Diffusion-controlled reaction

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Diffusion-controlled (or diffusion-limited) reactions are reactions in which the reaction rate is equal to the rate of transport of the reactants through the reaction medium (usually a solution).[1] The process of chemical reaction can be considered as involving the diffusion of reactants until they encounter each other in the right stoichiometry and form an activated complex which can form the product species. The observed rate of chemical reactions is, generally speaking, the rate of the slowest or "rate determining" step. In diffusion controlled reactions the formation of products from the activated complex is much faster than the diffusion of reactants and thus the rate is governed by collision frequency.

Diffusion control is rare in the gas phase, where rates of

Heterogeneous reactions
where reactants are in different phases are also candidates for diffusion control.

One classical test for diffusion control of a heterogeneous reaction is to observe whether the rate of reaction is affected by stirring or agitation; if so then the reaction is almost certainly diffusion controlled under those conditions.

Derivation

The following derivation is adapted from Foundations of Chemical Kinetics.[2] This derivation assumes the reaction . Consider a sphere of radius , centered at a spherical molecule A, with reactant B flowing in and out of it. A reaction is considered to occur if molecules A and B touch, that is, when the distance between the two molecules is apart.

If we assume a local steady state, then the rate at which B reaches is the limiting factor and balances the reaction.

Therefore, the steady state condition becomes

1.

where

is the flux of B, as given by

Fick's law of diffusion
,

2. ,

where is the diffusion coefficient and can be obtained by the

Stokes-Einstein equation
, and the second term is the gradient of the chemical potential with respect to position. Note that [B] refers to the average concentration of B in the solution, while [B](r) is the "local concentration" of B at position r.


Inserting 2 into 1 results in

3. .

It is convenient at this point to use the identity allowing us to rewrite 3 as


4. .

Rearranging 4 allows us to write

5.

Using the boundary conditions that , ie the local concentration of B approaches that of the solution at large distances, and consequently , as , we can solve 5 by separation of variables, we get

6. or

7. (where : )

For the reaction between A and B, there is an inherent reaction constant , so . Substituting this into 7 and rearranging yields

8.

Limiting conditions

Very fast intrinsic reaction

Suppose is very large compared to the diffusion process, so A and B react immediately. This is the classic diffusion limited reaction, and the corresponding diffusion limited rate constant, can be obtained from 8 as . 8 can then be re-written as the "diffusion influenced rate constant" as

9.

Weak intermolecular forces

If the forces that bind A and B together are weak, ie for all r except very small r, . The reaction rate 9 simplifies even further to

10. This equation is true for a very large proportion of industrially relevant reactions in solution.

Viscosity dependence

The

Stokes-Einstein
equation describes a frictional force on a sphere of diameter as where is the viscosity of the solution. Inserting this into 9 gives an estimate for as , where R is the gas constant, and is given in centipoise. For the following molecules, an estimate for is given:

Solvents and
Solvent Viscosity (
centipoise
)
n-Pentane
0.24 27
Hexadecane 3.34 1.9
Methanol 0.55 11.8
Water 0.89 7.42
Toluene 0.59 11

[3]

See also

  • Diffusion limited enzyme

References

  1. ^ Atkins, Peter (1998). Physical Chemistry (6th ed.). New York: Freeman. pp. 825–8.
  2. ^ Roussel, Marc R. "Lecture 28:Diffusion-influenced reactions, Part I" (PDF). Foundations of Chemical Kinetics. University of Lethbridge (Canada). Retrieved 19 February 2021.
  3. ^ Berg, Howard, C. Random Walks in Biology. pp. 145–148.{{cite book}}: CS1 maint: multiple names: authors list (link)