← Back to article

Equation 1 · Three Ways to Measure a System That Refuses to Settle Down

What does this equation mean?

⟨e−βW⟩=e−βΔF\left\langle e^{-\beta W} \right\rangle = e^{-\beta \Delta F}

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.

Inputs and operationse^-β Δ F
Result or conditionlangle e^-β W rangle
How to read the two sides of this formula. Follow the article passage for the meaning of each quantity.

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

e−βWe^{-\beta W}

Symbol e^-β W

e−e^-β W is part of the quantity the equation computes from the expression on the right.

Understand this part →

e−βΔFe^{-\beta \Delta F}

Symbol e^-β Δ F

e−e^-β Δ F is one of the signed contributions combined to compute the quantity on the left.

Understand this part →

=

=

The expressions on both sides represent the same quantity under the stated assumptions.

Understand this part →

See an illustrated explanation →
change

change

Capital delta attached to a quantity marks a difference between two values of that quantity; the article’s sign convention determines the order.

Understand this part →

superscript

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.

Understand this part →

See an illustrated explanation →

How to interpret it

Read it with the definitions, units, and assumptions supplied by the article.

What the article says around this equation

Because these three frameworks share vocabulary, it is worth being explicit about the one place where a formal expression clarifies rather than decorates the comparison: the Jarzynski equality itself. Written compactly, it states ⟨e−βW⟩=e−βΔF\left\langle e^{-\beta W} \right\rangle = e^{-\beta \Delta F}. where W is the work performed on the system along a single nonequilibrium trajectory, Δ\Delta F is the equilibrium free-energy difference between the initial and final states, and β\beta is inverse temperature. The average on the left is taken over repeated realizations of the same driving protocol, each of which can dissipate a different amount of work due to thermal fluctuations. The identity holds exactly regardless of how fast or far from…
Read the full surrounding passage
Because these three frameworks share vocabulary, it is worth being explicit about the one place where a formal expression clarifies rather than decorates the comparison: the Jarzynski equality itself. Written compactly, it states ⟨e−βW⟩=e−βΔF\left\langle e^{-\beta W} \right\rangle = e^{-\beta \Delta F}. where W is the work performed on the system along a single nonequilibrium trajectory, Δ\Delta F is the equilibrium free-energy difference between the initial and final states, and β\beta is inverse temperature. The average on the left is taken over repeated realizations of the same driving protocol, each of which can dissipate a different amount of work due to thermal fluctuations. The identity holds exactly regardless of how fast or far from equilibrium the driving protocol runs, which is precisely what makes it usable on single-molecule pulling experiments where the process is never quasi-static. Jensen’s inequality applied to the same average recovers the ordinary second-law statement that mean dissipated work is non-negative, $⟨\langle W ⟩\rangle ≥\geq Δ\Delta F$, showing directly why the equality is a refinement of the second law rather than a challenge to it. No comparable single equation captures the entropy-production framework or large-deviation theory as cleanly for a general audience, because the former is defined at the level of an entire trajectory ensemble with system-specific rate matrices, and the latter is defined by an asymptotic scaling limit rather than a single closed-form identity; both are better conveyed through what they compute and what they require than through their governing equations.

Read the equation in its article →

For background, read the article’s source list.

Return to Three Ways to Measure a System That Refuses to Settle Down

See this formula across 1 published context →

Browse the mathematical compendium →