When a closed system receives, at constant volume, a quantity of heat Q V, its change in internal energy ΔU is equal to this quantity of heat : ΔU = U (final) – U (initial) = Q V( 1 )
When a closed system receives, at constant pressure, a quantity of heat Q P, its enthalpy variation ΔH is equal to this quantity of heat : ΔH = H (final) – H (initial) = Q P( 2 )
The definition of thermal capacity is very general and concerns a system as a whole (provided its temperature is uniform).
The notations Cp and C V are used for molar heat capacities, which is why the notations...
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