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Composition fluctuations, chemical exchange, and nuclear relaxation in membranes containing cholesterol
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10.1063/1.2730805
/content/aip/journal/jcp/126/18/10.1063/1.2730805
http://aip.metastore.ingenta.com/content/aip/journal/jcp/126/18/10.1063/1.2730805
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Figures

Image of FIG. 1.
FIG. 1.

(Color) Theoretical phase diagram. The diagram simulates the results obtained experimentally by Veatch and Keller using fluorescence microscopy (Ref. 11) and NMR spectroscopy (Ref. 3) for the ternary lipid mixture, cholesterol, DPPC, and DOPC. The theoretical diagram uses a thermodynamic model (Refs. 8 and 10) involving the formation of a complex of one molecule of cholesterol and two molecules of DPPC, along with a mean-field repulsion between the complex and DOPC.

Image of FIG. 2.
FIG. 2.

Molecular free energies as a function of composition. The free energy parameters employed to construct the phase diagram in Fig. 1 are used to calculate the molecular free energy changes for composition variations along three illustrative directions indicated by the dotted lines. Small composition fluctuations along a line parallel to the stoichiometric tie line (b) have the lowest free energy, particularly near the critical temperature, as can be seen in panel (b). Composition fluctuations calculated in this paper only include composition fluctuations along this direction (b) where the initial mole fractions of cholesterol and DPPC are in a 1:2 ratio. The intersection point of the three lines is the ternary critical composition.

Image of FIG. 3.
FIG. 3.

Spectral density factors and correlation times for no sample spinning. Panels (a) and (b) consider fluctuations in the total cholesterol concentration. The dependence of on temperature and on the cut-off wavelength is shown in (a). A plot of the average correlation time for is shown in (b) as a function of temperature. The zero frequency spectral density factors and the average correlation time are related to one another by the fluctuation in the concentration of complexes: . This correlation time diverges at the critical temperature (asymptote shown by dotted vertical line). Panels (c) and (d) consider complex formation (chemical exchange) kinetics, i.e., fluctuations in complex concentration at fixed total cholesterol concentration. The dependence of on temperature and on the cut-off wavelength is shown in (c). In this case the fluctuations arise from the kinetics of complex formation and dissociation, and are characterized by a single kinetic correlation time. A plot of this kinetic correlation time [Eq. (44)] is shown in (d) as a function of temperature.

Image of FIG. 4.
FIG. 4.

Magic angle spinning spectral density factors related to composition fluctuations and chemical exchange. Panels (a) and (b) give the spectral density factors due to composition fluctuations and complex formation (chemical exchange) kinetics, respectively. Both calculations include a gradient term in the free energy of the fluctuations.

Image of FIG. 5.
FIG. 5.

Calculated nuclear resonance linewidths. The linewidths refer to a half height linewidth (HHLW). This is for Lorentzian signals. Panel (a), solid line, gives the calculated Lorentzian HHLW due to fluctuations in complex concentration that arise from fluctuations in total cholesterol concentration. The linewidth refers to the quadrupole axis orientation , corresponding to the outer wings of the deuterium NMR spectra with no sample spinning. The Lorentzian (which diverges at the critical temperature) assumes rapid gradient diffusion so that Eq. (14) can be used. The dotted line gives the Gaussian HHLW corresponding to a zero gradient diffusion coefficient. The dashed curve gives the contribution to arising from chemical exchange kinetics. Panel (b) gives the sum of the two Lorentzian contributions in panel (a). Panels (c) and (d) give the results for the case of magic angle spinning at . In panel (c), the solid curve gives the Lorentzian HHLW due to fluctuations in total cholesterol concentration and the dashed curve gives the Lorentzian HHLW due to fluctuations in complex concentration with fixed total cholesterol concentration, arising from the kinetics of complex formation and dissociation. Panel (d) gives the sum of the two contributions in (c). All calculations include the gradient energy term [Eqs. (21) and (46)].

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/content/aip/journal/jcp/126/18/10.1063/1.2730805
2007-05-14
2014-04-18
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Composition fluctuations, chemical exchange, and nuclear relaxation in membranes containing cholesterol
http://aip.metastore.ingenta.com/content/aip/journal/jcp/126/18/10.1063/1.2730805
10.1063/1.2730805
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