Laboratory of Chemical Physics, National Institute of Diabetes and Digestive and Kidney Diseases, National Institutes of Health, Bethesda, Maryland 20892-0520, USA.
J Am Chem Soc. 2010 Jul 28;132(29):9948-51. doi: 10.1021/ja1048253.
Recent studies have implicated non-fibrillar oligomers of the amyloid beta (Abeta) peptide as the primary toxic species in Alzheimer's disease. Detailed structural and kinetic characterization of these states, however, has been difficult. Here we use NMR relaxation measurements to address the kinetics of exchange between monomeric and large, polymorphic oligomeric species of Abeta(1-40). (15)N and (1)H(N) R(2) data at multiple magnetic fields were recorded for several peptide concentrations subsequent to the establishment of a stable pseudo-equilibrium between monomeric and NMR-invisible soluble oligomeric species. The increase in (15)N and (1)H(N) R(2) rates as a function of protein concentration is independent of nucleus and magnetic field and shows only a small degree of variation along the peptide chain. This phenomenon is due to a lifetime broadening effect arising from the unidirectional conversion of monomer to the NMR-invisible oligomeric species ("dark" state). At a total Abeta(1-40) concentration of 300 microM, the apparent first-order rate constant for this process is approximately 3 s(-1). Fitting the McConnell equations for two dipolar-coupled spins in two-site exchange to transfer-of-saturation profiles at two radiofrequency field strengths gives an estimate for k(off) of 73 s(-1) and transiently bound monomer (1)H(N) R(2) rates of up to 42,000 s(-1) in the tightly bound central hydrophobic region and approximately 300 s(-1) in the disordered regions, such as the first nine residues. The fraction of peptide within the "dark" oligomeric state undergoing exchange with free monomer is calculated to be approximately 3%.
最近的研究表明,淀粉样β(Abeta)肽的非纤维状寡聚物是阿尔茨海默病中主要的毒性物质。然而,这些状态的详细结构和动力学特征很难确定。在这里,我们使用 NMR 弛豫测量来研究 Abeta(1-40)单体和大的、多态寡聚物之间交换的动力学。在建立单体和 NMR 不可见的可溶性寡聚物之间的稳定假平衡后,记录了多个磁场下几种肽浓度的 (15)N 和 (1)H(N)R(2)数据。(15)N 和 (1)H(N)R(2) 速率随蛋白浓度的增加与核和磁场无关,并且仅沿肽链表现出很小的变化。这种现象是由于单体向 NMR 不可见的寡聚物物种(“暗”态)的单向转化引起的寿命展宽效应所致。在总 Abeta(1-40)浓度为 300 μM 时,该过程的表观一级速率常数约为 3 s(-1)。将 McConnell 方程拟合到两个双偶极耦合自旋在两个位点交换中的两个射频场强度下的饱和传递谱,给出了 k(off)的估计值为 73 s(-1),以及在紧密结合的中央疏水区中瞬态结合单体的 (1)H(N)R(2)速率高达 42,000 s(-1),在无序区域,如前九个残基中约为 300 s(-1)。与游离单体进行交换的肽的“暗”寡聚物状态的分数约为 3%。