Relationship between Cv and Cp for an ideal gas is as follows:
Heat capacity, C=q/T [where, q: Heat; T: Temperature]
At constant volume, Heat capacity is denoted by Cv.
So, Cv= qv/∆T
Or, qv=Cv∆T -----------------(1)
Since, ∆U=q - P∆V [Where, ∆U: Internal energy change]
At constant volume , P∆V=0
Therefore, at constant volume, ∆U=qv -------(2)
From (1) and (2),
∆U =Cv∆T
At constant pressure, Heat capacity is denoted by Cp.
So, Cp= qp/∆T
qp= Cp∆T ---------------------(3)
we know, ∆H=∆U+∆(PV) [where, ∆H:enthalpy change]
At constant pressure, ∆H=∆U+ P∆V
Since at constant pressure, ∆U=qp- P∆V
qp=∆U+P∆V
qp=∆H -------------(4)
From (3) and (4),
∆H= Cp∆T
Since, ∆H=∆U+∆(PV)
∆H=∆U+∆(nRT) [we are deriving Relationship between Cv and Cp for an ideal gas]
∆H=∆U+∆(RT) [For 1 mole of an ideal gas]
∆H=∆U+R∆T
After putting the values of ∆H and ∆U in above equation ,we get,
Cp∆T = Cv∆T + R∆T
Cp = Cv + R or Cp- Cv = R