Internal pressure

From Wikipedia, the free encyclopedia

The classical Carnot heat engine
Book:Thermodynamics

Branches

State
Equation of state Ideal gas Real gas Phase / State of matter Equilibrium Control volume Instruments
Processes
Isobaric Isochoric Isothermal Adiabatic Isentropic Isenthalpic Quasistatic Polytropic Free expansion Reversibility Irreversibility Endoreversibility
Cycles
Heat engines Heat pumps Thermal efficiency

System properties

Functions of state (Conjugate variables in italics)
Property diagrams Intensive and extensive properties
Temperature / Entropy Introduction to entropy Pressure / Volume Chemical potential / Particle number Vapor quality Reduced properties
Process functions
Work Heat

Material properties

Specific heat capacity

$c=$

$T$	$\partial S$
$N$	$\partial T$

Compressibility

$\beta =-$

$1$	$\partial V$
$V$	$\partial p$

Thermal expansion

$\alpha =$

$1$	$\partial V$
$V$	$\partial T$

Property database

Equations

Potentials

Enthalpy
$H(S,p)=U+pV$

Helmholtz free energy
$A(T,V)=U-TS$

Gibbs free energy
$G(T,p)=H-TS$

History / Culture

Philosophy
Entropy and time Entropy and life Brownian ratchet Maxwell's demon Heat death paradox Loschmidt's paradox Synergetics
History
General Heat Entropy Gas laws "Perpetual motion" machines
Theories
Caloric theory Vis viva Theory of heat Mechanical equivalent of heat Motive power
Key publications
"An Experimental Enquiry Concerning ... Heat" "On the Equilibrium of Heterogeneous Substances" "Reflections on the Motive Power of Fire"
Timelines
Thermodynamics Heat engines
Art
Maxwell's thermodynamic surface
Education
Entropy as energy dispersal

Scientists

Internal pressure is a measure of how the internal energy of a system changes when it expands or contracts at constant temperature. It has the same dimensions as pressure, the SI unit of which is the pascal.

Internal pressure is usually given the symbol $\pi _{T}$ . It is defined as a partial derivative of internal energy with respect to volume at constant temperature:

$\pi _{T}=\left({\frac {\partial U}{\partial V}}\right)_{T}$

Thermodynamic equation of state

Internal pressure can be expressed in terms of temperature, pressure and their mutual dependence:

$\pi _{T}=T\left({\frac {\partial p}{\partial T}}\right)_{V}-p$

This equation is known as the thermodynamic equation of state for it expresses pressure in terms of thermodynamic properties of the system.

Derivation of the thermodynamic equation of state

Internal energy is a state function, therefore its differential is exact. We can take it to be a function of other state functions, namely entropy S and volume V:

$\operatorname {d}U=\left({\frac {\partial U}{\partial S}}\right)_{V}\operatorname {d}S+\left({\frac {\partial U}{\partial V}}\right)_{S}\operatorname {d}V$ .

Diving this equation by $\operatorname {d}V$ at constant temperature gives:

$\left({\frac {\partial U}{\partial V}}\right)_{T}=\left({\frac {\partial U}{\partial S}}\right)_{V}\left({\frac {\partial S}{\partial V}}\right)_{T}+\left({\frac {\partial U}{\partial V}}\right)_{S}$

Comparing the above differential with the fundamental thermodynamic equation $\operatorname {d}U=T\operatorname {d}S-p\operatorname {d}V$

gives

$\left({\frac {\partial U}{\partial S}}\right)_{V}=T$ and $\left({\frac {\partial U}{\partial V}}\right)_{S}=-p$ .

This, and the definition of internal pressure, leads to

$\pi _{T}=T\left({\frac {\partial S}{\partial V}}\right)_{T}-p$

One of the Maxwell relations states that

$\left({\frac {\partial S}{\partial V}}\right)_{T}=\left({\frac {\partial p}{\partial T}}\right)_{V}$

Inserting this into the above relation completes the proof.

Perfect gas

In a perfect gas, there are no potential energy interactions between the particles, so any change in the internal energy of the gas is directly proportional to the change in the kinetic energy of its constituent species and therefore also to the change in temperature:

$\operatorname {d}U\propto \operatorname {d}T$ .

The internal pressure is taken to be at constant temperature, therefore

$dT=0$ , which implies $dU=0$ and finally $\pi _{T}=0$ ,

i.e. the internal energy of a perfect gas is independent of the volume it occupies. The above relation can be used as a definition of a perfect gas.

The relation $\pi _{T}=0$ can be proved without the need to invoke any molecular arguments. It follows directly from the thermodynamic equation of state if we use the ideal gas law $pV=nRT$ .

Real gases

Plot of internal energy vs. volume for gases with different internal pressures

Real gases have non-zero internal pressures because their internal energy changes as the gases expand isothermally - it can increase on expansion ( $\pi _{T}>0$ , signifying presence of dominant attractive forces between the particles of the gas) or decrease ( $\pi _{T}<0$ ,dominant repulsion).

In the limit of infinite volume these internal pressures reach the value of zero:

$\lim _{{V\to \infty }}\pi _{T}=0$ ,

corresponding to the fact that all real gases can be approximated to be perfect in the limit of a suitably large volume. The above considerations are summarized on the graph on the right.

If a real gas can be described by the van der Waals equation of state

$p={\frac {nRT}{V-nb}}-a{\frac {n^{2}}{V^{2}}}$

it follows from the thermodynamic equation of state that

$\pi _{T}=a{\frac {n^{2}}{V^{2}}}$

Since the parameter $a$ is always positive, so is its internal pressure: internal energy of a van der Waals gas always increases when it expands isothermally.

The Joule experiment

James Joule tried to measure the internal pressure of air in his expansion experiment by isothermally pumping high pressure air from one metal vessel into another evacuated one. The water bath in which the system was immersed did not change its temperature, signifying that that no change in the internal energy occurred, the internal pressure of the air was equal to zero and the air was a perfect gas. The actual deviations from the perfect behaviour were not observed since they are very small and the specific heat capacity of water is relatively high.

References

Peter Atkins and Julio de Paula, Physical Chemistry 8th edition, pp. 60–61

This article is issued from Wikipedia. The text is available under the Creative Commons Attribution/Share Alike; additional terms may apply for the media files.