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首页> 外文期刊>The Journal of Chemical Physics >Escape from a cavity through a small window: Turnover of the rate as a function of friction constant
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Escape from a cavity through a small window: Turnover of the rate as a function of friction constant

机译:通过一个小窗口从空腔中逸出:速率的变化与摩擦常数的关系

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To escape from a cavity through a small window the particle has to overcome a high entropy barrier to find the exit.As a consequence,its survival probability in the cavity decays as a single exponential and is characterized by the only parameter,the rate constant.We use simulations to study escape of Langevin particles from a cubic cavity through a small round window in the center of one of the cavity walls with the goal of analyzing the friction dependence of the escape rate.We find that the rate constant shows the turnover behavior as a function of the friction constant,zeta: The rate constant grows at very small zeta,reaches a maximum value which is given by the transition-state theory (TST),and then decreases approaching zero as zeta->infinity.Based on the results found in simulations and some general arguments we suggest a formula for the rate constant that predicts a turnover of the escape rate for ergodic cavities in which collisions of the particle with the cavity walls are defocusing.At intermediate-to-high friction the formula describes transition between two known results for the rate constant: the TST estimation and the high friction limiting behavior that characterizes escape of diffusing particles.In this range of friction the rate constants predicted by the formula are in good agreement with those found in simulations.At very low friction the rate constants found in simulations are noticeably smaller than those predicted by the formula.This happens because the simulations were run in the cubic cavity which is not ergodic.
机译:为了通过小窗口从腔中逃逸,粒子必须克服高熵屏障才能找到出口。结果,粒子在腔中的生存概率以单指数衰减,并且由唯一的参数速率常数表征。为了模拟逃逸速率的摩擦依存性,我们通过模拟研究了兰氏蛋白颗粒从立方腔通过一个腔壁中心的小圆形窗口逃逸的过程,发现速率常数显示了周转行为根据摩擦常数zeta:速率常数在非常小的zeta处增长,达到过渡状态理论(TST)给出的最大值,然后随着zeta-> infinity减小到零。在模拟和一些一般性论证中发现的结果,我们提出了一个速率常数的公式,该公式可预测遍历腔的逃逸率的周转率,其中粒子与腔壁的碰撞被限定在中高摩擦状态下,该公式描述了速率常数的两个已知结果之间的过渡:TST估算和表征扩散粒子逸出的高摩擦极限行为。在此摩擦范围内,公式所预测的速率常数与模拟中的数值非常吻合。在非常低的摩擦下,模拟中的速率常数明显小于公式所预测的常数,这是因为模拟是在非遍历的立方腔中进行的。

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