Frehland E
Biophys Chem. 1978 Jul;8(3):255-65. doi: 10.1016/0301-4622(78)87007-0.
Subject of this paper is the transport noise in discrete systems. The transport systems are given by a number (n) of binding sites separated by energy barriers. These binding sites may be in contact outer reservoirs. The state of the systems is characterized by the occupation numbers of particles (current carriers) at these binding sites. The change in time of the occupation numbers is generated by individual "jumps" of particles over the energy barriers, building up the flux matter (for charged particles: the electric current). In the limit n leads to infinity continuum processes as e.g. usual diffusion are included in the transport model. The fluctuations in occupation numbers and other quantities linearly coupled to the occupation numbers may be treated with the usual master equation approach. The treatment of the fluctuation in fluxes (current) makes necessary a different theoretical approach which is presented in this paper under the assumption of vanishing interactions between the particles. This approach may be applied to a number of different transport systems in biology and physics (ion transport through porous channels in membranes, carriers mediated ion transport through membranes, jump diffusion e.g. in superionic conductors). As in the master equation approach the calculation of correlations and noise spectra may be reduced to the solution of the macroscopic equations for the occupation numbers. This result may be regarded as a generalization to non-equilibrium current fluctuations of the usual Nyquist theorem relating the current (voltage) noise spectrum in thermal equilibrium to the macroscopic frequency dependent admittance. The validity of the general approach is demonstrated by the calculation of the autocorrelation function and spectrum of current noise for a number of special examples (e.g. pores in membranes, carrier mediated ion transport).
本文的主题是离散系统中的输运噪声。输运系统由若干个被能垒隔开的束缚位点(数量为(n))给出。这些束缚位点可能与外部储库接触。系统的状态由这些束缚位点处粒子(载流子)的占据数来表征。占据数随时间的变化是由粒子在能垒上的单个“跳跃”产生的,从而形成物质通量(对于带电粒子:电流)。在(n)趋于无穷大的极限情况下,连续过程(例如通常的扩散)被纳入输运模型。占据数的涨落以及与占据数线性耦合的其他量可以用通常的主方程方法来处理。通量(电流)涨落的处理需要一种不同的理论方法,本文在粒子间相互作用可忽略的假设下给出了这种方法。这种方法可应用于生物学和物理学中的许多不同输运系统(离子通过膜中的多孔通道的输运、载体介导的离子通过膜的输运、例如在超离子导体中的跳跃扩散)。与主方程方法一样,关联和噪声谱的计算可以简化为占据数宏观方程的求解。这个结果可以看作是通常的奈奎斯特定理对非平衡电流涨落的推广,该定理将热平衡中的电流(电压)噪声谱与宏观频率相关导纳联系起来。通过对一些特殊例子(例如膜中的孔、载体介导的离子输运)的电流噪声自相关函数和谱的计算,证明了该一般方法的有效性。