Nekouzadeh Ali, Rudy Yoram
Cardiac Bioelectricity and Arrhythmia Center, Washington University in St. Louis, 290 Whitaker Hall, Campus Box 1097, One Brooking Drive, St. Louis, MO 63130-4899, USA.
Math Biosci. 2007 Nov;210(1):291-314. doi: 10.1016/j.mbs.2007.04.004. Epub 2007 May 4.
Macroscopic ion channel current can be derived by summation of the stochastic records of individual channel currents. In this paper, we present two probability density functions of single channel records that can uniquely determine the macroscopic current regardless of other statistical properties of records or the stochastic model of channel gating (presented often with stationary Markov models). We show that H(t), probability density function of channel opening events (introduced explicitly in this paper), and D(t), probability density function of the open duration (sometimes has named dwell time distribution as well), determine the normalized macroscopic current, G(t), through G(t) = P(t) - H(t) * Q(t) where P(t) is the cumulative density function of H(t), Q(t) is the cumulative density function of D(t), * is the symbol of convolution integral and G(t) is the macroscopic current divided by the amplitude of single channel current and the number of single channel sweeps. Compared to other equations for the macroscopic current, here the macroscopic current is expressed only in terms of the statistical properties of single channel current and not the stochastic model of ion channel gating or a conditioned form of macroscopic current. Single channel currents of an inactivating BK channel were used to validate this relationship experimentally too. In this paper, we used median filters as they can remove the unwanted noise without smoothing the transitions between open and closed states (compare to low pass filters). This filtering leads to more accurate measurement of transition times and less amount of missed events.
宏观离子通道电流可通过对单个通道电流的随机记录进行求和得到。在本文中,我们给出了单通道记录的两个概率密度函数,它们能够唯一地确定宏观电流,而无需考虑记录的其他统计特性或通道门控的随机模型(通常用平稳马尔可夫模型表示)。我们表明,通道开放事件的概率密度函数H(t)(本文中明确引入)和开放持续时间的概率密度函数D(t)(有时也称为驻留时间分布),通过G(t) = P(t) - H(t) * Q(t)来确定归一化宏观电流G(t),其中P(t)是H(t)的累积密度函数,Q(t)是D(t)的累积密度函数,*是卷积积分符号,G(t)是宏观电流除以单通道电流幅度和单通道扫描次数。与其他宏观电流方程相比,这里宏观电流仅根据单通道电流的统计特性来表示,而不是离子通道门控的随机模型或宏观电流的条件形式。失活型BK通道的单通道电流也被用于通过实验验证这种关系。在本文中,我们使用中值滤波器,因为它们可以去除不需要的噪声,而不会平滑开放和关闭状态之间的转换(与低通滤波器相比)。这种滤波导致更准确地测量转换时间,并且错过事件的数量更少。