1996
DOI: 10.1006/jcis.1996.0328
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Miscibility Behavior of Binary Monolayers in Dependence on the Chain Length Differences and Film States of the Phosphatidylcholine/Phosphatidylethanolamine Mixtures

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Cited by 10 publications
(8 citation statements)
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“…Because the highest deviation from the additivity rule is observed for the mixtures of X AmB between 0.5 and 0.7 (Figure ), one may assume that the highest stability of the complex is reached at X AmB = 0.66, corresponding to a system of 2:1 AmB/DPPA (i.e., the one in which a phospholipid molecule is sandwiched between two AmB molecules). The complexes of the same stoichiometry have been reported for similar systems. ,, Likewise, the slow, spontaneous mixing of separately spread monolayer components has been observed by several authors. …”
Section: Discussionsupporting
confidence: 73%
“…Because the highest deviation from the additivity rule is observed for the mixtures of X AmB between 0.5 and 0.7 (Figure ), one may assume that the highest stability of the complex is reached at X AmB = 0.66, corresponding to a system of 2:1 AmB/DPPA (i.e., the one in which a phospholipid molecule is sandwiched between two AmB molecules). The complexes of the same stoichiometry have been reported for similar systems. ,, Likewise, the slow, spontaneous mixing of separately spread monolayer components has been observed by several authors. …”
Section: Discussionsupporting
confidence: 73%
“…However, the finding that when ergosterol and AmB are spread separately on the substrate there is a gradual rise in the surface pressure of the low-pressure π− A inflection region as the two components diffuse into each other (Figure ) suggests that in all cases this region reflects the transition of AmB molecules from horizontal to vertical orientation, and that the rise in surface pressure is due to an increasing, presumably nonhydrophobic, attractive interaction between AmB and ergosterol molecules (minimal when the monolayer components are spread separately and left only for a short time (10 min) before film compression (Figure , curve 2), greater when the components are spread separately but left for a longer time (2 h) allowing mutual diffusion (Figure , curve 3), and greatest when the component mixture is prepared before the film is spread (Figure , curve 1)). The slow, spontaneous mixing of initially unmixed monolayer components has been observed by several authors. Attractive interaction between AmB and ergosterol molecules would also account for the transition region of curve 1 in Figure occurring at smaller mean molecular areas than the low-pressure transition region of curve 2. It is hoped that further research using other techniques such as BAM or fluorescence microscopy may confirm these findings.…”
Section: Discussionmentioning
confidence: 59%
“…Thus, the results of Niccolai et al, related to mixed monolayers of 1-glycerol monooleoil (MON) and 1-glycerol monoestearoil (MOS), confirm the “empirical rule” that immiscibility of the components at the interface is due to their different orientations (MON, horizontal; MOS, vertical). Other authors , attribute the miscibility or immiscibility of the components to the physical state of their respective monolayers: when both are in the same surface state (for example in the expanded state), components are miscible at the interface, whereas if they are in different surface states (for example, liquid-expanded and liquid-condensed states), they are partially miscible or immiscible. In fact, this reference to the physical states of the monolayer is another way of considering the different orientations of the molecules at the interface, because the nature of the surface state depends on the arrangement of molecules on the water surface.…”
Section: Discussionmentioning
confidence: 99%