Volume 106, Issue 10, Pages (May 2014)

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Volume 106, Issue 10, Pages 2126-2133 (May 2014) Probing the Transmembrane Structure and Dynamics of Microsomal NADPH- cytochrome P450 oxidoreductase by Solid-State NMR  Rui Huang, Kazutoshi Yamamoto, Meng Zhang, Nataliya Popovych, Ivan Hung, Sang-Choul Im, Zhehong Gan, Lucy Waskell, Ayyalusamy Ramamoorthy  Biophysical Journal  Volume 106, Issue 10, Pages 2126-2133 (May 2014) DOI: 10.1016/j.bpj.2014.03.051 Copyright © 2014 Biophysical Society Terms and Conditions

Figure 1 (A) A schematic of MFBD with its N-terminal transmembrane domain incorporated in lipid bilayers. (B) SDS-PAGE gel of MFBD. (C) Proton-decoupled 31P chemical-shift spectra of DLPC/DHPC/cholesterol bicelles containing MFBD. Narrow peaks from DLPC and DHPC demonstrate a high degree of alignment of bicelles. Peaks observed at 0 ppm are from phosphorous atoms of the FMN molecule. To see this figure in color, go online. Biophysical Journal 2014 106, 2126-2133DOI: (10.1016/j.bpj.2014.03.051) Copyright © 2014 Biophysical Society Terms and Conditions

Figure 2 15N NMR spectra of 15N-labeled MFBD incorporated in magnetically aligned bicelles were obtained using RINEPT (A) and ramped cross-polarization (CP) with a contact time of 2.0 ms (B), 1.0 ms (C), 0.4 ms (D), and 0.1 ms (E). The RINEPT spectrum (A) shows spectral intensity only in the 100–140 ppm region, indicating the high mobility of the soluble domain. Resonances in the 70–100-ppm region in the CP spectra (B–E) are assigned to the immobile transmembrane domain. Buildup curves (F) were measured for resonances at 93.5 ppm (black) and 128.4 ppm (red) representing the two chemical-shift regions corresponding to two different domains of the protein. To see this figure in color, go online. Biophysical Journal 2014 106, 2126-2133DOI: (10.1016/j.bpj.2014.03.051) Copyright © 2014 Biophysical Society Terms and Conditions

Figure 3 Hydrogen/deuterium exchange spectra of 15N-labeled MFBD incorporated in magnetically aligned bicelles. 15N NMR spectra were obtained using ramped cross-polarization with a contact time of 0.5 ms before H/D exchange (A), and 5 h (B), and 17 h (C) after H/D exchange. Biophysical Journal 2014 106, 2126-2133DOI: (10.1016/j.bpj.2014.03.051) Copyright © 2014 Biophysical Society Terms and Conditions

Figure 4 Two-dimensional 15N separated-local-field NMR spectrum of a uniformly 15N-labeled MFBD incorporated in magnetically aligned DLPC/DHPC/cholesterol bicelles. The spectrum was collected with a 0.5-ms CP contact time and 25 kHz SPINAL16 decoupling. To see this figure in color, go online. Biophysical Journal 2014 106, 2126-2133DOI: (10.1016/j.bpj.2014.03.051) Copyright © 2014 Biophysical Society Terms and Conditions

Figure 5 (A–C) Simulated helical wheels showing the sensitivity of the wheel pattern to the indicated tilt angle of the helix. (D and E) Fitting of the observed resonances in two-dimensional SLF spectra (blue circles) with different tilt angles and order parameters (S). The tilt angle used in panel D is 13° with order parameters S of 0.6 (red), 0.8 (black), and 1.0 (purple). The order parameter used in panel E is 0.8 with varied tilt angles: 11° (orange), 12° (purple), 13° (black), 14° (green), and 15° (blue). The best-fitting wheel indicates an average helical tilt angle of 13° and an order parameter S of 0.8 (F) for the transmembrane helix of the MFBD protein embedded in magnetically aligned DLPC/DHPC/cholesterol bicelles. To see this figure in color, go online. Biophysical Journal 2014 106, 2126-2133DOI: (10.1016/j.bpj.2014.03.051) Copyright © 2014 Biophysical Society Terms and Conditions