For the process A - B, it is given that
PT = constant
Differentiating above equation partially, we have
PdT + TdP = 0
Equation of state for two moles of a gas
`PV = 2 RT` or `P = (2RT)/(V)`
After differentiating Eq. (ii) partially, we get
PdV + VdP = 2R dT
From Eq. (ii) partially, we get
PdV + VdP = 2R dT
From Eqs. (i) and (ii), we have
`((2RT)/(V)) dT + T dP = 0`
or 2RT dT + VTdP = 0
VdP = - 2 RdT
Now form Eqs. (iii) and (iv), we have
`- 2RdT + VdP = 2RdT`
or `PdV = 4 RdT`
a. The work done in the process AB
`W_(AB) int PdV = int_(600)^(300) 4 RdT`
`= 4 R |T|_(600)^(300) = 4 R (300 - 600)`
`= - 1200 R`
b. As process `B rarr C` is isobaric, so
`Q_(BC) = nC_(P) Delta T = 2 xx (5R)/(2) xx (600 - 300)`
= 1500 R
ii. Process `C rarr A` is isothermal, so `Delta U = 0`
`Q_(CA) = Delta U + W_(CA) = W-(CA)`
`W_(CA) = nRT 1n (P_(C ) // P_(A))`
`2R xx 600 1n (2P_(1) // P_(1)) = 1200 R1n 2`
`Q_(CA) = 1200 R 1n 2`
Again for process `A rarr B`
`Q_(AB) = Delta U + W_(AB)`
`= nC_(V) Delta T + W_(AB)`
`= 2 xx ((3R)/(2)) xx (300 - 600) - 1200 R`
`= - 900 R - 1200 R = - 2100 R`