Partition function: Difference between revisions
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at temperature <math>T</math> is the normalization constant of the [[Boltzmann distribution]] | at temperature <math>T</math> is the normalization constant of the [[Boltzmann distribution]] | ||
function, and therefore its expression is given by | function, and therefore its expression is given by | ||
:<math> \left. Z \right.= {\mathrm {Tr}} \{ e^{-\beta H} \}</math> | |||
where ''H'' is the [[Hamiltonian]], or as | |||
:<math>Z(T)=\int \Omega(E)\exp(-E/k_BT)\,dE</math>, | :<math>Z(T)=\int \Omega(E)\exp(-E/k_BT)\,dE</math>, | ||
Revision as of 15:21, 24 September 2007
The canonical ensemble partition function of a system in contact with a thermal bath at temperature is the normalization constant of the Boltzmann distribution function, and therefore its expression is given by
where H is the Hamiltonian, or as
- ,
where is the density of states with energy and the Boltzmann constant. The symbol Z is from the German Zustandssumme meaning "sum over states".
Helmholtz energy function
The partition function of a system is related to the Helmholtz energy function through the formula
This connection can be derived from the fact that is the entropy of a system with total energy . This is an extensive magnitude in the sense that, for large systems (i.e. in the thermodynamic limit, when the number of particles or the volume ), it is proportional to or . In other words, if we assume large, then
where is the entropy per particle in the thermodynamic limit, which is a function of the energy per particle . We can therefore write
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left.Z(T)\right.=N\int \exp\{N(s(e)-e/T)/k_B\}\,de.}
Since Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle N} is large, this integral can be performed through steepest descent, and we obtain
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left.Z(T)\right.=N\exp\{N(s(e_0)-e_0/k_BT)\}} ,
where Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle e_0} is the value that maximizes the argument in the exponential; in other words, the solution to
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left.s'(e_0)\right.=1/T.}
This is the thermodynamic formula for the inverse temperature provided Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle e_0} is the mean energy per particle of the system. On the other hand, the argument in the exponential is
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \frac{1}{k_BT}(TS(E_0)-E_0)=-\frac{A}{k_BT}}
the thermodynamic definition of the Helmholtz energy function. Thus, when Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle N} is large,
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left.A\right.=-k_BT\log Z(T).}
Connection with thermodynamics
We have the aforementioned Helmholtz energy function,
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \left.A\right.=-k_BT\log Z(T)}
we also have the internal energy, which is given by
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle U=k_B T^{2} \left. \frac{\partial \log Z(T)}{\partial T} \right\vert_{N,V}}
and the pressure, which is given by
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle p=k_B T \left. \frac{\partial \log Z(T)}{\partial V} \right\vert_{N,T}} .
These equations provide a link between classical thermodynamics and statistical mechanics