From the first law of thermodynamics, show the following formulas C_V = (frac{partial U}{partial T})_V , C_P = (frac{partial H}{partial T})_P , where C_V and C_P are heat capacities at constant volume and constant pressure, respectively. U and H are internal energy and enthalpy, respectively.
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For a simple compressible system with only pV work, δW = p dV, so δQ = dU + p dV. Show more…
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