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De Schutter: Purkinje Cell Model

Estimates of Model Parameters

The Hodgkin-Huxley equations employed by this model require detailed information on channel kinetics and peak conductances. In principle, all of these data should be obtained from the cell being simulated. However, all the necessary data are rarely available for any particular neuron. For this reason it is usually necessary to obtain kinetic information from a variety of sources.

Estimating channel conductances

Constructing an accurate representation of an ionic channel also requires an estimate of the channel ˉg . However, channel conductance values measured in voltage-clamp experiments are often quite variable [8] and are only indicative. For this reason, channel gˉ s in the model were not based on experimental measurements [12].

Estimating channel densities

Having established and parameterized the equations governing the voltage-dependent behavior of the ionic conductances in this cell, it was necessary to determine the channel densities in the model. Because precise information on channel densities is not technically obtainable, channel densities, usually expressed as ˉg , are largely a free parameter in detailed single-cell models [14710].

Estimates of other parameters for ionic channels

Constructing an accurate representation of an ionic channel also requires an estimate of the channel ˉg . However, channel conductance values measured in voltage-clamp experiments are often quite variable [8] and are only indicative. For this reason, channel gˉ s in the model were not based on experimental measurements [12].

Temperature dependence of channel kinetics

Temperature is a well-known critical parameter for channel kinetics [3]. In the current simulations the in vivo and in vitro data used to tune the model were collected at 37 C whereas all of the published voltage-clamp data were obtained at room temperature. Assuming a Q 10 factor of 3 [5] all rate constants were multiplied by a factor of 5.

Modeling calcium concentrations

In the present model realistic simulation of Ca2+ concentrations was not attempted. However, computation of Ca2+ concentrations was required to activate the KC and K2 channels. Because these channels are assumed to be sensitive to the quickly changing, high Ca2+ concentrations just below the membrane surface [6], Ca2+ concentrations were computed in a thin submembrane shell [9]. These shells integrated the full Ca2+ inflow through the CaP and CaT channels. Their volume and decay time constants were initially free parameters in the model. The model tuning resulted in shells 0.2 μm deep with a decay time of 0.1 ms. The basal internal Ca2+ concentration was 0.040 μM; the outside concentration was constant at 2.4 mM. These concentrations were also used to compute Nernst potentials [3] for the CaP and CaT currents.

References

[1]   US Bhalla and JM Bower. Exploring parameter space in detailed single neuron models: Simulations of the mitral and granule cells of the olfactory bulb. Journal of Neurophysiology, 6:1948–1965, 1993.

[2]   E De Schutter, JD Angstadt, and RL Calabrese. A model of graded synaptic transmission for use in dynamic network simulations. Journal of Neurophysiology, 69:1225–1235, 1993.

[3]   B Hille. Ionic Channels of Excitable Membranes. Sunderland MA: Sinauer, 1991.

[4]   Calabrese R L and De Schutter E. Motor pattern generating networks in invertebrates: Modeling our way toward understanding. Trends in Neurosciences, 15:439–445, 1992.

[5]   Hodgkin A L and Huxley A F. A quantative description of membrane current and its application to conduction and excitation in nerve. Journal of Physiology (Lond.), 117:500–544, 1952.

[6]   L Lanḍ and RS Zucker. Caged calcium in aplasia pacemaker neurons—characterization of calcium-activated potassium and nonspecific cation channels. Journal of General Physiology, 93:1017–1060, 1989.

[7]   WW Lytton and TJ Sejnowski. Simulations of cortical pyramidal neurons synchronized by inhibitory interneurons. Journal of Neurophysiology, 66:1059–1079, 1991.

[8]   DA McCormick and JR Huguenard. A model of the electrophysiological properties of thalamocortical relay neurons. Journal of Neurophysiology, 68:1384–1400, 1992.

[9]   RD Traub. Simulation of intrinsic bursting in CA3 hippocampal neurons. Neuroscience, 7:1233–1242, 1982.

[10]   RD Traub, RKS Wong, R Miles, and H Michelson. A model of a CA3 hippocampal pyramidal neuron incorporating voltage-clamp data on intrinsic conductances. Journal of Neurophysiology, 66:635–650, 1991.