Pressure dependence of the Heat Capacity

Click For Summary
SUMMARY

The discussion centers on the pressure dependence of heat capacity, specifically the relationship between isobaric specific heat (C_p) and isochoric specific heat (C_v) as described by the equations C_p/C_v = 1 + αγT and C_v = αVK_T/γ. Participants clarify that while specific heat is influenced by temperature, it does not inherently depend on pressure, as density changes with pressure rather than the specific heat itself. The conclusion emphasizes that specific heat remains a property of the substance, consistent across conditions for the same material, despite its temperature dependency.

PREREQUISITES
  • Understanding of thermodynamic principles, particularly heat capacity
  • Familiarity with the concepts of thermal expansivity (α) and the Anderson-Gruneisen parameter (γ)
  • Knowledge of isothermal bulk modulus (K_T) and its role in thermodynamics
  • Basic grasp of the relationship between density, temperature, and pressure
NEXT STEPS
  • Research the implications of temperature dependence on specific heat in various materials
  • Explore the mathematical modeling of heat transport considering density and specific heat
  • Investigate the effects of pressure on thermodynamic properties in different phases of matter
  • Learn about the derivation and application of the Anderson-Gruneisen parameter in material science
USEFUL FOR

Researchers, physicists, and engineers involved in thermodynamics, material science, and heat transfer analysis will benefit from this discussion, particularly those focusing on the properties of materials under varying temperature and pressure conditions.

Hypatio
Messages
147
Reaction score
1
I am trying to understand the nature of the dependence of heat capacity/specific heat on pressure.

I understand that one may give the the following relations:

\frac{C_p}{C_v}=1+\alpha\gamma T
where C_p,C_v,\alpha,\gamma, and T are isoberic specific heat, isochoric specific heat, thermal expansivity, Anderson-Gruneisen parameter, and Temperature, respectively.
C_v=\frac{\alpha V K_T}{\gamma}
where V is volume and K_T is the isothermal bulk modulus.What I do not think I fully grasp from these relationships is how the specific heat is related to the pressure. Is appears as though the heat capacity of a material depends on the pressure only because the density depends on the pressure.

In other words, and more specifically related to my own challenges; If I wanted to model heat transport with both the density and specific heat depending on pressure and temperature in a thermodynamically consistent way (lets ignore conductivity, with which I have no problems), I could use temperature-dependent data for C_p and temperature-pressure dependent data for the density and the model would be fully consistent (lets also ignore phase changes)?

If so, am I correct to say that it must be true that the specific heat, having the dimensions of J kg-1 K-1 actually does NOT have a dependence on pressure? And also, that the volumetric specific heat having dimensions J m-3 K-1 is actually just \rho C_p.

Thank you!
 
Science news on Phys.org
specific heat or heat capacity are the properties of the substance . the shall remain same under any condition for the same substance.
 
That explanation isn't compatible with the fact that specific heat is strongly temperature dependent. Why is specific heat temperature dependent and not pressure dependent?
 

Similar threads

  • · Replies 2 ·
Replies
2
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
2
Views
3K
  • · Replies 9 ·
Replies
9
Views
4K
  • · Replies 1 ·
Replies
1
Views
4K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 2 ·
Replies
2
Views
3K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 4 ·
Replies
4
Views
3K