# Clausius–Duhem inequality

The Clausius–Duhem inequality[1][2] is a way of expressing the second law of thermodynamics that is used in continuum mechanics. This inequality is particularly useful in determining whether the constitutive relation of a material is thermodynamically allowable.[3]

This inequality is a statement concerning the irreversibility of natural processes, especially when energy dissipation is involved. It was named after the German physicist Rudolf Clausius and French physicist Pierre Duhem.

## Clausius–Duhem inequality in terms of the specific entropy

The Clausius–Duhem inequality can be expressed in integral form as

${\displaystyle {\cfrac {d}{dt}}\left(\int _{\Omega }\rho ~\eta ~{\text{dV}}\right)\geq \int _{\partial \Omega }\rho ~\eta ~(u_{n}-\mathbf {v} \cdot \mathbf {n} )~{\text{dA}}-\int _{\partial \Omega }{\cfrac {\mathbf {q} \cdot \mathbf {n} }{T}}~{\text{dA}}+\int _{\Omega }{\cfrac {\rho ~s}{T}}~{\text{dV}}.}$

In this equation ${\displaystyle t\,}$ is the time, ${\displaystyle \Omega \,}$ represents a body and the integration is over the volume of the body, ${\displaystyle \partial \Omega \,}$ represents the surface of the body, ${\displaystyle \rho \,}$ is the mass density of the body, ${\displaystyle \eta \,}$ is the specific entropy (entropy per unit mass), ${\displaystyle u_{n}\,}$ is the normal velocity of ${\displaystyle \partial \Omega \,}$, ${\displaystyle \mathbf {v} }$ is the velocity of particles inside ${\displaystyle \Omega \,}$, ${\displaystyle \mathbf {n} }$ is the unit normal to the surface, ${\displaystyle \mathbf {q} }$ is the heat flux vector, ${\displaystyle s\,}$ is an energy source per unit mass, and ${\displaystyle T\,}$ is the absolute temperature. All the variables are functions of a material point at ${\displaystyle \mathbf {x} }$ at time ${\displaystyle t\,}$.

In differential form the Clausius–Duhem inequality can be written as

${\displaystyle \rho ~{\dot {\eta }}\geq -{\boldsymbol {\nabla }}\cdot \left({\cfrac {\mathbf {q} }{T}}\right)+{\cfrac {\rho ~s}{T}}}$

where ${\displaystyle {\dot {\eta }}}$ is the time derivative of ${\displaystyle \eta \,}$ and ${\displaystyle {\boldsymbol {\nabla }}\cdot (\mathbf {a} )}$ is the divergence of the vector ${\displaystyle \mathbf {a} }$.

## Clausius–Duhem inequality in terms of specific internal energy

The inequality can be expressed in terms of the internal energy as

${\displaystyle \rho ~({\dot {e}}-T~{\dot {\eta }})-{\boldsymbol {\sigma }}:{\boldsymbol {\nabla }}\mathbf {v} \leq -{\cfrac {\mathbf {q} \cdot {\boldsymbol {\nabla }}T}{T}}}$

where ${\displaystyle {\dot {e}}}$ is the time derivative of the specific internal energy ${\displaystyle e\,}$ (the internal energy per unit mass), ${\displaystyle {\boldsymbol {\sigma }}}$ is the Cauchy stress, and ${\displaystyle {\boldsymbol {\nabla }}\mathbf {v} }$ is the gradient of the velocity. This inequality incorporates the balance of energy and the balance of linear and angular momentum into the expression for the Clausius–Duhem inequality.

## Dissipation

The quantity

${\displaystyle {\mathcal {D}}:=\rho ~(T~{\dot {\eta }}-{\dot {e}})+{\boldsymbol {\sigma }}:{\boldsymbol {\nabla }}\mathbf {v} -{\cfrac {\mathbf {q} \cdot {\boldsymbol {\nabla }}T}{T}}\geq 0}$

is called the dissipation which is defined as the rate of internal entropy production per unit volume times the absolute temperature. Hence the Clausius–Duhem inequality is also called the dissipation inequality. In a real material, the dissipation is always greater than zero.