(T –2.4) K
(T + 4)K
(T – 4) K
(T + 2.4)K
To solve the problem, we need to determine the final temperature of an ideal gas after it performs adiabatic work.
Given data:
For an adiabatic process, the relation between initial and final temperatures is given by:
T_{\text{final}} = T_{\text{initial}} \times \left( \frac{V_{\text{final}}}{V_{\text{initial}}} \right)^{1 - \gamma}However, an alternative way to use the work done in terms of change in internal energy is to use:
W = nC_v(T_{\text{initial}} - T_{\text{final}})Because the work done is 6R, and using the relation C_p - C_v = R along with \gamma = \frac{C_p}{C_v}, we can calculate:
C_v = \frac{R}{\gamma - 1}Substituting given \gamma = 35:
C_v = \frac{R}{35 - 1} = \frac{R}{34}Now solve for the final temperature:
6R = \left(\frac{R}{34}\right)(T - T_f) 204 = T - T_f T_f = T - 204Therefore, our working step needs a correction, with actual question parameters and calculations:
Since specific problematic ratio handling is suspect:
Need to restate under exam correction checks:
Correct deduction was non-finale solved, mismapping mentioned by mistake possibly 4 decrement consideration?
Hence Correct answer Using clean check route:
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 \( R = 8 \, \text{J/molK} \)):
