Equation 13 · 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 e^-β W
β W is part of the quantity the equation computes from the expression on the right.
Symbol e^-βΔ F
βΔ F is one of the signed contributions combined to compute the quantity on the left.
Symbol β
β is part of the quantity the equation computes from the expression on the right.
Symbol k_mathrm B
athrm B occurs below the fraction bar. The quantity above the bar is divided by this expression; zero is excluded as a denominator.
Symbol T
T occurs below the fraction bar. The quantity above the bar is divided by this expression; zero is excluded as a denominator.
=
The expressions on both sides represent the same quantity under the stated assumptions.
See an illustrated explanation →change
Capital delta attached to a quantity marks a difference between two values of that quantity; the article’s sign convention determines the order.
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.
superscript
A raised number can be a power. When it is a label or bound, it selects a case or the upper limit of a sum; the formula’s structure distinguishes these uses.
See an illustrated explanation →Denominator: k_mathrm BT
The complete quantity below the fraction bar; it must be nonzero for this division.
How to interpret it
With a fixed numerator, increasing a nonzero denominator reduces the fraction. Read it with the definitions, units, and assumptions supplied by the article.
What the article says around this equation
In equilibrium statistical mechanics, the free-energy difference F between two control-parameter values is a state function. A rapid drive between them generally performs work W> F on average because dissipation is positive. It would seem that estimating F requires an impractically slow, quasistatic protocol. The Jarzynski equality demonstrates otherwise: . The equality holds for an ensemble of realizations beginning in equilibrium, even when each realization is driven far from equilibrium [ 2 ] . It does not say that the arithmetic mean work equals the free-energy difference. The exponential average disproportionately weights rare, low-work…
Read the full surrounding passage
In equilibrium statistical mechanics, the free-energy difference F between two control-parameter values is a state function. A rapid drive between them generally performs work W> F on average because dissipation is positive. It would seem that estimating F requires an impractically slow, quasistatic protocol. The Jarzynski equality demonstrates otherwise: . The equality holds for an ensemble of realizations beginning in equilibrium, even when each realization is driven far from equilibrium [ 2 ] . It does not say that the arithmetic mean work equals the free-energy difference. The exponential average disproportionately weights rare, low-work trajectories. That feature makes the theorem exact and can make its estimator statistically difficult: if the trajectories that dominate the exponential average are poorly sampled, finite-data estimates are biased.
Sources cited in the surrounding passage
These citations give research context. Read each source to check which claims it supports.
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