Hamaker constant

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In

H. C. Hamaker) is a physical constant that can be defined for a van der Waals
(vdW) body–body interaction:

where ρ1, ρ2 are the number densities of the two interacting kinds of particles, and C is the London coefficient in the particle–particle pair interaction.[1][2] The magnitude of this constant reflects the strength of the vdW-force between two particles, or between a particle and a substrate.[1]

The Hamaker constant provides the means to determine the interaction parameter C from the vdW-pair potential,

Hamaker's method and the associated Hamaker constant ignores the influence of an intervening medium between the two particles of interaction. In 1956

dielectric properties of this intervening medium (often a continuous phase).[3]

The

Van der Waals forces are effective only up to several hundred angstroms
. When the interactions are too far apart, the dispersion potential decays faster than this is called the
Casimir–Polder force
.

See also

References

  1. ^ .
  2. .
  3. ^ Lifshitz, E.M. (1956). "The Theory of Molecular Attractive Forces between Solids". Soviet Journal of Experimental and Theoretical Physics. 2: 73–83.