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We know that ideal gas equation
"PV=nRT"
P=constant differentiate with respect T
"(\\frac{dV}{dT})_p=\\frac{R}{P}"
V constant differentiate with respect to T
"(\\frac{dP}{dT})_V=\\frac{R}{V}"
Now We know that
"c_p=[\\frac{dQ}{dT}]_p"
"C_p-C_v=T[\\frac{dp}{dT}]_v[\\frac{dV}{dT}]_p"
Assume
"C_v=0"
"C_p=T[\\frac{dp}{dT}]_v[\\frac{dV}{dT}]_p"
We know that
"[\\frac{dp}{dT}]_v=[\\frac{dp}{dT}]_s"
"C_p=T[\\frac{dp}{dT}]_s[\\frac{dV}{dT}]_p"
Hance proved
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