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Search for "fluid squeeze-out" in Full Text gives 1 result(s) in Beilstein Journal of Nanotechnology.

Single-asperity contact mechanics with positive and negative work of adhesion: Influence of finite-range interactions and a continuum description for the squeeze-out of wetting fluids

Martin H. Müser

Beilstein J. Nanotechnol. 2014, 5, 419–437, doi:10.3762/bjnano.5.50

of the finite-range attraction. The results can benefit the interpretation of atomic force microscopy in liquid environments and the modeling of multi-asperity contacts. Keywords: cohesive zone model; contact mechanics; environmental; fluid squeeze-out; nanomechanics; single-asperity contacts

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Figure 1: Geometry of the deformed tip (upper grey solid), the substrate (lower solid), and the reference tip...

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Figure 2: (a) Finite-range surface energies and (b) forces per unit area for the models investigated in this ...

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Figure 3: Scaled gap g(r) as a function of scaled distance from origin r for two different parameter realizat...

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Figure 4: Negative elastic displacement −u(r) (as defined in Figure 1) of a tip with R = E = 1 pressed against a rigi...

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Figure 5: Interfacial pressure on a free, linearly-elastic half space resting at zero external load on a rigi...

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Figure 6: Gap between a rigid, adhesive, parabolic tip and a linearly-elastic half space for two different Ta...

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Figure 7: Pressure p(r) in the Gauss model at zero load for two different Tabor coefficients as a function of...

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Figure 8: Gap g(r) in linear (a) and logarithmic (b) representation as well as (c) first derivative g′(r) for...

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Figure 9: Contact radius a_c at zero external load as a function of the Tabor coefficient μ_T for different mod...

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Figure 10: Normal displacement d at zero external load as a function of the Tabor coefficient μ_T for different...

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Figure 11: Contact radius a_c as a function of load F_N for the exponential and the MD model using different Tab...

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Figure 12: Normal displacement d as a function of load F_L for the exponential and the MD model using different...

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Figure 13: Relative errors in per cent for the contact radius a_c for μ_T = 1 at (a) negative and (b) positive l...

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Figure 14: Relative errors in per cent for (a) contact radius and (b) normal displacement at zero normal load....

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Figure 15: Excess contact radius Δa_c = a_c − a_p as a function of the excess load ΔF_N = F_N + F_p for different va...

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Figure 16: Contact radius a_c as a function of normal force F_N for the exponential (full symbols) and the Gauss...

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Figure 17: Contact radius a_c as a function of normal force F_N in the vicinity of the spontaneous wetting force ...

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Figure 18: Displacement d as a function of normal force F_N in the vicinity of the spontaneous wetting force F_sw...

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Figure 19: Gap g(r) as a function of the lateral distance from the origin r for a large load F_N = 60 (a) and (...

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Figure 20: Contact geometry for a Gauss model with finite-range repulsion. Arrows indicate the direction of no...

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Published 08 Apr 2014

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