Volume 103, Issue 12, Pages (December 2012)

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Volume 103, Issue 12, Pages 2465-2474 (December 2012) Insights into Sphingolipid Miscibility: Separate Observation of Sphingomyelin and Ceramide N-Acyl Chain Melting  Sherry S.W. Leung, Jon V. Busto, Amir Keyvanloo, Félix M. Goñi, Jenifer Thewalt  Biophysical Journal  Volume 103, Issue 12, Pages 2465-2474 (December 2012) DOI: 10.1016/j.bpj.2012.10.041 Copyright © 2012 Biophysical Society Terms and Conditions

Figure 1 2H NMR spectra for 90:10 PSM-D31:PCer and 90:10 PSM:PCer-D31 at various temperatures. (Boxed temperatures) Boundaries of the phase transition. The minor baseline irregularities at ±60 kHz in the 56–75°C spectra of 90:10 PSM:PCer-D31 are artifacts from acoustic ringing. Biophysical Journal 2012 103, 2465-2474DOI: (10.1016/j.bpj.2012.10.041) Copyright © 2012 Biophysical Society Terms and Conditions

Figure 2 Effect of PCer concentration on the temperature dependence of M1 for 100:0(●), 90:10(▴), 80:20(▾), 70:30(♦), 60:40(■) PSM-D31:PCer (solid symbols), and PSM:PCer-D31 (open symbols). Biophysical Journal 2012 103, 2465-2474DOI: (10.1016/j.bpj.2012.10.041) Copyright © 2012 Biophysical Society Terms and Conditions

Figure 3 Order parameter profiles for 90:10, 80:20, 70:30, and 60:40 PSM-D31:PCer (solid symbols) and PSM:PCer-D31 (open symbols) at 75°C. All membranes are in the Lα phase. SCD values within the plateau regions are average values because the quadrupolar splittings from deuterons on these carbons are unresolved. Biophysical Journal 2012 103, 2465-2474DOI: (10.1016/j.bpj.2012.10.041) Copyright © 2012 Biophysical Society Terms and Conditions

Figure 4 The negative integral of the DSC thermograms of PSM:PCer (dotted lines) are superimposed on 2H NMR M1 temperature-dependence graphs for 100:0, 90:10, 80:20, 70:30, and 60:40 PSM-D31:PCer (solid symbols) and PSM:PCer-D31 (open symbols). The two graphs are scaled such that the maximum and minimum values of the integral and M1 are aligned. Biophysical Journal 2012 103, 2465-2474DOI: (10.1016/j.bpj.2012.10.041) Copyright © 2012 Biophysical Society Terms and Conditions

Figure 5 Phase diagram constructed from spectral inspections of PSM-D31:PCer (▴), spectral inspections of PSM:PCer-D31 (▵), spectral subtractions of PSM:PCer-D31 (○), completion of the highest-temperature DSC endotherm (■), and the apex temperature of the low-temperature endotherm (∼40°C) for 0–30% PCer and low-temperature onset of the broad endotherm (∼70°C) for 40 and 50% PCer on DSC thermograms (□). Biophysical Journal 2012 103, 2465-2474DOI: (10.1016/j.bpj.2012.10.041) Copyright © 2012 Biophysical Society Terms and Conditions

Figure 6 Phase boundaries calculated from regular solution theory based on the assumption of ideal mixing (solid lines) superimposed on the experimental data of Fig. 5. Biophysical Journal 2012 103, 2465-2474DOI: (10.1016/j.bpj.2012.10.041) Copyright © 2012 Biophysical Society Terms and Conditions

Figure 7 The PSM:PCer partial phase diagram. (Solid lines) Liquidus and the three-phase line at 41°C reflecting the good agreement of DSC and 2H NMR data. Other phase boundaries are expected, and we offer possible locations for these (dashed lines). An interpretation of the phases is also shown and corresponds to labeled regions of the phase diagram in Fig. 5. (Shaded and solid lipids) PSM and PCer, respectively. (Straight tails) Gel phase lipids. (Curvy tails) Lα phase lipids. Biophysical Journal 2012 103, 2465-2474DOI: (10.1016/j.bpj.2012.10.041) Copyright © 2012 Biophysical Society Terms and Conditions