Master equation: Difference between revisions
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Carl McBride (talk | contribs) m (Added terms) |
Carl McBride (talk | contribs) m (→References: Corrected spelling error) |
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:<math>G_{00}(\tau) = \frac{1}{2\pi i} \oint_c \exp (-iz \tau) \psi^+_{00} (z)~ {\mathrm d}z </math> | :<math>G_{00}(\tau) = \frac{1}{2\pi i} \oint_c \exp (-iz \tau) \psi^+_{00} (z)~ {\mathrm d}z </math> | ||
==References== | ==References== | ||
#[http://dx.doi.org/10.1016/0031-8914(61)90008-8 I. | #[http://dx.doi.org/10.1016/0031-8914(61)90008-8 I. Prigogine and P. Résibois "On the kinetics of the approach to equilibrium", Physica '''27''' pp. 629-646 (1961)] | ||
[[category: Non-equilibrium thermodynamics]] | [[category: Non-equilibrium thermodynamics]] | ||
Revision as of 13:26, 27 June 2008
The master equation describes the exact behavior of the velocity distribution for any time (Ref. 1 Eq. 3-11)
where the time dependent functional of the initial conditions is given by (Ref. 1 Eq. 3-9)
- Failed to parse (Conversion error. Server ("https://wikimedia.org/api/rest_") reported: "Cannot get mml. Server problem."): {\displaystyle {\mathcal {D}}_{0}\left(t,\rho _{\{k''\}}\left(\{{\mathbf {\upsilon } }\},0\right)\right)={\frac {-1}{2\pi }}\oint _{c}\exp(-izt)\sum _{\{k''\}\neq 0}{\mathcal {D}}_{0\{k''\}}^{+}(z)\rho _{\{k''\}}\left(\{{\mathbf {\upsilon } }\},0\right)}
and the diagonal fragment is given by (Ref. 1 Eq. 3-10)
- 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 G_{00}(\tau) = \frac{1}{2\pi i} \oint_c \exp (-iz \tau) \psi^+_{00} (z)~ {\mathrm d}z }