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Collision frequency describes the rate of collisions between two atomic or molecular species in a given volume, per unit time. In an ideal gas, assuming that the species behave like hard spheres, the collision frequency between entities of species A and species B is:chem.libretexts.org: Collision Frequency
/ref> : Z = N_\text N_\text \sigma_\text \sqrt\frac, SI unit of ''Z'' is the volumetric collision rate (unit m3⋅s−1). where: * N_\text is the number of A molecules in the gas, * N_\text is the number of B molecules in the gas, * \sigma_\text is the collision cross section (unit m2), the area when two molecules collide with each other, simplified to \sigma_\text = \pi(r_\text+r_\text)^2 , where r_\text the radius of A and r_\text the radius of B. * k_\text is the Boltzmann constant (unit m2⋅kg⋅s−2⋅K−1), * T is the temperature (unit K), * \mu_\text is the reduced mass of the reactants A and B, \mu_\text = \frac (unit kg)


Collision in diluted solution

Collision in diluted gas or liquid solution is regulated by diffusion instead of direct collisions, which can be calculated from
Fick's laws of diffusion Fick's laws of diffusion describe diffusion and were derived by Adolf Fick in 1855. They can be used to solve for the diffusion coefficient, . Fick's first law can be used to derive his second law which in turn is identical to the diffusion equ ...
. In the case of equal-size particles at a concentration n in a solution of viscosity \eta , an expression for collision frequency \nu=ZV where V is the volume in question, and \nu is the number of collisions per second, can be written as: : \nu = \frac{3 \eta} n, Where: * k_B is the Boltzmann constant * T is the absolute temperature (unit K) * \eta is the viscosity of the solution (pascal seconds) * n is the concentration of particles per cm3 Here the frequency is independent of particle size, a result noted as counter-intuitive. For particles of different size, more elaborate expressions can be derived for estimating \nu.


References

Chemical kinetics