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The Hamaker constant A can be defined for a van der Waals (vdW) body–body interaction:

A=\pi ^{2}C\rho _{1}\rho _{2},

where $\rho _{1}$ and $\rho _{2}$ 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] It is named after H. C. Hamaker. 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, $w(r)=-C/r^{6}$ .

Hamaker's method and the associated Hamaker constant ignores the influence of an intervening medium between the two particles of interaction. In 1956 Lifshitz developed a description of the vdW energy but with consideration of the 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 $1/r^{6}$ ; this is called the retarded regime, and the result is a Casimir–Polder force.

References

^ ^a ^b Hamaker, H. C. (1937). "The London – van der Waals attraction between spherical particles". Physica. 4 (10): 1058–1072. doi:10.1016/S0031-8914(37)80203-7.
^ Seung-woo Lee and Wolfgang M. Sigmund (23 May 2002). "AFM study of repulsive Van der Waals forces between Teflon AF thin film and silica or alumina". Colloids and Surfaces A: Physicochemical and Engineering Aspects. 204 (1–3): 43-50. doi:10.1016/S0927-7757(01)01118-9.
^ Lifshitz, E.M. (1956). "The Theory of Molecular Attractive Forces between Solids". Soviet Journal of Experimental and Theoretical Physics. 2: 73–83.

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[:0-1] Hamaker, H. C. (1937). "The London – van der Waals attraction between spherical particles". Physica. 4 (10): 1058–1072. doi:10.1016/S0031-8914(37)80203-7.

[2] Seung-woo Lee and Wolfgang M. Sigmund (23 May 2002). "AFM study of repulsive Van der Waals forces between Teflon AF thin film and silica or alumina". Colloids and Surfaces A: Physicochemical and Engineering Aspects. 204 (1–3): 43-50. doi:10.1016/S0927-7757(01)01118-9.

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

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 The Hamaker constant  provides the means to determine the interaction parameter ''C'' from the vdW-pair potential, <math>w(r) = -C/r^6</math>.
-Hamaker's method and the associated Hamaker constant ignores the influence of an intervening medium between the two particles of interaction. In the 1950s [[E. M. Lifshitz|Lifshitz]] developed a description of the vdW energy but with consideration of the dielectric properties of this intervening medium (often a continuous phase).
+Hamaker's method and the associated Hamaker constant ignores the influence of an intervening medium between the two particles of interaction. In 1956 [[E. M. Lifshitz|Lifshitz]] developed a description of the vdW energy but with consideration of the dielectric properties of this intervening medium (often a continuous phase)<ref>{{Cite journal |last=Lifshitz |first=E.M. |date=1956 |title=The Theory of Molecular Attractive Forces between Solids |journal=Soviet Journal of Experimental and Theoretical Physics |volume=2 |pages=73-83}}</ref>.
 The [[Van der Waals forces]] are effective only up to several hundred [[angstrom]]s. When the interactions are too far apart, the dispersion potential decays faster than <math>1/r^6</math>; this is called the [[Retarded potential|retarded]] regime, and the result is a [[Casimir–Polder force]].

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Revision as of 19:38, 28 February 2022

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