Journal of Chemical Physics
The Journal of Chemical Physics
Search:
   
 
 
 
Previous Article
Kinetic phase diagram for CO oxidation on Pt(210): Pattern formation in the hysteresis and oscillation regions
The reactive behavior of catalytic CO oxidation on Pt(210) is studied by means of combined reaction rate measurements and photoelectron emission microscopy (PEEM). These methods allow an investigation...
Next Article
The role of structural changes in the excitation of chemical waves in the system Rh(110)/NO+H2
Previous investigations have demonstrated that the formation of chemical waves in the NO+H2 reaction on Rh(110) involves a cyclic transformation of the surface structure via various N,O-induced recons...

Structure and solvation forces in confined films: Linear and branched alkanes

J. Chem. Phys. 106, 4309 (1997); doi:10.1063/1.473132

Issue Date: 8 March 1997

You are not logged in to this journal. Log in

Jianping Gao, W. D. Luedtke, and Uzi Landman
School of Physics, Georgia Institute of Technology, Atlanta, Georgia 30332
Equilibrium structures, solvation forces, and conformational dynamics of thin confined films of n-hexadecane and squalane are investigated using a new grand canonical ensemble molecular dynamics method for simulations of confined liquids. The method combines constant pressure simulations with a computational cell containing solid surfaces and both bulk and confined liquid regions in equilibrium with each other. For both molecular liquids layered density oscillations in the confined films are found for various widths of the confining gap. The solvation force oscillations as a function of the gap width for the straight chain n-hexadecane liquid are more pronounced exhibiting attractive and repulsive regions, while for the branched alkane the solvation forces are mostly repulsive, with the development of shallow local attractive regions for small values of the gap width. Furthermore, the nature of the transitions between well-formed layered configurations is different in the two systems, with the n-hexadecane film exhibiting solid-like characteristics portrayed by step-like variations in the number of confined segments occurring in response to a small decrease in the gap width, starting from well-layered states of the film. On the other hand the behavior of the squalane film is liquid-like, exhibiting a monotonic continuous decrease in the number of confined segments as the gap width is decreased. These characteristics are correlated with structural properties of the confined films which, for n-hexadecane, exhibit enhanced layered ordering and in-plane ordered molecular arrangements, as well as with the relatively high tendency for interlayer molecular interdigitation in the squalane films. Reduced conformational (trans-guache) transition rates in the confined films, compared to their bulk values, are found, and their oscillatory dependence on the degree of confinement is analyzed, showing smaller transition rates for the well-formed layered states of the films. ©1997 American Institute of Physics.
History: Received 1 November 1996; accepted 4 December 1996
Permalink: http://link.aip.org/link/?JCPSA6/106/4309/1
BUY THIS ARTICLE   (US$24)
Download PDF (1769 kB) View Cart

KEYWORDS and PACS

Keywords
PACS
  • 82.30.Nr
    Physical Chemistry Specific chemical reactions; reaction mechanisms Association, addition, insertion, cluster formation, hydrogen bonding
  • 02.70.Ns
    Mathematical methods in physics Computational techniques Molecular dynamics and particle methods
  • 61.20.Ja
    Structure of solids and liquids; crystallography Structure of liquids Computer simulation of liquid structure
  • YEAR: 1996-97

PUBLICATION DATA

ISSN:
0021-9606 (print)   1089-7690 (online)
Publisher:
AIP is a member of CrossRef AIP

REFERENCES (44)

For access to fully linked references, you need to log in. For access to fully linked references, you need to Log in.
  1. For a recent review see, B. Bhushan, J. N. Israelachvili, and U. Landman, Nature 374, 607 (1995).
  2. Fundamentals of Friction: Macroscopic and Microscopic Processes, edited by I. L. Singer and H. M. Pollock (Kluwer, Dordrecht, 1992).
  3. Physics of Sliding Friction, edited by B. N. J. Persson and E. Tosatti (Kluwer, Dordrecht, 1996).
  4. Handbook of Micro/Nano Tribology, edited by B. Bhushan (CRC, Boca Raton, Florida, 1995).
  5. See articles in Langmuir 12, 4481–4609 (1996).
  6. See U. Landman, W. D. Luedtke, and E. M. Ringer in Ref. 2, p. 463.
  7. U. Landman, W. D. Luedtke, and J. Gao, Langmuir 12, 4514 (1996).
  8. M. Robbins and E. D. Smith, Langmuir 12, 4543 (1996).
  9. M. D. Perry and J. A. Harrison, Langmuir 12, 4552 (1996).
  10. H. T. Davis, Statistical Mechanics of Phases, Interfaces and Thin Films (VCH, New York, 1996).
  11. J. N. Israelachvili, Intermolecular and Surface Forces, 2nd ed. (Academic, New York, 1992).
  12. B. N. J. Persson, Sliding Friction (Springer, Berlin, 1997).
  13. P. B. Babuena, D. Berry, and K. E. Gubbins, J. Phys. Chem. 97, 937 (1993).
  14. K. Walley, K. S. Schweizer, J. Peanasky, L. Cai, and S. Granick, J. Phys. Chem. 100, 3361 (1994).
  15. M. Urbakh, L. Daikhin, and J. Klafter, J. Chem. Phys. 103, 10 707 (1995);
  16. M. G. Rozman, M. Urbakh, and J. Klafter, Phys. Rev. Lett. 77, 683 (1996).
  17. (a) C. L. Rhykerd, Jr., M. S. Schoen, D. Diester, and J. Cushman, Nature 330, 461 (1987), see citations 38–41 cited in Ref. 1;
  18. (b) U. Landman, W. D. Luedtke, and M. W. Ribarsky, J. Vac. Sci. Technol. A 7, 2829 (1989).
  19. J. N. Israelachvili and R. G. Horn, J. Chem. Phys. 35, 1400 (1981).
  20. S. Granick, A. L. Demirel, L. L. Cai, and J. Peanasky, Isr. J. Chem. 35, 75 (1995).
  21. J. Klein and E. Kumacheva, Science 269, 816 (1995).
  22. H. K. Christenson, D. W. R. Gruen, R. G. Horn, and J. N. Israelachvili, J. Chem. Phys. 87, 1834 (1987).
  23. M. W. Ribarsky and U. Landman, J. Chem. Phys. 97, 1937 (1992), and references therein.
  24. (a) U. Landman, W. D. Luedtke, J. Ouyang, and T. K. Xia, Jpn. J. Appl. Phys. 32, 1444 (1993);
  25. (b) W. D. Luedtke and U. Landman, Comput. Mater. Sci. 1, 1 (1992).
  26. U. Landman and W. D. Luedtke, MRS Bull. 17, 36 (1993).
  27. S. Gupta, D. C. Koopman, G. B. Westerman-Clark, and I. A. Bitsanis, J. Chem. Phys. 100, 8444 (1994).
  28. E. Manias, G. Hadziioannou, and G. ten Brinke, Langmuir 12, 4587 (1996).
  29. J. N. Israelachvili, S. J. Kott, M. Gee, and T. A. Witten, Macromolecules 22, 4247 (1989).
  30. M. L. Gee and J. N. Israelachvili, J. Chem. Soc. Faraday Trans. (2) 86, 4049 (1990).
  31. For simulations of confined alkanes with a single pendant methyl, where force oscillations similar to those found for the corresponding straight chain alkanes, see: (a) Y. Yang, K. Hill, and J. G. Harris, J. Chem. Phys. 100, 3276 (1994);
  32. (b) J. Ouyang, Ph.D. dissertation, Georgia Institute of Technology, 1995;
    J. Ouyang, W. D. Luedtke, and U. Landman, Bull. Am. Phys. Soc. 40, 425 (1995).
  33. J. N. Israelachvili (private communication).
  34. S. Granick, Science 253, 1374 (1991).
  35. D. Y. C. Chan and R. G. Horn, J. Chem. Phys. 83, 5311 (1985).
  36. J. N. Israelachvili, J. Colloid. Interface Sci. 110, 263 (1986).
  37. G. Reiter, A. L. Demirel, and S. Granick, Science 263, 1741 (1994).
  38. H. Yoshizawa, P. McGuiggan, and J. N. Israelachvili, Science 259, 1305 (1993).
  39. P. A. Thompson and M. O. Robbins, Science 250, 792 (1990);
  40. M. O. Robbins and P. A. Thompson, ibid. 253, 916 (1991).
  41. B. N. J. Persson, Phys. Rev. B 50, 4771 (1994).
  42. J. Gao, W. D. Luedtke, and U. Landman, Science 270, 605 (1995).
  43. J, van Alsten and S. Granick, Macromolecules 23, 4856 (1990);
  44. S. Granick and H.-W. Hu, Langmuir 10, 3857 (1994);
    J. Peanasky, L. Cai, C. R. Kessel, and S. Granick, ibid. 10, 3874 (1994).
  45. I. K. Snook and W. J. van Megen, J. Chem. Phys. 72, 2907 (1980).
  46. W. J. van Megen and I. K. Snook, J. Chem. Phys. 74, 1409 (1981).
  47. M. Parrinello and A. Rahman, J. Appl. Phys. 52, 7182 (1981). In deriving the equations of motion within the Parrinello-Rahman formalism, we take as our Lagrangian dynamical variables the scaled-space coordinates of the fluid particles and the component of the calculation cell along the x direction.
  48. M. Mondello and G. S. Grest, J. Chem. Phys. 103, 7156 (1995).
  49. T. K. Xia, J. Ouyang, M. W. Ribarsky, and U. Landman, Phys. Rev. Lett. 69, 1967 (1992).
  50. Similar simulations which we performed for simple spherical LJ fluids have shown an even more pronounced step-like behavior than that found by us for n-hexadecane [see Fig. 5(a)]. This indicates that solid-like behavior is enhanced in sufficiently thin confined liquids which pack well and exhibit a high degree of ordering, as in OMCTS (Ref. 19). Furthermore, recent simulations for n-tetracosane (n-C24H50) show a similar behaviour to that of n-hexadecane, leading us to conclude that the different behaviour of squalane is caused by branching rather than by increased chain-length; J. Gao, W. D. Luedtke, and U. Landman (in preparation).

CITING ARTICLES

For access to citing articles, you need to log in.
For access to citing articles, you need to Log in.