The secondary minimum in a classical DLVO potential curve is often at a relatively large surface-to-surface (or center-to-center) inter-particle distance.
My question is: How can particles trapped in a secondary potential well be reversibly agglomerated (i.e., held together by weak forces in a flocculated state) despite being at a non-zero inter-particle separation distance? Doesn't agglomeration require the surface-to-surface separation to be zero (i.e., contact between particles) in order to take place? In other words, how would two flocculated particles look like when trapped in a secondary minimum?