For a thermodynamic system, isobaric coefficient of volume expansion (alpa) and isothermal compressibility (bita) are defined as
ailpa=1/V(dV/dT)p
bita=-1/V(dV/dT)T
Show that for an isochoric change, dp = dT.
Given,
"\\alpha = \\frac{1}{V}(\\frac{dV}{dT})_p"
"\\beta = - \\frac{1}{V}(\\frac{dV}{dP})_T"
Now, from the ideal gas equation,
"PV=nRT"
"V=\\frac{nRT}{P}"
Now, taking the differentiation with respect to the corresponding terms,
"\\frac{dV}{dT}=\\frac{nR}{P}"
if P is constant then,
"(\\frac{dV}{dT})_P=\\frac{nR}{P}...(i)"
now, taking the differentiation with respect to P,
"(\\frac{dV}{dP})_T=\\frac{nRT}{P^2}...(ii)"
Now, taking the ratio of "(i)" and "(ii)"
"\\frac{(\\frac{dV}{dT})_P}{(\\frac{dV}{dP})_T}=\\frac{\\frac{nR}{P}}{\\frac{nRT}{P^2}}"
"\\frac{(dP)_T}{(dT)_P}=\\frac{P}{T}"
"(dP)_T=(dT)_P\\times \\frac{P}{T}"
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