1994
DOI: 10.1063/1.468042
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Lattice structures and molecular tilts in Langmuir monolayers of saturated fatty acid–alcohol mixtures

Abstract: We have studied Langmuir monolayers composed of mixtures of heneicosanoic acid and heneicosanol using π-A isotherms and x-ray diffraction. We find that the two materials are miscible in monolayer form. We have determined how the phase diagram of the acid evolves to that of the alcohol as the composition varies. X-ray diffraction data along isotherms and isobars show that the head–head interactions, like the tail–tail interactions, are anisotropic. The ‘‘swiveling transition’’ between phases with different tilt… Show more

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Cited by 46 publications
(60 citation statements)
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“…Most of them were devoted to partially ordered [3][4][5][6][7][8][9][10][11][12][13][14][15][16][17] and 2D crystalline 18-29 phases of simple amphiphiles-fatty acids, alcohols, and their derivatives. At least eight structurally distinct condensed phases were revealed for nonchiral substances.…”
Section: Introductionmentioning
confidence: 99%
“…Most of them were devoted to partially ordered [3][4][5][6][7][8][9][10][11][12][13][14][15][16][17] and 2D crystalline 18-29 phases of simple amphiphiles-fatty acids, alcohols, and their derivatives. At least eight structurally distinct condensed phases were revealed for nonchiral substances.…”
Section: Introductionmentioning
confidence: 99%
“…The swiveling transition, which has been recently extensively studied, 12,13 is the transition between the L 2 (L 2h ) phase ͓rectangular lattice with molecules tilted towards ͑NN͒ direction͔ and the phase denoted as L 2 Ј(L 2 *) ͓rectangular lattice, characterized by molecular tilt ordering towards ͑NNN͒ direction͔. In terms of the order parameters introduced here, the transition corresponds to the change: ͗Y 4 ͘⇒Ϫ͗Y 4 ͘, or equivalent ⑀ 2 ⇒Ϫ⑀ 2 , for one domain of the phases and with corresponding relations for the two other domains.…”
Section: The Swiveling Transitionmentioning
confidence: 99%
“…Further, we have departed from the assumptions of previous authors by modeling these phases with only one molecule per unit cell. 12 These calculations were done at a low enough pressure ͑isotropic͒ to ensure a global minimum that exhibited tilt ͑Ϫ45 in our arbitrary pressure scale͒. 6 After locating the potential minimum ͑with respect to lattice vectors a and b and the three orientational angles͒, ⑀ 1 was set equal to 0, and a 0 of the parent hexagonal lattice was found by solving the equation…”
Section: Calculationsmentioning
confidence: 99%
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