Let initial volume of air in tyre be V and after pumping one stroke it becomes (V + dP) and pressure increased from P to (P + dP).
Then,
P1V1γ = P2V2γ
P(V + dV)γ= (P + dP)Vγ
PVγ. \((1+\frac{dV}{V})^γ\) = \(P[1+\frac{dP}{P}]V^γ\)
Volume of tyre remains constant
PVγ. \([1+γ\frac{dV}{V}]\) = \(PV^γ[1+\frac{dP}{P}]\)
or, \(
γ\frac{dV}{V}=\frac{dP}{P}\)
or, \(
{dV}=\frac{VdP}{γP}\)
or, \(
{PdV}=\frac{VdP}{γ}\)
Integrating both sides,
\(\int{PdV}\)= \(\int^{p_2}_{p_1}\frac{VdP}{γ}\)
or, \(\int{dW}\) = \(\int^{p_2}_{p_1}\frac{VdP}{γ}\) [V = constant]