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Theory of the diffusion-influenced substrate binding rate to a buried and gated active site

机译:扩散影响底物与掩埋和门控活性位点结合率的理论

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The effects of stochastic gating on the diffusion-influenced substrate binding rate to a buried active site are studied. An approximation introduced by Samson and Deutch [J. Chem. Phys. 68, 285 (1978)] is shown to be equivalent to making the constant-flux approximation on the entrance to the active site. The constant-flux approximation is then extended to the case where the entrance to the active site is stochastically gated because of conformational fluctuations of the enzyme. The stochastically gated rate constant, k(sg), is found to be given by the relation 1/k(sg) = 1/k + w(o)/w(c)(w(o) + w(c))(h) over cap(w(o) + w(c)), where k is the rate constant in the absence of gating, (h) over cap(s) is the Laplace transform of the total flux across the entrance after the substrate is started from an equilibrium distribution outside the entrance, and w(o) and w(c) are the transition rates between the open and closed gating states. This relation reduces to an approximate relation derived earlier for a more restrictive situation, where the reactivity within the active site is gated. The leading term in the expansion of s (h) over cap(s) for large s is DA[exp(-beta U)](s/D)(1/2)/2, where D is the diffusion coefficient of the substrate, A is the total area of the entrance, and [exp(-beta U)] is the average Boltzmann factor on the entrance. The time scale of conformational fluctuations, similar to a few picoseconds, is much shorter than the time scale of diffusion, so this leading term is useful for estimating (w(o) + w(c))(h) over cap(w(o) + w(c)). A further consequence of the disparity in time scales is that the value of (w(o) + w(c))(h) over cap(w(o) + w(c)) is much larger than k. As a result the decrease of the rate constant due to gating is relatively small (unless the entrance to the active site is closed nearly all the time). This suggests that a buried and gated active site may play the important role of controlling enzyme specificity without sacrificing efficiency. (C) 1998 American Institute of Physics. [References: 31]
机译:研究了随机门控对扩散影响的底物与掩埋的活性位点的结合率的影响。由Samson和Deutch提出的近似值[J.化学物理68,285(1978)]显示等效于在活动站点的入口处进行恒定通量近似。然后,将恒定通量近似扩展到由于酶的构象波动而使随机进入活性位点的情况。发现随机门控速率常数k(sg)由以下关系式给定:1 / k(sg)= 1 / k + w(o)/ w(c)(w(o)+ w(c)) (h)超过上限(w(o)+ w(c)),其中k是没有门控时的速率常数,(h)超过上限(s)是经过入口后总通量的拉普拉斯变换基板从入口外部的平衡分布开始,并且w(o)和w(c)是打开和关闭门控状态之间的过渡速率。该关系简化为较早得出的近似关系,适用于限制性较高的情况,其中活动位点内的反应性受到控制。对于较大的s,s(h)在盖帽上的展开的最主要项是DA [exp(-beta U)](s / D)(1/2)/ 2,其中D是物体的扩散系数。底物,A是入口的总面积,[exp(-beta U)]是入口的平均玻尔兹曼因子。构象波动的时间尺度类似于几皮秒,比扩散的时间尺度短得多,因此,该前导项对于估计在上限(w(w(w)+ w(c))(h) o)+ w(c))。时间尺度差异的另一个结果是,在上限(w(o)+ w(c))上的(w(o)+ w(c))(h)的值远大于k。结果,由于选通而导致的速率常数的减小相对较小(除非活动位置的入口几乎始终关闭)。这表明掩埋和门控的活性位点可能在不牺牲效率的情况下起控制酶特异性的重要作用。 (C)1998美国物理研究所。 [参考:31]

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