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:
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:
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.