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仅使用15N弛豫数据的谱密度函数映射。

Spectral density function mapping using 15N relaxation data exclusively.

作者信息

Farrow N A, Zhang O, Szabo A, Torchia D A, Kay L E

机构信息

Protein Engineering Network of Centre of Excellence, University of Toronto, ON, Canada.

出版信息

J Biomol NMR. 1995 Sep;6(2):153-62. doi: 10.1007/BF00211779.

Abstract

A method is presented for the determination of values of the spectral density function, J(omega), describing the dynamics of amide bond vectors from 15N relaxation parameters alone. Assuming that the spectral density is given by the sum of Lorentzian functions, the approach allows values of J(omega) to be obtained at omega = 0, omega N and 0.870 omega H, where omega N and omega H are Larmor frequencies of nitrogen and proton nuclei, respectively, from measurements of 15N T1, T2 and 1H-15N steady-state NOE values at a single spectrometer frequency. Alternatively, when measurements are performed at two different spectrometer frequencies of i and j MHz, J(omega) can be mapped at omega = 0, omega iN, omega jN, 0.870 omega iH and 0.870 omega iH, where omega iN, for example, is the 15N Larmor frequency for a spectrometer operating at 1 MHz. Additionally, measurements made at two different spectrometer frequencies enable contributions to transverse relaxation from motions on millisecond-microsecond time scales to be evaluated and permit assessment of whether a description of the internal dynamics is consistent with a correlation function consisting of a sum of exponentials. No assumptions about the specific form of the spectral density function describing the dynamics of the 15N-NH bond vector are necessary, provided that dJ(omega)/d omega is relatively constant between omega = omega H + omega N to omega = omega H - omega N. Simulations demonstrate that the method is accurate for a wide range of protein motions and correlation times, and experimental data establish the validity of the methodology. Results are presented for a folded and an unfolded form of the N-terminal SH3 domain of the protein drk.

摘要

本文提出了一种仅根据(^{15}N)弛豫参数来确定描述酰胺键向量动力学的光谱密度函数(J(\omega))值的方法。假设光谱密度由洛伦兹函数之和给出,该方法允许从在单个光谱仪频率下对(^{15}N)的(T_1)、(T_2)以及(^{1}H - ^{15}N)稳态核欧沃豪斯效应(NOE)值的测量中,获得(\omega = 0)、(\omega_N)和(0.870\omega_H)处的(J(\omega))值,其中(\omega_N)和(\omega_H)分别是氮核和质子核的拉莫尔频率。或者,当在(i)和(j)兆赫兹的两个不同光谱仪频率下进行测量时,(J(\omega))可以在(\omega = 0)、(\omega_{iN})、(\omega_{jN})、(0.870\omega_{iH})和(0.870\omega_{jH})处进行映射,例如,(\omega_{iN})是在(1)兆赫兹下运行的光谱仪的(^{15}N)拉莫尔频率。此外,在两个不同光谱仪频率下进行的测量能够评估毫秒至微秒时间尺度上的运动对横向弛豫的贡献,并允许评估内部动力学的描述是否与由指数之和组成的相关函数一致。只要在(\omega = \omega_H + \omega_N)至(\omega = \omega_H - \omega_N)之间(dJ(\omega)/d\omega)相对恒定,就无需对描述(^{15}N - NH)键向量动力学的光谱密度函数的具体形式做任何假设。模拟表明该方法对于广泛的蛋白质运动和相关时间都是准确的,并且实验数据证实了该方法的有效性。给出了蛋白质drk的N端SH3结构域的折叠形式和未折叠形式的结果。

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