Nobuaki Matsumori, Toshiyuki Yamaguchi, Yoshiko Maeta, Michio Murata 

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Orientation and Order of the Amide Group of Sphingomyelin in Bilayers Determined by Solid-State NMR  Nobuaki Matsumori, Toshiyuki Yamaguchi, Yoshiko Maeta, Michio Murata  Biophysical Journal  Volume 108, Issue 12, Pages 2816-2824 (June 2015) DOI: 10.1016/j.bpj.2015.05.011 Copyright © 2015 Biophysical Society Terms and Conditions

Figure 1 Structure of 13C/15N doubly labeled SMs. To see this figure in color, go online. Biophysical Journal 2015 108, 2816-2824DOI: (10.1016/j.bpj.2015.05.011) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 2 Synthesis of 13C/15N doubly labeled SMs. (a–p) Reagents and conditions: (a) (Boc)2O, NaOH, H2O, dioxane, rt, 2 h; (b) NH(Me)OMe∙HCl, NMM, EDC, CH2Cl2, −15°C, 4 h; (c) TBSCl, imidazole, DMF, rt, 1 h (86% for three steps); (d) vinyl MgBr, THF, rt, 1.5 h (86%); (e) LiAlH(OtBu)3, EtOH, −78°C, 2 h (93%); (f) 1-pentadecene, Grubbs II catalyst, p-quinone, CH2Cl2, 55°C, 2 h (64%); (g) TBAF, THF, rt, 35 min (93%); (h) PivCl, pyridine, −30°C, 2 h (89%); (i) TBSOTf, 2,6-lutidine, CH2Cl2, 0°C, 30 min; (j) DBU, MeOH, rt, 16 h (40% for two steps); (k) 2-chloro-1,3,2-dioxaphosphoran-2-oxide, Et3N, DMAP, benzene, 0°C, 1.5 h; (l) Me3N, CH3CN, 85°C, 46 h (90% for two steps); (m) TFA, CH2Cl2, 0°C, 1 h; (o) Et3N, DMAP, THF, rt, 21 h; and (p) TBAF, THF, rt, 28 h (53% for three steps). Biophysical Journal 2015 108, 2816-2824DOI: (10.1016/j.bpj.2015.05.011) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 3 (a and b) Amide regions of CP-MAS spectra (black lines) of powdered 1′-13C-SM (a) and 2-15N-SM (b) with spectral simulation using SIMPSON (red lines). Spectra were recorded at 45°C under MAS of (a) 1.5 kHz or (b) 0.7 kHz. To see this Figure in color, go online. Biophysical Journal 2015 108, 2816-2824DOI: (10.1016/j.bpj.2015.05.011) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 4 Top view of the amide group of SM from calculated 13C and 15N CSA principal-axis systems. The axes of δ22N and δ33C are perpendicular to the amide plane. Experimental principal values in ppm (Table 1) are shown in parentheses. To see this figure in color, go online. Biophysical Journal 2015 108, 2816-2824DOI: (10.1016/j.bpj.2015.05.011) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 5 13C CP-MAS spectra of hydrated 1′-13C-2-15N-SM with spectral simulations using SIMPSON (red lines). (a and b) 1′-13C-2-15N-SM (a) and 1′-13C-2-15N-SM/Chol (b) at a 1:1 molar ratio were hydrated with 50 wt% D2O, and both spectra were recorded at 45°C under MAS of 600 Hz. To see this figure in color, go online. Biophysical Journal 2015 108, 2816-2824DOI: (10.1016/j.bpj.2015.05.011) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 6 Intramolecular REDOR experiments for 1′-13C-2-15N-SM. (a) 13C-15N REDOR spectra for the SM-Chol membrane (1′-13C-2-15N-SM/Chol = 1:1 in 50 wt% D2O) with a dephasing time of 4 ms at 45°C. The S0 (black line) and S (red line) spectra were obtained with and without 15N-irradiation, respectively. (b) REDOR dephasing effects for (●) SM-Chol membranes and (▪) SM-only membranes at various dephasing times. ΔS was (S0 − S). The best-fit theoretical curves were obtained with D = 265 Hz (red line) and 150 Hz (blue line) for SM-Chol and SM membranes, respectively. The possible errors were within ±20 Hz. To see this figure in color, go online. Biophysical Journal 2015 108, 2816-2824DOI: (10.1016/j.bpj.2015.05.011) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 7 Intramolecular REDOR plots for 2′-13C-2-15N-SM in membranes in the (●) presence and (▪) absence of Chol. ΔS was (S0 − S). Intramolecular REDOR dephasing was not observed for the SM membrane. The best-fit theoretical curve for SM-Chol with D = 13 Hz is shown. The possible errors were within ±2 Hz. To see this figure in color, go online. Biophysical Journal 2015 108, 2816-2824DOI: (10.1016/j.bpj.2015.05.011) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 8 The rotation-axis direction is defined by the polar coordinates α (azimuthal angle) and β (polar angle) with respect to the 13C CSA tensor axes. Angle θ is the angle between the rotation axis and the C1′-N bond. The oxygen atom on C1′ was omitted for clarity. To see this figure in color, go online. Biophysical Journal 2015 108, 2816-2824DOI: (10.1016/j.bpj.2015.05.011) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 9 (a and b) 2D RMSD contour plots for (a) SM at S = 0.67 and (b) SM-Chol at S = 0.84; β has two possible values. To see this figure in color, go online. Biophysical Journal 2015 108, 2816-2824DOI: (10.1016/j.bpj.2015.05.011) Copyright © 2015 Biophysical Society Terms and Conditions

Figure 10 (a–c) Two rotation-axis directions for an SM-Chol membrane (a) with respect to the amide plane and partial orientations of an SM molecule for (b) β = 31° or (c) 149°, based on the conformation of SM deduced from bicelle experiments (15). The orange axes indicate the rotation axes. Considering the direction of an acyl chain, orientation b is more likely than c. Structure b also shows one possible intermolecular hydrogen bond involving the SM amide group. To see this figure in color, go online. Biophysical Journal 2015 108, 2816-2824DOI: (10.1016/j.bpj.2015.05.011) Copyright © 2015 Biophysical Society Terms and Conditions