Amount of heat to be supplied to a given amount of a material to produce a unit change in its temperature:
C = \frac{\delta Q}{\delta T} |
Symbol | Dimension | SI units | Oil metric units | Oil field units |
---|---|---|---|---|
C | M L2 T−2 Θ−1 | J/K | J/K |
Heat Capacity depends on the way the heat is transferred and as such is not a table property of the matter.
The two major heat transfer processes are isobaric and isohoric which result in different values of heat capacity:
Both
C_P and
C_V are proportional to the amount of chemical substance involved in a heat transfer process and as such are not the material properties.
The ratio \gamma = C_P/C_V is called a Heat Capacity Ratio (γ) or Adiabatic Index (γ) or Isentropic expansion factor (κ) and is a material property.
Based on Mayer's relation the Isobaric heat capacity is always greater than Isochoric heat capacity:
(1) | C_P \geq C_V |
One can relate them to material properties through the known material mass
m or a material volume
V or material amount of substance
\nu:
Molar Heat Capacity | Specific heat capacity | Volumetric Heat Capacity | ||||||
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|
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Overall, there are totally six different intensive physical properties related to heat capacity:
Molar Heat Capacity | Specific heat capacity | Volumetric Heat Capacity | |||||||
---|---|---|---|---|---|---|---|---|---|
Isobaric (V= const) |
| Isobaric specific heat capacity
| Isobaric volumetric heat capacity
| ||||||
Isochoric (P = const) |
| Isochoric specific heat capacity
| Isochoric volumetric heat capacity
|
See also
Physics / Thermodynamics / Thermodynamic process / Heat Transfer
[ Heat ] [ Isobaric heat capacity ] [ Isochoric heat capacity ]
[ Specific heat capacity ] [ Volumetric Heat Capacity ][ Molar Heat Capacity ][ Mayer's relation ]