Collision frequency

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:[1]

Z = N A N B σ AB 8 k B T π μ AB , {\displaystyle Z=N_{\text{A}}N_{\text{B}}\sigma _{\text{AB}}{\sqrt {\frac {8k_{\text{B}}T}{\pi \mu _{\text{AB}}}}},}

which has units of [volume][time]−1.

Here,

  • N A {\displaystyle N_{\text{A}}} is the number of A molecules in the gas,
  • N B {\displaystyle N_{\text{B}}} is the number of B molecules in the gas,
  • σ AB {\displaystyle \sigma _{\text{AB}}} is the collision cross section, the "effective area" seen by two colliding molecules, simplified to σ AB = π ( r A + r B ) 2 {\displaystyle \sigma _{\text{AB}}=\pi (r_{\text{A}}+r_{\text{B}})^{2}} , where r A {\displaystyle r_{\text{A}}} the radius of A and r B {\displaystyle r_{\text{B}}} the radius of B.
  • k B {\displaystyle k_{\text{B}}} is the Boltzmann constant,
  • T {\displaystyle T} is the temperature,
  • μ AB {\displaystyle \mu _{\text{AB}}} is the reduced mass of the reactants A and B, μ AB = m A m B m A + m B {\displaystyle \mu _{\text{AB}}={\frac {{m_{\text{A}}}{m_{\text{B}}}}{{m_{\text{A}}}+{m_{\text{B}}}}}}

Collision in diluted solution

In the case of equal-size particles at a concentration n {\displaystyle n} in a solution of viscosity η {\displaystyle \eta } , an expression for collision frequency Z = V ν {\displaystyle Z=V\nu } where V {\displaystyle V} is the volume in question, and ν {\displaystyle \nu } is the number of collisions per second, can be written as:[2]

ν = 8 k B T 3 η n , {\displaystyle \nu ={\frac {8k_{\text{B}}T}{3\eta }}n,}

Where:

  • k B {\displaystyle k_{B}} is the Boltzmann constant
  • T {\displaystyle T} is the absolute temperature (unit K)
  • η {\displaystyle \eta } is the viscosity of the solution (pascal seconds)
  • n {\displaystyle 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 ν {\displaystyle \nu } .[2]

References

  1. ^ chem.libretexts.org: Collision Frequency
  2. ^ a b Debye, P. (1942). "Reaction Rates in Ionic Solutions". Transactions of the Electrochemical Society. 82 (1): 265. doi:10.1149/1.3071413. ISSN 0096-4743.