabatic processes:
\( W = C_V (T_i - T_f) \)
Where:
Rearrange the formula to solve for \( T_f \):
\( T_f = T_i - \frac{W}{C_V} \)
Substitute the known values:
\( T_f = 300 \, \text{K} - \frac{3000 \, \text{J}}{20 \, \text{J} \cdot \text{mol}^{-1} \cdot \text{K}^{-1}} \)
Simplify the calculation:
\( T_f = 300 \, \text{K} - 150 \, \text{K} \)
\( T_f = 150 \, \text{K} \)
The final temperature of the gas is 150 K, which falls within the expected range as specified.
A real gas within a closed chamber at \( 27^\circ \text{C} \) undergoes the cyclic process as shown in the figure. The gas obeys the equation \( PV^3 = RT \) for the path A to B. The net work done in the complete cycle is (assuming \( R = 8 \, \text{J/molK} \)):
