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Realistic protein–protein association rates from a simple diffusional model neglecting long-range interactions free energy barriers and landscape ruggedness

机译:忽略远距离相互作用自由能垒和景观坚固性的简单扩散模型的真实蛋白质-蛋白质缔合速率

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摘要

We develop a simple but rigorous model of protein–protein association kinetics based on diffusional association on free energy landscapes obtained by sampling configurations within and surrounding the native complex binding funnels. Guided by results obtained on exactly solvable model problems, we transform the problem of diffusion in a potential into free diffusion in the presence of an absorbing zone spanning the entrance to the binding funnel. The free diffusion problem is solved using a recently derived analytic expression for the rate of association of asymmetrically oriented molecules. Despite the required high steric specificity and the absence of long-range attractive interactions, the computed rates are typically on the order of 104–106 M−1 sec−1, several orders of magnitude higher than rates obtained using a purely probabilistic model in which the association rate for free diffusion of uniformly reactive molecules is multiplied by the probability of a correct alignment of the two partners in a random collision. As the association rates of many protein–protein complexes are also in the 105–106 M−1 sec−1 range, our results suggest that free energy barriers arising from desolvation and/or side-chain freezing during complex formation or increased ruggedness within the binding funnel, which are completely neglected in our simple diffusional model, do not contribute significantly to the dynamics of protein–protein association. The transparent physical interpretation of our approach that computes association rates directly from the size and geometry of protein–protein binding funnels makes it a useful complement to Brownian dynamics simulations.
机译:我们建立了一个简单而严格的蛋白质-蛋白质缔合动力学模型,该模型基于通过对天然复合结合漏斗内和周围的配置取样而获得的自由能景观上的扩散缔合。以在完全可解决的模型问题上获得的结果为指导,在存在跨越结合漏斗入口的吸收区的情况下,我们将势能扩散问题转换为自由扩散问题。使用最近得出的不对称取向分子缔合速率的解析表达式可以解决自由扩散问题。尽管需要很高的空间特异性并且没有长期的吸引力相互作用,但计算出的速率通常约为10 4 –10 6 M -1 sec -1 ,比使用纯概率模型获得的速率高几个数量级,在纯概率模型中,均匀反应性分子自由扩散的缔合速率乘以两个伙伴发生随机碰撞。由于许多蛋白质-蛋白质复合物的缔合率也在10 5 –10 6 M -1 sec -1 < / sup>范围内,我们的结果表明,在简单的扩散模型中完全忽略了在复合物形成过程中由于去溶剂化和/或侧链冻结或结合漏斗中增加的坚固性而产生的自由能垒,并没有对动力学产生重大影响蛋白质之间的关系。对我们方法的透明物理解释,该方法直接根据蛋白质-蛋白质结合漏斗的大小和几何形状计算缔合率,使其成为布朗动力学模拟的有用补充。

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