Specific Heat Capacity Derivation

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SUMMARY

The specific heat capacity at constant volume, \(c_v\), and at constant pressure, \(c_p\), are defined as partial derivatives of the internal energy \(u(T, v)\) and enthalpy \(h(T, p)\) respectively. These definitions are not derivable in the traditional sense as they represent intrinsic properties of pure, simple compressible substances rather than being directly related to heat, which is path-dependent. The terms specific heat and heat capacity are often used interchangeably, although heat capacity can also refer to the product of specific heat and the number of moles or mass.

PREREQUISITES
  • Understanding of thermodynamic properties such as internal energy and enthalpy.
  • Familiarity with the concepts of partial derivatives in thermodynamics.
  • Knowledge of intensive and extensive properties in physical chemistry.
  • Basic grasp of the definitions and differences between specific heat and heat capacity.
NEXT STEPS
  • Study the derivation of internal energy \(u(T, v)\) and enthalpy \(h(T, p)\) in thermodynamics.
  • Explore the implications of path dependence in thermodynamic processes.
  • Research the differences between intensive and extensive properties in detail.
  • Learn about the applications of specific heat and heat capacity in real-world scenarios.
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Students of thermodynamics, physical chemists, and engineers seeking a deeper understanding of heat capacity concepts and their applications in material science.

cwill53
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Homework Statement
Problem with Specific Heat Capacity Derivation
Relevant Equations
##c_v=\left ( \frac{\partial u}{\partial T} \right )_v##
##c_p=\left ( \frac{\partial h}{\partial T} \right )_p##
The specific heat capacity at constant volume and the specific heat capacity at constant pressure are intensive properties defined for pure, simple compressible substances as partial derivatives of the functions u(T, v) and h(T, p), respectively,
$$c_v=\left ( \frac{\partial u}{\partial T} \right )_v$$
$$c_p=\left ( \frac{\partial h}{\partial T} \right )_p$$
Can someone explain why this is? The book from which I got this from doesn't derive these expressions. I want to know what expressions for u(T,v) and h(T,p) are differentiated.
 
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cwill53 said:
Homework Statement:: Problem with Specific Heat Capacity Derivation
Relevant Equations:: ##c_v=\left ( \frac{\partial u}{\partial T} \right )_v##
##c_p=\left ( \frac{\partial h}{\partial T} \right )_p##

The specific heat capacity at constant volume and the specific heat capacity at constant pressure are intensive properties defined for pure, simple compressible substances as partial derivatives of the functions u(T, v) and h(T, p), respectively,
$$c_v=\left ( \frac{\partial u}{\partial T} \right )_v$$
$$c_p=\left ( \frac{\partial h}{\partial T} \right )_p$$
Can someone explain why this is? The book from which I got this from doesn't derive these expressions. I want to know what expressions for u(T,v) and h(T,p) are differentiated.
They are impossible to derive...because they are definitions. They will match the old definitions you are used to, in terms of heat, in the specific cases of constant volume and constant pressure, respectively. But defining them in terms of heat is not really valid because they are physical properties of the material, and not related to heat, which is process path dependent (and thus can't be a physical property).
 
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Chestermiller said:
They are impossible to derive...because they are definitions. They will match the old definitions you are used to, in terms of heat, in the specific cases of constant volume and constant pressure, respectively. But defining them in terms of heat is not really valid because they are physical properties of the material, and not related to heat, which is process path dependent (and thus can't be a physical property).
I see. Can heat capacity in general, not specific heat, be defined in terms of physical properties? Or are those also definitions.
 
cwill53 said:
I see. Can heat capacity in general, not specific heat, be defined in terms of physical properties? Or are those also definitions.
My experience is that most of the time, people use the terms specific heat and heat capacity synonymously. However, in some cases, heat capacity is used to mean specific heat times the number of moles or mass. So, either way, they are defined the way I have said. And in the latter case, heat capacity is the extensive property equivalent of specific heat, just as U is the extensive property equivalent of u.
 
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Chestermiller said:
My experience is that most of the time, people use the terms specific heat and heat capacity synonymously. However, in some cases, heat capacity is used to mean specific heat times the number of moles or mass. So, either way, they are defined the way I have said. And in the latter case, heat capacity is the extensive property equivalent of specific heat, just as U is the extensive property equivalent of u.
Thanks for the informative reply!
 

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