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Published equation contexts

r∝exp⁡ ⁣(−Ea(ΔEbind)kBT)r \propto \exp\!\left(-\frac{E_a(\Delta E_{\text{bind}})}{k_B T}\right)

Why this formula appears here

A catalyst does its work by opening a lower-energy pathway between reactants and products — typically by binding an intermediate, weakening a bond that would otherwise need more thermal energy to break, and then releasing the product so the surface is free for another cycle. The energetics of that binding step follow a well-established shape: bind too weakly and the reactant never activates; bind too strongly and the product never leaves. Plotted against binding energy, catalytic activity for a given reaction traces an inverted-U — the Sabatier principle — and the best catalysts sit as close as possible to the peak. Here the activation energy EaE_a is itself a function of the binding energy…

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rr

Symbol r

r is a part of this expression. Its role is fixed by the surrounding article and by the operations shown in the formula.

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EaE_a

Symbol E_a

itself a function of the binding energy Δ\Delta EbindE_{\text{bind}} , so tuning a catalyst is really tuning where on that curve a given surface sits — through composition, structure, and the local electronic environment around active sites.

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ΔEbind\Delta E_{\text{bind}}

Symbol Δ E_bind

Δ EbE_bind occurs above the fraction bar. The numerator is divided by the entire denominator below it.

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kBk_B

Symbol k_B

kBk_B occurs below the fraction bar. The quantity above the bar is divided by this expression; zero is excluded as a denominator.

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TT

Symbol T

T occurs below the fraction bar. The quantity above the bar is divided by this expression; zero is excluded as a denominator.

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Ea(ΔEbind)E_a(\Delta E_{\text{bind}})

Numerator: E_a(Δ E_bind)

The complete quantity above the fraction bar.

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How to interpret it

With a fixed numerator, increasing a nonzero denominator reduces the fraction.

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Published contexts (1)

A symbol can carry a different meaning in another article. Each occurrence keeps its own guide and term definitions.

r∝exp⁡ ⁣(−Ea(ΔEbind)kBT)r \propto \exp\!\left(-\frac{E_a(\Delta E_{\text{bind}})}{k_B T}\right)

Equation 1 · Chemistry

Chemical Dynamics and Catalysis in 2035: Scenarios, Signals, and Falsifiable Predictions

This mathematical expression combines the displayed quantities; its precise role follows from the surrounding article text.

A catalyst does its work by opening a lower-energy pathway between reactants and products — typically by binding an intermediate, weakening a bond that would otherwise need more thermal energy to break, and then releasing the product so the surface is free for another cycle. The energetics of that binding step follow a well-established shape: bind too weakly and the reactant never activates; bind too strongly and the product never leaves. Plotted against binding energy, catalytic activity for a given reaction traces an inverted-U — the Sabatier principle — and the best catalysts sit as close as possible to the peak. Here the activation energy EaE_a is itself a function of the binding energy…

Meanings in this article

  • EaE_a: itself a function of the binding energy Δ\Delta EbindE_{\text{bind}} , so tuning a catalyst is really tuning where on that curve a given surface sits — through composition, structure, and the local electronic environment around active sites.
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