4.2 Article

The search for the hydrophobic force law

Journal

FARADAY DISCUSSIONS
Volume 146, Issue -, Pages 299-308

Publisher

ROYAL SOC CHEMISTRY
DOI: 10.1039/b926184b

Keywords

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Funding

  1. Camille and Henry Dreyfus Foundation
  2. National Science Foundation [CBET-0845074]
  3. National Institutes of Health [R01 GM076709]
  4. NATIONAL INSTITUTE OF DENTAL & CRANIOFACIAL RESEARCH [R01DE018468] Funding Source: NIH RePORTER
  5. NATIONAL INSTITUTE OF GENERAL MEDICAL SCIENCES [R01GM076709] Funding Source: NIH RePORTER

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After nearly 30 years of research on the hydrophobic interaction, the search for the hydrophobic force law is still continuing. Indeed, there are more questions than answers, and the experimental data are often quite different for nominally similar conditions, as well as, apparently, for nano-, micro-, and macroscopic surfaces. This has led to the conclusion that the experimentally observed force distance relationships are either a combination of different 'fundamental' interactions, or that the hydrophobic force-law, if there is one, is complex - depending on numerous parameters. The only unexpectedly strong attractive force measured in all experiments so far has a range of D approximate to 100-200 angstrom, increasing roughly exponentially down to similar to 10-20 angstrom and then more steeply down to adhesive contact at D = 0 or, for power-law potentials, effectively at D approximate to 2 angstrom. The measured forces in this regime (100-200 angstrom) and especially the adhesive forces are much stronger, and have a different distance-dependence from the continuum VDW force (Lifshitz theory) for non-conducting dielectric media. We suggest a three-regime force-law for the forces observed between hydrophobic surfaces: In the first, from 100-200 angstrom to thousands of angstroms, the dominating force is created by complementary electrostatic domains or patches on the apposing surfaces and/or bridging vapour cavities; a 'pure' but still not well-understood 'long-range hydrophobic force' dominates the second regime from similar to 150 to similar to 15 angstrom, possibly due to an enhanced Hamaker constant associated with the 'proton-hopping' polarizability of water; while below similar to 10-15 angstrom to contact there is another 'pure short-range hydrophobic force' related to water structuring effects associated with surface-induced changes in the orientation and/or density of water molecules and H-bonds at the water hydrophobic interface. We present recent SFA and other experimental results, as well as a simplified model for water based on a spherically-symmetric potential that is able to capture some basic features of hydrophobic association. Such a model may be useful for theoretical studies of the HI over the broad range of scales observed in SFA experiments.

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