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首页> 外文期刊>The Biochemical Journal >EFFECT OF MAGNETIC FIELD STRENGTH ON THE LINEWIDTH AND SPIN-LATTICE RELAXATION TIME OF THE THIOCYANATE CARBON OF CYANYLATED BETA-LACTOGLOBULIN B - OPTIMIZATION OF THE EXPERIMENTAL PARAMETERS FOR OBSERVING THIOCYANATE CARBONS IN PROTEINS
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EFFECT OF MAGNETIC FIELD STRENGTH ON THE LINEWIDTH AND SPIN-LATTICE RELAXATION TIME OF THE THIOCYANATE CARBON OF CYANYLATED BETA-LACTOGLOBULIN B - OPTIMIZATION OF THE EXPERIMENTAL PARAMETERS FOR OBSERVING THIOCYANATE CARBONS IN PROTEINS

机译:磁场强度对氰化β-乳球蛋白B硫氰酸盐碳线宽和自旋弛豫时间的影响-优化蛋白质中观察硫氰酸盐的实验参数

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摘要

The linewidths and spin-lattice relaxation times of the C-13-n.m.r. signal at 109.7 p.p.m. due to the thiocyanate carbon of intact [cyanato-C-13]cyanylated-beta-lactoglobulin-B have been determined at magnetic field strengths of 1.88, 6.34 and 11.74 T as well as the spin-lattice relaxation times of its backbone alpha-carbon atoms. The linewidths were directly proportional to the square of the magnetic field strength and we conclude that, at magnetic field strengths of 6.34 T or above, more than 70% of the linewidth will be determined by chemical-shift anistropy. We estimate that the spin-lattice relaxation time resulting from the chemical-shift anistropy of the thiocyanate carbon is 1.52 +/- 0.1 s and we conclude that for magnetic field strengths of 6.34 T and above the observed spin-lattice relaxation time of the thiocyanate carbon will be essentially independent of magnetic field strength. Using the rigid-rotor model we obtain estimates of the rotational correlation time of [cyanato-C-13]cyanylated-beta-lactoglobulin-B and of the chemical-shift anisotropy shielding tenser of its thiocyanate carbon. We have calculated the linewidths and spin-lattice relaxation times of thiocyanate carbons at magnetic field strengths of 1.88-14.1 T in proteins with M(r) values in the range 10000-400000. The effects of magnetic field strength on the resolution and signal-to-noise ratios of the signals due to thiocyanate carbons attached to proteins of M(r) greater than 10000 are discussed.
机译:C-13-n.m.r。的线宽和自旋晶格弛豫时间。晚上109.7点发出信号由于完整的[氰基-C-13]氰基化的β-乳球蛋白-B的硫氰酸盐碳已在1.88、6.34和11.74 T的磁场强度下及其骨架α-碳的自旋晶格弛豫时间确定原子。线宽与磁场强度的平方成正比,我们得出的结论是,在6.34 T或更高的磁场强度下,超过70%的线宽将由化学位移定律决定。我们估计,由硫氰酸盐碳的化学位移无规性导致的自旋晶格弛豫时间为1.52 +/- 0.1 s,并且我们得出结论,对于6.34 T和更高的磁场强度,所观察到的硫氰酸盐的自旋晶格弛豫时间碳将基本上与磁场强度无关。使用刚性转子​​模型,我们获得了[cyanato-C-13]氰基化β-乳球蛋白B的旋转相关时间及其硫氰酸盐碳的化学位移各向异性屏蔽张量的估计值。我们已经计算出M(r)值在10000-400000范围内的蛋白质中,磁场强度为1.88-14.1 T时,硫氰酸盐碳的线宽和自旋晶格弛豫时间。讨论了磁场强度对信号的分辨率和信噪比的影响,该信号是由于附着在M(r)大于10000的蛋白质上的硫氰酸盐碳所致。

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