From first law of thermodynamics,
ΔU=q+W
The change in internal energy during the cyclic process is zero. Therefore, heat supplied to the gas is equal to work done by it, i.e.,
q=−W
As the heat is withdrawn from the sample, thus
q=−1200J
Therefore,
WTotal=−(−1200)=+1200J
As the cyclic process is traced anticlockwise, the net work done by the system is negative.
∴W=−1200
Now from fig.,
W=WA→B+WB→C+WC→A
⇒WA→B+WB→C+WC→A=−1200.....(1)(∵W=−1200J)
Now, work done during process A→B,
WA→B=PΔV=nRΔT(From ideal gas equation, i.e., PV=nRT)
∴WA→B=nR(TB−TA)
⇒WA→B=2×8.314×(500−300)
⇒WA→B=3325.6J
Now work done during process B→C,
WB→C=?
Now work done during process C→A,
WC→A=0(∵V is constant, i.e., ΔV=0)
Now from eqn(1), we have
3325.6+WB→C+0=−1200
⇒WB→C=−1200+(−3325.6)=−4525.6J
Hence the work done by the gas in process B→C is −4525.6J.