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In the thermodynamic treatment of JKR (Ref. 1) and the energy balance of Frenkel (Ref. 5) there is no direct assumption regarding the nature of the forces. However, an attractive force field across a gap is clearly implied by JKR in their assumed deformation modes
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In the thermodynamic treatment of JKR (Ref. 1) and the energy balance of Frenkel (Ref. 5) there is no direct assumption regarding the nature of the forces. However, an attractive force field across a gap is clearly implied by JKR in their assumed deformation modes.
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Note a possible inconsistency in this picture: a sharp cusp implies an infinite curvature and hence infinite traction. This is resolved by resolved by the fact that the total force obtained by integrating around the cusp is finite (Ref. 55) and is accounted for in the numerical analysis
-
Note a possible inconsistency in this picture: a sharp cusp implies an infinite curvature and hence infinite traction. This is resolved by resolved by the fact that the total force obtained by integrating around the cusp is finite (Ref. 55) and is accounted for in the numerical analysis.
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