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Equation 22 · Part 3 · The Statistical Mechanics of Irreversibility at Molecular Scale

fraction

Var⁡(Jτ)⟨Jτ⟩2≥2⟨Στ⟩.\frac{\operatorname{Var}(J_\tau)}{\langle J_\tau\rangle^2} \ge \frac{2}{\langle\Sigma_\tau\rangle}.
fraction

What this part means

Divide the expression above the line by the one below it.

Its job in the formula

The expression above the fraction bar is divided by the complete expression below it. The denominator must not be zero.

The passage around this formula

A molecular clock or motor is useful not only when its average current is nonzero but when that current is sufficiently precise. Let JτJ_\tau be an integrated current observed for time τ\tau , such as net molecular steps or transported ions. Define dimensionless mean entropy production ⟨\langleΣτ\Sigma_\tau⟩\rangle=⟨\langleΔ\Delta stots_{\mathrm{tot}}⟩\rangle/kBk_{\mathrm B} . A canonical steady-state thermodynamic uncertainty relation has the form Var⁡(Jτ)⟨Jτ⟩2≥2⟨Στ⟩\frac{\operatorname{Var}(J_\tau)}{\langle J_\tau\rangle^2} \ge \frac{2}{\langle\Sigma_\tau\rangle}. The relation says that suppressing relative current fluctuations requires dissipation. Barato and Seifert introduced this precision–cost connection for biomolecular processes [ 5 ] , and later large-deviation results established broad bounds…

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A fraction a/b means a divided by b. The top number is the numerator; the bottom number is the denominator, and it cannot be zero.

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