Tribocharging Model

The Tribocharging contact model allows you to simulate a change of charge of particles within a material after they come into contact with a different material.

For repeated contacts, a saturation charge level is reached which is a function of both charge generation and dissipation processes. In most ESD (electrostatic discharge) problems, triboelectrification is the prime charge generation process.

You must first specify the work function. Tribocharging (triboelectric charging) will occur if the work functions of two materials differ. There will not be a charge transfer if the work functions remain the same.

The following equation is based on work by Greason (2000) and describes the change in charge:

dqdt=α(qsq)βq

Where q is a charge of a sphere at time t, α and β are the time constants of the charge generation and dissipation respectively. α is in the range of 0.02–0.085 s-1 for polymers and in the range 0.002–0.005 s-1 for metals. β is neglected in calculations because charge dissipation through atmospheric ion impingement is slow (Hogue, et al. 2007).

And qs is a saturation charge defined as:

qs=σAs

Where σ is a surface charge density which is approximately equal to 2.66e-5 cm-2 for air standard pressure and temperature, and As is the surface area of a particle.