Linear Cohesion

Cohesion modeling facilitates simulation of inter-molecular attraction forces (Van der Waals forces) between particle surfaces. For some classes of simulations, such as dry powders, these forces significantly affect the outcome and cannot be ignored.

This variant of cohesion modeling can use either of two models that are described in published literature: the Johnson-Kendall-Roberts (JKR) model [726] or the Derjaguin-Muller-Toporov (DMT) model [717].

Cohesion force between two spherical particles is expressed in both cases as:

Figure 1. EQUATION_DISPLAY
F c o h e s i o n = R min W π F
(3274)

where R min is the minimal radius of surfaces in contact, W is the work of cohesion [ J / m 2 ] , and F is a multiplication model blending factor with values as follows:

  • 3 2 for the JKR model
  • 2 for the DMT model

When the two contacting particles are non-spherical, R min in Eqn. (3274) becomes the minimum value of the two volume equivalent sphere radiuses (one for each particle).

The principal difference between JKR and DMT model formulation is the surface area where the cohesion force is acting. In the JKR model, this area is limited to direct contact, while in the DMT model it also incorporates the neck area in immediate contact proximity.