Equation 18 · The Statistical Mechanics of Irreversibility at Molecular Scale
What does this equation mean?
Read the formula alongside the article passage below. Each part has a deeper page with its role in the equation, the supporting passage and nearby citations.
This equation states an equality: the expressions on both sides have the same value under the article’s assumptions. Read the equation part by part below; each part has a contextual explanation and a link to its mathematical background.
Read it piece by piece
Symbol s_sys
ys is part of the quantity the equation computes from the expression on the right.
Symbol t
t is an argument of the function-like quantity on the left; its role is set by that function’s stated inputs.
Symbol k_mathrm B
athrm B is one of the signed contributions combined to compute the quantity on the left.
Symbol p
p is one of the signed contributions combined to compute the quantity on the left.
Symbol x_t
is one of the signed contributions combined to compute the quantity on the left.
=
The expressions on both sides represent the same quantity under the stated assumptions.
See an illustrated explanation →subscript
The lower label selects a particular version, component, or indexed member of the quantity. For example, x₀ and xₜ can be values at different positions.
How to interpret it
Read it with the definitions, units, and assumptions supplied by the article.
What the article says around this equation
The system’s stochastic entropy is defined from the ensemble density evaluated at the realized state, . For a single thermal bath, the medium entropy change is related to dissipated heat, subject to sign convention, and total entropy combines system and medium contributions. This allows every observed path to receive a thermodynamic accounting while preserving the distinction between a random trajectory-level quantity and its ensemble expectation [ 4 ] .
Sources cited in the surrounding passage
These citations give research context. Read each source to check which claims it supports.
Return to The Statistical Mechanics of Irreversibility at Molecular Scale