The influence of the chloride currents on action potential firing and volume regulation of excitable cells studied by a kinetic model
Introduction
Action potentials (APs) represent elevations of the membrane potential from a typical resting value of about −70 mV to a peak value of about +40 mV within a few milliseconds, followed by an equally fast decline back to the resting value. During an AP, voltage-gated membrane channels for small ions such as Na+ and K+ open and close in a timely well-coordinated fashion to enable transient extra currents of these ions along their concentration gradients: Sodium ions enter the cell and potassium ions flow into the extracellular space. Changes of the membrane potential feed back not only to voltage-gated ion channels but also to the electro-diffusion of ions through passive channels, in particular chloride channels, which in most excitable cells possess a high resting conductivity. Shifts in the trans-membrane distribution of , and occurring during an AP have to be reset by active ion transport. If this resetting has not been completed before a new AP is elicited, the perturbation of small-ion gradients across the membrane may successively progress during a series of APs (spike train).
Progressive changes of trans-membrane ion gradients during excitation may induce volume changes (Andrew and MacVicar, 1994, Ballanyi et al., 1990, Hill, 1950). In the brain, swelling of neurons can be critical as it further reduces the small interstitial space and hence raises the external potassium concentration. This causes a shift of the membrane potential toward the firing threshold and thus increases excitability, which at the extreme can ignite seizures, spreading depression (SD) or hypoxic SD-like depolarization (Andrew, 1991, Kager et al., 2007).
For the regulation of the cell volume chloride is very prominent (Jentsch, 1996), as membrane currents of this negative and diffusible small ion may rapidly compensate additional anion currents. The basal chloride permeability is also an important determinant of the firing threshold. In many excitable cells as well as in the non-dendritic parts of the neuron, the cellular chloride concentration is mainly controlled by passive chloride currents implying that the reversal potential of chloride is very close to the cell's resting membrane potential. Thus, initial depolarization by excitatory cation currents causes a counteracting inward directed chloride current. As a consequence, in order to reach a depolarization that is sufficient to open voltage-gated sodium channels, increasing chloride permeabilities entail higher excitatory currents. An important exception from this general behavior is the postsynaptic membrane of GABAergic neurons. Here, active transport of chloride is indispensable for the corresponding membrane region to either hyperpolarize (inhibitory synapse) or depolarize (excitatory synapse) upon neurotransmitter-gated opening of chloride channels (Coull et al., 2003, Kahle et al., 2008, Woo et al., 2002, Zhu et al., 2008).
In this work we present a detailed computational study on the impact of chloride currents on the volume regulation and firing pattern of excitable cells. The mathematical model used to simulate temporal changes in the intra- and extracellular concentrations of Na+, K+ and Cl‐ couples changes of ion concentrations to trans-membrane ion currents mediated by active ion pumps, non-gated and voltage-gated ion channels and membrane permeabilities. The simulations correctly recapitulate observed volume changes of active neuronal cells and the hyper-excitability of muscle cells underlying the neuromuscular disease myotonia congenita. The simulations also predict a number of novel and hitherto experimentally unstudied effects that a variable passive chloride permeability may have on the frequency, shape and duration of spike trains. Based on our theoretical findings we hypothesize that variations of the chloride permeability may represent a hitherto underestimated mechanism to tailor neuron responsiveness to specific profiles of excitatory stimuli.
Section snippets
Description of the mathematical model
The model describes the dynamics of the three ion species , and in a model cell characterized by its spherical geometry and the types, membrane densities and kinetic properties of ion channels and ion pumps (in the following referred to as ‘cell’).
The model takes into account three types of trans-membrane ion transports: (i) passive ion transport mediated by non-gated ion channels, (ii) passive ion transport through voltage-gated (excitatory) ion channels and (iii) active transport of
Volume regulation of non-excitable cells
To illustrate the general role of chloride fluxes in changes of the cellular volume, we first applied our model to a non-excitable cell by putting the permeability constants for the gated potassium and sodium channels to zero, . In this case, our model comprises the same membrane processes as the model that Armstrong (2003) proposed to simulate the impact of the and chloride on the osmotic stabilization of the cell. It has to be noted, however, that our simulations
Discussion
Every action potential is accompanied by a transient perturbation of trans-membrane ion distributions. Incomplete nullification of this perturbation between successive action potentials may give rise to cell swelling and distort the shape and frequency of action potentials or the duration of AP firing. Such alterations would interfere with the capability of an excitable cell to respond in a precise and reproducible manner to incoming electric or humoral stimuli. To address this issue we have
Acknowledgement
S. Hoffmann was funded by Deutsche Forschungsgemeinschaft in SFB 618.
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