利用泊松-能-普朗克方程的轴突和细胞外空间的电扩散模型

Jurgis Pods
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This neglects a \nsecond, possibly important contributor to the extracellular field: the time- and position-dependent concentrations of ions in the intra- and extracellular fluids. \n \nIn this thesis, a 3D model of a single axon in extracellular fluid is presented based on the Poisson-Nernst-Planck (PNP) equations of electrodiffusion. This \nfundamental model includes not only the potential, but also the concentrations of all participating ion concentrations in a self-consistent way. This enables us to study the propagation of an action potential (AP) along the axonal membrane based on first principles by means of numerical simulations. By exploiting the cylinder symmetry of this geometry, the problem can be reduced to two dimensions. The numerical solution is implemented in a flexible and efficient way, using the DUNE framework. A suitable mesh generation strategy and a parallelization of the algorithm allow to solve the problem in reasonable time, with a high spatial and temporal resolution. The methods and programming \ntechniques used to deal with the numerical challenges of this multi-scale problem are presented in detail. \n \nSpecial attention is paid to the Debye layer, the region with strong concentration gradients close to the membrane, which is explicitly resolved by the computational mesh. The focus lies on the evolution of the extracellular electric \npotential at different membrane distances. Roughly, the extracellular space can be divided into three distinct regions: first, the distant farfield, which exhibits \na characteristic triphasic waveform in response to an action potential traveling along the membrane. This is consistent with previous modeling efforts and \nexperiments. Secondly, the Debye layer close to the membrane, which shows a completely different extracellular response in the form of an “AP echo”, which \nis also observed in juxtacellular recordings. Finally, there is the intermediate or diffusion layer located in between, which shows a gradual transition from the \nDebye layer potential towards the farfield potential. Both of these potentialregions show marked deviations from volume conductor models, which can be attributed to the redistribution of concentrations and associated ion fluxes. These differences are explained by analyzing the capacitive and ionic components of the potential. \n \nIn an extension, we also include myelination into the model, which has a significant impact on the extracellular field. 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引用次数: 6

摘要

在大脑和神经系统的研究中,通过局部场电位(LFPs)或脑电图(EEG)测量的细胞外信号非常重要,因为它们可以同时从多个神经元获得数据。然而,这些信号的确切生物物理基础仍未完全了解。目前,大多数细胞外电位模型都是基于体积导体理论,该理论假设细胞外液是电中性的,并且对电场的唯一贡献是由膜电流给出的,膜电流可以作为数学模型中的边界条件施加。这忽略了细胞外场的第二个可能重要的因素:细胞内和细胞外液中随时间和位置变化的离子浓度。本文基于电扩散的泊松-能-普朗克(PNP)方程,建立了细胞外液中单个轴突的三维模型。这个基本模型不仅包括电位,还包括所有参与离子浓度的自一致的浓度。这使我们能够基于第一性原理,通过数值模拟的方法研究动作电位沿轴突膜的传播。利用这种几何的圆柱对称性,问题可以简化为二维。利用DUNE框架,以一种灵活有效的方式实现了数值解。合适的网格生成策略和并行化算法可以在合理的时间内解决问题,具有较高的时空分辨率。详细介绍了用于处理这一多尺度问题的数值挑战的方法和编程技术。特别注意Debye层,即靠近膜的浓度梯度较强的区域,该区域由计算网格明确地分解。重点在于细胞外电位在不同膜距离上的演变。粗略地说,细胞外空间可以分为三个不同的区域:首先,远场,它表现出一个特征的三相波形,以响应沿膜传播的动作电位。这与之前的建模工作和实验一致。其次,靠近膜的Debye层表现出完全不同的细胞外反应,以“AP回声”的形式出现,这在细胞旁记录中也可以观察到。最后,中间层或扩散层位于两者之间,从德拜层电位逐渐过渡到远场电位。这两个电位区都显示出与体积导体模型的明显偏差,这可归因于浓度和相关离子通量的重新分布。这些差异是通过分析电势的电容和离子成分来解释的。在扩展中,我们还将髓鞘形成纳入模型,它对细胞外场有重大影响。再一次,数值结果与体积导体模型进行了比较。最后,进行了一个模型研究,以评估触觉效应的大小,即一个细胞的电场对相邻细胞的影响,在某种程度上是人造的几何形状。虽然在大多数生理情况下,结果可能无法定量解释,但定性行为显示出有趣的影响。一个轴突可以引起周围轴突束的动作电位,只要距离足够小,细胞外介质的电阻率显著增加。本研究的进一步结果是极大的细胞外电位,振幅高达100毫伏,以及一种不寻常的神经元放电模式,在这种模式下,细胞不是通过细胞内电位的增加而去极化,而是通过细胞外电位的减少。一些文献资料表明,这些观察结果与以往的研究是一致的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Electrodiffusion Models of Axon and Extracellular Space Using the Poisson-Nernst-Planck Equations
In studies of the brain and the nervous system, extracellular signals – as measured by local field potentials (LFPs) or electroencephalography (EEG) – are of capital importance, as they allow to simultaneously obtain data from multiple neurons. The exact biophysical basis of these signals is, however, still not fully understood. Most models for the extracellular potential today are based on volume conductor theory, which assumes that the extracellular fluid is electroneutral and that the only contributions to the electric field are given by membrane currents, which can be imposed as boundary conditions in the mathematical model. This neglects a second, possibly important contributor to the extracellular field: the time- and position-dependent concentrations of ions in the intra- and extracellular fluids. In this thesis, a 3D model of a single axon in extracellular fluid is presented based on the Poisson-Nernst-Planck (PNP) equations of electrodiffusion. This fundamental model includes not only the potential, but also the concentrations of all participating ion concentrations in a self-consistent way. This enables us to study the propagation of an action potential (AP) along the axonal membrane based on first principles by means of numerical simulations. By exploiting the cylinder symmetry of this geometry, the problem can be reduced to two dimensions. The numerical solution is implemented in a flexible and efficient way, using the DUNE framework. A suitable mesh generation strategy and a parallelization of the algorithm allow to solve the problem in reasonable time, with a high spatial and temporal resolution. The methods and programming techniques used to deal with the numerical challenges of this multi-scale problem are presented in detail. Special attention is paid to the Debye layer, the region with strong concentration gradients close to the membrane, which is explicitly resolved by the computational mesh. The focus lies on the evolution of the extracellular electric potential at different membrane distances. Roughly, the extracellular space can be divided into three distinct regions: first, the distant farfield, which exhibits a characteristic triphasic waveform in response to an action potential traveling along the membrane. This is consistent with previous modeling efforts and experiments. Secondly, the Debye layer close to the membrane, which shows a completely different extracellular response in the form of an “AP echo”, which is also observed in juxtacellular recordings. Finally, there is the intermediate or diffusion layer located in between, which shows a gradual transition from the Debye layer potential towards the farfield potential. Both of these potentialregions show marked deviations from volume conductor models, which can be attributed to the redistribution of concentrations and associated ion fluxes. These differences are explained by analyzing the capacitive and ionic components of the potential. In an extension, we also include myelination into the model, which has a significant impact on the extracellular field. Again, the numerical results are compared to volume conductor models. Finally, a model study is carried out to assess the magnitude of ephaptic effects, i.e. the influence of the electric field of one cell on a neighboring cell, in a somewhat artificial geometry. While the results probably can not be interpreted quantitatively in the majority of physiological situations, the qualitative behavior shows interesting effects. An axon can elicit an action potential in a surrounding bundle of axons, given that the distance is small enough and the resistivity of the extracellular medium is significantly increased. Further results of this study are extremely large extracellular potentials with amplitudes up to 100 mV and an unusual neuronal firing mode in which the cell is not depolarized by an increase in the intracellular potential, but by a decrease in the extracellular potential. Some literature references are given that show that these observations are consistent with previous studies.
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