Calculating the equilibrium distance

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SUMMARY

The discussion centers on calculating the equilibrium distance (h_o) between a sphere and a plane under Van der Waals (VDW) forces, represented by the Hammaker equation F = Aa/6h^2. Participants emphasize that as the gap (h) approaches zero, the force (F) cannot tend to infinity, indicating the presence of repulsive forces at very small separations. The conversation highlights the importance of surface roughness and its impact on adhesion, suggesting that true adhesion occurs at contact, where attractive VDW forces balance repulsive forces from surface electrons. The equilibrium distance is typically on the order of angstroms, complicating assumptions about air flow in such small gaps.

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  • Understanding of Van der Waals forces and their mathematical representation
  • Familiarity with the Hammaker constant and its role in adhesion
  • Knowledge of surface roughness and its effect on effective surface area
  • Basic principles of electromechanics and fluid dynamics at low Reynolds numbers
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  • Research the derivation of the Hammaker force equation and its implications
  • Study the effects of surface roughness on adhesion in micro-scale interactions
  • Explore the relationship between adhesion, traction, and friction in particle systems
  • Investigate the behavior of fluids in micro-scale gaps, particularly at low Reynolds numbers
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Researchers and students in materials science, mechanical engineering, and physics, particularly those focusing on adhesion phenomena and micro-particle interactions in electromechanical systems.

Clausius2
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Hi there,

Let's imagine a sphere touching a plane. Then, I may consider valid the law for adhesion coming from VDW forces:

F=\frac{Aa}{6h^2}

where A is the Hammaker constant, a is the sphere radius and h is the gap between the two bodies. My question is, is there a way of calculating the equilibrium distance h_o where the force reaches its maximum? What cannot be is that as h tends to zero F tends to infinity. There must be some point of equilibrium for very small h in which maybe repulsion forces start to take place. Is that right?
 
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I guess I'd like to see the derivation of this formula.

F clearly cannot go to infinite.

What bothers me is "h is the gap between the two bodies." How does one achieve adhesion with a gap between bodies?

Adhesion should be a function of surface roughness, in addition to VDW. Surface roughness would affect the effective surface area involvedin VDW. And there could also be a softness (hardness) component.

Is 'adhesion' related to traction/friction?
 
Typically, in Hammaker models, the separation between particles is a center-to-center spacing and the global maximum of the inter-particle force is at "contact". By contact, one roughly means that the particles are close enough (of the order of an angstrom between surfaces) that repulsion from surface electrons equals the attractive VDW force.

Clearly, the (Hammaker) force equation provided above models only part of the forces present in the system, since it has no horizontal tangent at finite separation (ie: it provides no finite equilibrium separation).
 
Last edited:
Astronuc said:
I guess I'd like to see the derivation of this formula.

F clearly cannot go to infinite.

What bothers me is "h is the gap between the two bodies." How does one achieve adhesion with a gap between bodies?

Adhesion should be a function of surface roughness, in addition to VDW. Surface roughness would affect the effective surface area involvedin VDW. And there could also be a softness (hardness) component.

Is 'adhesion' related to traction/friction?

It is obtained integrating the interaction energy (see fundamentals of adhesion, Lee). You're right about the roughness, h models an average gap between both surfaces.

Gokul said:
Typically, in Hammaker models, the separation between particles is a center-to-center spacing and the global maximum of the inter-particle force is at "contact". By contact, one roughly means that the particles are close enough (of the order of an angstrom between surfaces) that repulsion from surface electrons equals the attractive VDW force.

Clearly, the (Hammaker) force equation provided above models only part of the forces present in the system, since it has no horizontal tangent at finite separation (ie: it provides no finite equilibrium separation).

Yeah, I did a little of research and I found that the equilibrium distance is usually of order of angstroms. What bothers me now is that I couldn't assume Continuum flow of air in such a small gap.

Thanks guys.
 
Just to satisfy my curiosity, what is the system you are trying to model?
 
Gokul43201 said:
Just to satisfy my curiosity, what is the system you are trying to model?

No problem. Actually, it is for my thesis. About Electromechanics of Particles, in particular I'm looking now at a micro particle near a wall at Low Reynolds Numbers. It's funny.
 

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