Pressure
#Physics
$\displaystyle P=\frac{F}{A}$
- $\displaystyle F$ is force
- $\displaystyle A$ is area
- Units are pascals or bars or torr or in Atm or in PSI
Statistical Mechanics
$\displaystyle P\equiv-\left( \frac{ \partial U }{ \partial V } \right)=\tau\left( \frac{ \partial \sigma }{ \partial V } \right)_{U}=\tau \frac{ \partial }{ \partial V }\ln Z$
- Statistical mechanics definition of pressure. Can be thought of as like a volumetric energy density
- $\displaystyle U$ is the [internal energy] of the system
- $\displaystyle V$ is volume of the system
- $\displaystyle \tau$ is the [fundamental temperature] of the system
- $\displaystyle \sigma$ is the [fundamental entropy] of the system
- $\displaystyle Z$ is the [partition function]
$\displaystyle P=-\left( \frac{ \partial U }{ \partial V } \right)_{\tau}+\tau\left( \frac{ \partial \sigma }{ \partial V } _{\tau} \right)$
- First term is energy pressure, important for solids
- Second term is entropy pressure, important for gases
$\displaystyle P=-\left( \frac{ \partial F }{ \partial V } \right)_{\tau}$
- $\displaystyle F$ is the [Helmholtz free energy]