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整合膜肽的动力学:短杆菌肽的氘核磁共振弛豫研究

Dynamics of an integral membrane peptide: a deuterium NMR relaxation study of gramicidin.

作者信息

Prosser R S, Davis J H

机构信息

Department of Physics, University of Guelph, Ontario, Canada.

出版信息

Biophys J. 1994 May;66(5):1429-40. doi: 10.1016/S0006-3495(94)80933-6.

Abstract

Solid state deuterium (2H) NMR inversion-recovery and Jeener-Broekaert relaxation experiments were performed on oriented multilamellar dispersions consisting of 1,2-dilauroyl-sn-glycero-3-phosphatidylcholine and 2H exchange-labeled gramicidin D, at a lipid to protein molar ratio (L/P) of 15:1, in order to study the dynamics of the channel conformation of the peptide in a liquid crystalline phase. Our dynamic model for the whole body motions of the peptide includes diffusion of the peptide around its helix axis and a wobbling diffusion around a second axis perpendicular to the local bilayer normal in a simple Maier-Saupe mean field potential. This anisotropic diffusion is characterized by the correlation times, tau R parallel and tau R perpendicular. Aligning the bilayer normal perpendicular to the magnetic field and graphing the relaxation rate, 1/T1Z, as a function of (1-S2N-2H), where S2N-2H represents the orientational order parameter, wer were able to estimate the correlation time, tau R parallel, for rotational diffusion. Although in the quadrupolar splitting, which varies as (3 cos2 theta D-1), has in general two possible solutions to theta D in the range 0 < or = theta D < or = 90 degrees, the 1/T1Z vs. (1-S2N-2H) curve can be used to determine a single value of theta D in this range. Thus, the 1/T1Z vs. (1-S2N-2H) profile can be used both to define the axial diffusion rate and to remove potential structural ambiguities in the splittings. The T1Z anisotropy permits us to solve for the two correlation times (tau R parallel = 6.8 x 10(-9) s and tau R perpendicular = 6 x 10(-6) s). The simulated parameters were corroborated by a Jeener-Broekaert experiment where the bilayer normal was parallel to the principal magnetic field. At this orientation the ratio, J2(2 omega 0)/J1(omega 0) was obtained in order to estimate the strength of the restoring potential in a model-independent fashion. This measurement yields the rms angle, <theta 2>1/2 (= 16 +/- 2 degrees at 34 degrees C), formed by the peptide helix axis and the average bilayer normal.

摘要

为了研究肽在液晶相中的通道构象动力学,对由1,2 - 二月桂酰 - sn - 甘油 - 3 - 磷脂酰胆碱和2H交换标记的短杆菌肽D组成的取向多层层状分散体进行了固态氘(2H)核磁共振反转恢复和Jeener - Broekaert弛豫实验,脂质与蛋白质的摩尔比(L/P)为15:1。我们关于肽整体运动的动力学模型包括肽围绕其螺旋轴的扩散以及在简单的迈尔 - 绍普平均场势中围绕垂直于局部双层法线的第二轴的摆动扩散。这种各向异性扩散由相关时间τR平行和τR垂直表征。将双层法线垂直于磁场排列,并绘制弛豫率1/T1Z作为(1 - S2N - 2H)的函数,其中S2N - 2H表示取向序参量,我们能够估计旋转扩散的相关时间τR平行。尽管在四极分裂中,其随(3cos2θD - 1)变化,在0≤θD≤90度范围内通常对θD有两个可能的解,但1/T1Z与(1 - S2N - 2H)曲线可用于确定该范围内θD的单一值。因此,1/T1Z与(1 - S2N - 2H)曲线既可以用于定义轴向扩散率,又可以消除分裂中潜在的结构模糊性。T1Z各向异性使我们能够求解两个相关时间(τR平行 = 6.8×10−9秒和τR垂直 = 6×10−6秒)。通过Jeener - Broekaert实验证实了模拟参数,在该实验中双层法线平行于主磁场。在这个取向下,获得了J2(2ω0)/J1(ω0)的比值,以便以与模型无关的方式估计恢复势的强度。该测量得出了由肽螺旋轴和平均双层法线形成的均方根角<θ2>1/2(在34℃时为16±2度)。

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