A Curious Antipathy for Water Hydrophobicity but Few Agree on the Details
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PERSPECTIVES apparent change in angular direction to a dis- numbers of objects, a critical precondition for matic advances are anticipated, with the com- tant object as Earth orbits the Sun during a year accurate mass and orbit determinations. bination of the LHC and Gaia. as a fundamental distance scale (9). Gaia pre- Dark matter is the dominant gravitating cision is an improvement on the best astrome- mass in the Universe. It is perhaps a mix of References and Notes try currently available by some 3 orders of several ingredients, with different contribu- 1. V. Springel, C. S. Frenck, S. D. M. White, Nature 440, 1137 (2006). magnitude, while its sensitivity provides an tions dominant on different scales, from the 2. V. Belokurov et al., Astrophys. J. 654, 897 (2007). improvement of 4 orders of magnitude. One of extremely small scale of weakly interacting 3. G. Gilmore et al., Astrophys. J. 663, 948 (2007). Gaia’s prime subjects will be galaxy evolution, massive particles to the very long scales of 4. M. Walker et al., Astrophys. J. 667, L53 (2007). 5. G. Gilmore, R. F. G. Wyse, K. Kuijken, Annu. Rev. Astron. including measuring the distribution of dark massive neutrinos. Disentangling this mix Astrophys. 27, 555 (1989). matter on whatever scales it is found. The tech- requires quantitative determination of the 6. S. Majewski, Annu. Rev. Astron. Astrophys. 31, 575 nically most difficult aspect of dark matter three-dimensional distribution of mass in dark (1993). 7. K. Freeman, J. Bland-Hawthorn, Annu. Rev. Astron. studies in astrophysics is precision mass mea- matter–dominated systems on astrophysical Astrophys. 40, 487 (2002). surement. Usually having access only to line- scales to complement direct detection and cre- 8. European Space Agency, Research and Scientific Support of-sight velocity data and knowing little of ation experiments on Earth. As galaxies have Department, www.rssd.esa.int/Gaia transverse velocities means that only partial been evolving for 13 billion years in real dark 9. Parallax distances are so fundamental in astronomy that the basic distance unit is the parsec (pc), the distance of information can be modeled. Gaia will provide matter halos since they became gravitationally an object that displays a parallax of one second of arc. 1 precision transverse kinematic data, thus giv- bound, quantification of the relevant astro- pc = 3.26 light-years = 3.1016 m. ing access to reliable six-dimensional phase physics is also necessary. Despite the chal- space measures of location and speed for large lenges, real progress is being made, while dra- 10.1126/science.1165790 CHEMISTRY How does water meet a hydrophobic surface? Like great art, everyone recognizes A Curious Antipathy for Water hydrophobicity but few agree on the details. on December 8, 2008 Steve Granick and Sung Chul Bae magine that you are a water molecule at a ejected spontaneously, whereas water films without friction (3). Such water-filled nan- hydrophobic (water-repellent) surface. confined between symmetric hydrophilic otubes switch from hydrophobic at room tem- IGiven the chance, you would bead up with surfaces are stable (1). perature to hydrophilic when the temperature other water molecules to form a droplet, just Hydrophobicity shows up differently in is lowered to 8°C (4), in line with predictions as water beads up on raincoats or leaves of carbon nanotubes, within which a hydrogen- that a switch of this kind can happen because plants (see the figure, left panel). But what bonded chain of water molecules can form, the free energy of a full nanotube is very close www.sciencemag.org would you do if you were inside a droplet, yet stretching like a thread down the middle of to that of an empty nanotube (2). The obser- located very near the hydrophobic surface? the nanotube (see the figure, right panel) (2). vation opens the possibility that temperature Water molecules in this situation cannot leave The unusual hydrogen-bonding geometry may one day be used as a switch to make car- the surface although they would if they could; and nonstick surface result in flow essentially bon nanotubes selectively suck up chemicals they are frustrated. Such proximity of water to a hydrophobic surface is fundamental to the so-called hydrophobic effect. Its reasons are Downloaded from disputed, as is its definition. Not in dispute is its importance. For example, the side chains of roughly half the amino acids are polar, while those of the other half are hydrophobic; the nonmixing of the two is key to steering the folding of pro- teins and other self-assembly processes (see the figure, middle panel). As a second exam- ple, the fact that oil and water hardly mix is at the root of the self-assembly of supramolec- ular structures known as cell membranes (in biology) and micelles (in technology), where the self-assembling molecules contain both How water meets different hydrophobic elements. (Left) On flat planar self-assembled monolayers, the situation is simplest: The contact angle is high when the monolayer is terminated uniformly with CF groups, nonpolar and polar moieties. Furthermore, 3 when the gap between two hydrophobic and zero when it is terminated uniformly with OH groups. (Middle) The situation is more complex on the sur- face of a protein, α-chymotrypsin in this example. Hydrophobicity of the amino acid residues is weaker than surfaces becomes critically small, water is in the left panel, the size of the hydrophobic patch is smaller, and nothing is planar. For these reasons, the ten- dency to dewet is less than in the left panel. Water is predicted to envelop even the hydrophobic (green) patch Departments of Materials Science and Engineering, of amino acids, but likely with more fluctuation than at hydrophilic patches (1, 13). (Right) Water fills a car- Chemistry, and Physics, University of Illinois, Urbana, IL bon nanotube spontaneously, forming linear hydrogen-bonded threads of water running down the middle (2), CREDIT: SHEKHAR GARDE AND RAHUL GODAWAT/RENSSELAER POLYTECHNIC INSTITUTE POLYTECHNIC SHEKHAR GARDE AND RAHUL GODAWAT/RENSSELAER CREDIT: 61801, USA. E-mail: [email protected] yet the simultaneous tendency to dewet causes it to flow through the tube essentially without friction (3). www.sciencemag.org SCIENCE VOL 322 5 DECEMBER 2008 1477 Published by AAAS PERSPECTIVES like with a straw—not only water, but poten- face has the same wettability (hydrophobic or approach is to explain this in terms of the tially other solutes also (5). It also confirms hydrophilic) everywhere, or is “patchy” from hydrophobic effect (4), but it can also be the well-known weakening of hydrophobic spot to spot? Answers will bring understand- understood on the basis of more general prin- interactions upon cooling below room tem- ing in this field into closer contact with ciples of the competition between enthalpy perature (6). emerging issues in fields as diverse as protein and entropy (16). The challenge, then, is to Despite its obvious importance, physical folding and surface science. predict from theory, rather than from empiri- insight into the origins of hydrophobicity is not Second, scientists have concentrated on cism, what makes water so special. easy to come by. Thermodynamic mea- systems that are subject to steady external surements are one approach, but interpreting conditions, such as a low temperature that References and Notes their physical significance is extraordinarily causes proteins to denature. We do not yet 1. X. Zhang, Y. Zhu, S. Granick, Science 295, 663 (2002). 2. G. Hummer, J. C. Rasaiah, J. P. Noworyta, Nature 414, subtle (6). Theoretical considerations and com- have good ways to think about how aqueous 188 (2001). puter simulations show that a key concept is the systems respond to an extreme but perhaps 3. A. Kalra, S. Garde, G. Hummer, Proc. Natl. Acad. Sci. size of the hydrophobic object (7–9). Water transient change of environment. Is it realistic U.S.A. 100, 10175 (2003). molecules can wrap efficiently around hydro- to expect a general theory of hydrophobic sur- 4. H.-J. Wang, X.-K. Xi, A. Kleinhammes, Y. Wu, Science 322, 80 (2008). phobic elements with a radius of curvature of faces when temperature and pressure change 5. A. Kalra, G. Hummer, S. Garde, J. Phys. Chem. B 108, 1 nm or less. When water meets hydrophobic in time and space? Empiricism shows that 544 (2004). surfaces that are flatter than this, it forms a what matters is not just the instantaneous sep- 6. D. Ben-Amotz, B. Widom, J. Phys. Chem. B 110, 19839 (2006). molecularly thin cushion of depleted density aration between hydrophobic surfaces but 7. F. H. Stillinger, J. Sol. Chem. 2, 141 (1973). between it and the hydrophobic surface. also the time (or frequency) of their contact 8. K. Lum, D. Chandler, J. D. Weeks, J. Phys. Chem. B. 103, The fly in the ointment is experiment. (1); the timeline of change also matters. 4570 (1999). Putative depletion layers must fight against Third: When does water act truly unlike 9. J. Janecek, R. R. Netz, Langmuir 12, 8417 (2007). 10. A. Poynor et al., Phys. Rev. Lett. 97, 266101 (2006). attraction of water to any hydrophobic sur- other fluids? Spectroscopic studies of vibra- 11. A. Poynor et al., Phys. Rev. Lett. 101, 039602 (2008). face, a ubiquitous force known as van der tions in water molecules are a technical tour 12. M. Mezger et al., J. Chem. Phys. 128, 244705 (2008). Waals attraction. This is probably why labora- de force but are problematic to interpret (15). 13. K. Kashimoto et al., Phys. Rev. Lett. 101, 076102 tory data have provided evidence both for Prevalent computational models use point (2008). 14. D. Chandler, Nature 437, 640 (2005). on December 8, 2008 [(10, 11) and references therein; (12)] and charges and do not explicitly recognize quan- 15.