Volume Spring Model

The Volume Spring contact model is an experimental model in which the normal force is proportional to the overlap volume of the two particles and does not involve the penetration depth.

This model is similar to Govender and Chen models which also use force proportional to overlap volume. In some cases, this has been found to provide enhanced stability of contacts. The form used in the EDEM implementation for the normal spring force is as follows:

f n = E * V R * MathType@MTEF@5@5@+= feaahyart1ev3aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamOzamaaBa aaleaacaWGUbaabeaakiabg2da9maalaaabaGaamyramaaCaaaleqa baGaaiOkaaaakiaadAfaaeaacaWGsbWaaWbaaSqabeaacaGGQaaaaa aaaaa@3D5B@

The damping force is calculated using the differential stiffness of the normal spring force. This is based on an analogy with the Linear Spring model, and the coefficient in this relationship is adjusted to give the correct Coefficient of Restitution for edge to face contacts. The tangential force is calculated using a tangential stiffness which has the same ratio to the differential normal stiffness as the Hertz-Mindlin model.

Note: The Volume Spring Model is available in OptionsAdditional Components Experimental Contact Models. Once enabled, the Volume Spring is displayed in the Contact Model Chain (Experimental contact models are highlighted in green).