1975
DOI: 10.1126/science.188.4195.1268
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Spatial Configuration of Macromolecular Chains

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Cited by 83 publications
(45 citation statements)
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“…[47] In fact, the enthalpy change observed during lipid main transition can mostly be ascribed to the extent of the interaction between guest molecules and hydrophobic tails of lipids. [48] Moreover, it has been shown that T m increases with the rigidity of the membrane, due to an interfacial lipid/peptide interaction. [48,49] With this in mind, DSC experiments were performed on both zwitterionic (DPPC; 1,2-dipalmitoyl-sn-glycero-3-phosphatidylcholine) and negatively charged (DPPS; 1,2-dipalmitoyl-sn-glycero-3-phosphoserine) lipid bilayers.…”
Section: Differential Scanning Calorimetry Of the Vdac Peptide In A Cmentioning
confidence: 99%
“…[47] In fact, the enthalpy change observed during lipid main transition can mostly be ascribed to the extent of the interaction between guest molecules and hydrophobic tails of lipids. [48] Moreover, it has been shown that T m increases with the rigidity of the membrane, due to an interfacial lipid/peptide interaction. [48,49] With this in mind, DSC experiments were performed on both zwitterionic (DPPC; 1,2-dipalmitoyl-sn-glycero-3-phosphatidylcholine) and negatively charged (DPPS; 1,2-dipalmitoyl-sn-glycero-3-phosphoserine) lipid bilayers.…”
Section: Differential Scanning Calorimetry Of the Vdac Peptide In A Cmentioning
confidence: 99%
“…This model, sometimes called the spaghetti model, is due to Flory [31]. It can be viewed as an analog of the CRN and the RCP models, subject to the same types of limitations, and especially designed for organic polymeric glasses such as polystyrene.…”
Section: Random Coil Model For Polymeric Glassesmentioning
confidence: 99%
“…For many transition metal/metalloid glasses (such as Ni3B), there seems to be even more ordering, with polyhedral building blocks suct as tetrahedral, octahedral, or tricapped trigonal prismatic units of atoms forming the solid by random close packing [30]. Finally, in the random coils of a polymeric organic glass [31], the long and flexible coils are intermeshed in random-walk configurations as illustrated in Fig. 6, but each individual coil is formed by the repetition (up to --lO times) of a monomeric molecular unit, so that the local environment of each atom, formed by those atoms (all within the same coil) to which it is bonded, is quite well-defined.…”
Section: Comparisons With Experimentsmentioning
confidence: 99%
“…A well-known example is the gauche-trans equilibrium in n-butane. It was argued (6) that in the disordered liquid phase the intramolecular potential averages to that in the isolated molecule. Experimental data for the energy difference between the trans and gauche forms overlap for the liquid and gaseous states (1).…”
Section: Introductionmentioning
confidence: 99%