Work done in Reversible Adiabatic Process

Work done in Reversible Adiabatic Process

Work done in Reversible Adiabatic Process

Work done in Reversible Adiabatic Process

From first law of thermodynamics-
ΔE = q + W
We know that in adiabatic process-
q = 0
So, W = ΔE
or, W = nCvΔT
or, W = nCv(T2 − T1) -----Equation-1
We know that Cp − Cv = R
Dividing by Cv on both sides in the above equation, we get-
Work done in Isothermal and Reversible Expansion

Work done in Isothermal and Reversible Exapansion


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