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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} 

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 define:

Both  and  are proportional to the amount of the matter involved in a Heat Transfer process and as such are not material properties.

One can relate them to material properties through the known material mass   or a material volume  or material amount of substance :

c_m = C/m

c_V = C/V

c_M = C/\nu

C_p= m \cdot c_{mp} = V \cdot c_{vp}

C_V= m \cdot c_{mV} = V \cdot c_{vV}

C_V= m \cdot c_{mV} = V \cdot c_{vV}

See also

Physics / Thermodynamics / Thermodynamic process / Heat Transfer

[ Heat ] [ Isobaric heat capacity ] [ Isochoric heat capacity ]

[ Specific heat capacity ] [ Volumetric Heat Capacity ][ Molar Heat Capacity ]