What is meant by heat capacity at constant pressure?

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SUMMARY

Heat capacity at constant pressure, denoted as \(C_p\), is a fundamental thermodynamic property defined by the equation \(C_p=\left(\frac{\partial H}{\partial T}\right)_P\), where \(H\) represents the molar enthalpy of a material. This property does not depend on whether the pressure is constant externally or internally, as thermodynamics assumes equilibrium where internal and external pressures are equal. Even in irreversible processes with non-uniform internal pressure and temperature, the local definition of heat capacity remains valid.

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  • Understanding of thermodynamic principles
  • Familiarity with molar enthalpy concepts
  • Knowledge of the relationship between pressure and temperature in physical systems
  • Basic grasp of irreversible processes in thermodynamics
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  • Study the derivation and applications of the heat capacity equations in thermodynamics
  • Explore the differences between heat capacities at constant pressure (\(C_p\)) and constant volume (\(C_v\))
  • Investigate the implications of irreversible processes on thermodynamic properties
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Students and professionals in chemistry and physics, particularly those studying thermodynamics, material science, and engineering applications involving heat transfer and energy systems.

Fermion70
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Generally in chemistry and physics, we learned that a material has a heat capacity at constant pressure. However, I am confused at whether this refers to a constant external pressure or a constant system internal pressure?

Thanks.
 
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Hello half integer spin, :welcome:

Thermodynamics is about equilibrium. Internal pressure and external pressure are supposed to be equal.
 
To elaborate on what BvU said, heat capacity is a physical property of a material, and does not depend on the process being applied to the material. Heat capacity per mole at constant pressure is defined as $$C_p=\left(\frac{\partial H}{\partial T}\right)_P$$
where H is the molar enthalpy of the material. If a process is irreversible so that the internal pressure and temperature of the material are not uniform, this equation still applies locally.
 

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