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氘核固态核磁共振弛豫测量揭示了淀粉样β纤维无序N端结构域中两个不同的构象交换过程。

Deuteron Solid-State NMR Relaxation Measurements Reveal Two Distinct Conformational Exchange Processes in the Disordered N-Terminal Domain of Amyloid-β Fibrils.

作者信息

Vugmeyster Liliya, Au Dan Fai, Ostrovsky Dmitry, Fu Riqiang

机构信息

Department of Chemistry, University of Colorado Denver, Denver CO, USA, 80204.

Department of Mathematics, University of Colorado Denver, Denver CO, USA, 80204.

出版信息

Chemphyschem. 2019 Jul 2;20(13):1680-1689. doi: 10.1002/cphc.201900363. Epub 2019 Jun 14.

Abstract

We employed deuterium solid-state NMR techniques under static conditions to discern the details of the μs-ms timescale motions in the flexible N-terminal subdomain of Aβ amyloid fibrils, which spans residues 1-16. In particular, we utilized a rotating frame (R ) and the newly developed time domain quadrupolar Carr-Purcell-Meiboom-Gill (QCPMG) relaxation measurements at the selectively deuterated side chains of A2, H6, and G9. The two experiments are complementary in terms of probing somewhat different timescales of motions, governed by the tensor parameters and the sampling window of the magnetization decay curves. The results indicated two mobile "free" states of the N-terminal domain undergoing global diffusive motions, with isotropic diffusion coefficients of 0.7-1 ⋅ 10 and 0.3-3 ⋅ 10 ad  s . The free states are also involved in the conformational exchange with a single bound state, in which the diffusive motions are quenched, likely due to transient interactions with the structured hydrophobic core. The conformational exchange rate constants are 2-3 ⋅ 10  s and 2-3 ⋅ 10  s for the fast and slow diffusion free states, respectively.

摘要

我们在静态条件下采用氘固态核磁共振技术,以识别Aβ淀粉样纤维柔性N端亚结构域中微秒至毫秒时间尺度运动的细节,该亚结构域跨度为1至16位残基。具体而言,我们在A2、H6和G9的选择性氘代侧链上利用旋转坐标系(R)和新开发的时域四极 Carr-Purcell-Meiboom-Gill(QCPMG)弛豫测量。这两个实验在探测不同时间尺度的运动方面具有互补性,运动由张量参数和磁化衰减曲线的采样窗口决定。结果表明,N端结构域存在两种经历整体扩散运动的移动“自由”状态,各向同性扩散系数分别为0.7 - 1⋅10 和0.3 - 3⋅10  ad  s 。自由状态还参与与单一结合状态的构象交换,其中扩散运动被淬灭,这可能是由于与结构化疏水核心的瞬时相互作用。快速和慢速扩散自由状态的构象交换速率常数分别为2 - 3⋅10  s 和2 - 3⋅10  s 。

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