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首页> 外文期刊>Journal of magnetic resonance >Measurement of ~(15)N chemical shift anisotropy in a protein dissolved in a dilute liquid crystalline medium with the application of magic angle sample spinning
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Measurement of ~(15)N chemical shift anisotropy in a protein dissolved in a dilute liquid crystalline medium with the application of magic angle sample spinning

机译:魔术角样品旋转法测量溶解在稀液晶介质中的蛋白质中〜(15)N化学位移各向异性

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The chemical shifts of nuclei that have chemical shielding anisotropy, such as the ~(15)N amide in a protein, show significant changes in their chemical shifts when the sample is altered from an isotropic state to an aligned state. Such orientation-dependent chemical shift changes provide information on the magnitudes and orientation of the chemical shielding tensors relative to the molecule's alignment frame. Because of the extremely high sensitivity of the chemical shifts to the sample conditions, the changes in chemical shifts induced by adding aligned bicelles do not arise only from the protein alignment but should also include the accumulated effects of environmental changes including protein-bicelle interactions. With the aim of determining accurate ~(15)N chemical shielding tensor values for solution proteins, here we have used magic angle sample spinning (MAS) to observe discriminately the orientation-dependent changes in the ~(15)N chemical shift. The application of MAS to an aligned bicelle solution removes the torque that aligns the bicelles against the magnetic filed. Thus, the application of MAS to a protein in a bicelle solution eliminates only the molecular alignment effect, while keeping all other sample conditions the same. THe observed chemical shift differences between experiments with an without MAS therefore provide accurate values of the orientation-dependent ~(15)N chemical shifts. From the values for ubiquitin in a 7.5% (w/v) bicelle medium, we determined the ~(15)N chemical shielding anisotropy (CSA) tensor. For this evaluation, we considered uncertainties in measuring the ~1H-~(15)N dipolar couplings and the ~(15)N chemical shifts and also structural noise present in the reference X-ray structure, assuming a random distribution of each NH bond vector in a cone with 5° deviation from the original orientation. Taking into account these types of noise, we determined the average ~(15)N CSA tensor for the residues in ubiquitin as △σ = -162.0 ± 4.3 ppm, η = 0.18 ± 0.02, and β = 18.6 ± 0.5°, assuming a ~1H-~(15)N bond length of 1.02 A. These tensor values are consistent with those obtained from solid-state NMR experiments.
机译:当样品从各向同性状态改变为排列状态时,具有化学屏蔽各向异性的原子核化学位移,例如蛋白质中的〜(15)N酰胺,会显示出化学位移的重大变化。这种与方向有关的化学位移变化提供了有关化学屏蔽张量相对于分子的排列框架的大小和方向的信息。由于化学位移对样品条件的敏感性极高,因此添加对齐的比色池所引起的化学位移变化不仅来自蛋白质比对,还应包括环境变化的累积效应,包括蛋白质-二聚体相互作用。为了确定溶液蛋白的精确〜(15)N化学屏蔽张量值,这里我们使用魔角样品旋转(MAS)来区分地观察〜(15)N化学位移的方向依赖性变化。将MAS应用于对齐的双锥解决方案,可消除将Bicell对准磁场的扭矩。因此,将MAS应用于比色杯溶液中的蛋白质,仅消除了分子排列效果,同时使所有其他样品条件保持不变。因此,在没有使用MAS的实验之间观察到的化学位移差异,因此提供了与方向相关的〜(15)N化学位移的准确值。从7.5%(w / v)比塞勒培养基中的泛素值,我们确定了〜(15)N化学屏蔽各向异性(CSA)张量。对于此评估,我们假设每个NH键的随机分布都考虑了测量〜1H-〜(15)N偶极耦合和〜(15)N化学位移以及参比X射线结构中存在的结构噪声的不确定性。与原始方向偏离5°的圆锥中的向量。考虑到这些类型的噪声,我们确定了遍在蛋白中的残基的平均〜(15)N CSA张量为△σ= -162.0±4.3 ppm,η= 0.18±0.02和β= 18.6±0.5°,假设〜1H-〜(15)N键长为1.02A。这些张量值与从固态NMR实验获得的张量值一致。

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