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J Neurophysiol (November 1, 2002). 10.1152/jn.00237.2002
Submitted on 1 April 2002
Accepted on 24 July 2002
1Swammerdam Institute for Life Sciences, Section Neurobiology, University of Amsterdam, 1098 SM Amsterdam, The Netherlands; and 2Department of Cell Biology, Duke University Medical Center, Durham, North Carolina 27710
Kager, H.,
W. J. Wadman, and
G. G. Somjen.
Conditions for the Triggering of Spreading Depression Studied
With Computer Simulations. J. Neurophysiol. 88: 2700-2712, 2002. In spite of five decades of study, the
biophysics of spreading depression (SD) is incompletely understood.
Earlier we have modeled seizures and SD, and we have shown that
currents through ion channels normally present in neuron membranes can
generate SD-like depolarization. In the present study, we define the
conditions for triggering SD and the parameters that influence its
course in a model of a hippocampal pyramidal cell with more complete representation of ions and channels than the previous version. "Leak" conductances for Na+,
K+, and Cl
and an ion
pump were present in the membrane of the entire cell; fast
inactivating voltage dependent conductances for sodium and potassium in
the soma; "persistent" conductances in soma and apical dendrite,
and K+- and voltage-dependent
N-methyl-D-aspartate (NMDA)-controlled conductance in the apical dendrite. The neuron was surrounded by
restricted interstitial space and by a "glia-endothelium" system of
extracellular ion regulation bounded by a membrane having leak conductances and an ion pump. Ion fluxes and concentration changes were
continuously computed as well as osmotic cell volume changes. As long
as reuptake into the neuron and "buffering" by glia kept pace with
K+ released from the neuron, stimulating current
applied to the soma evoked repetitive firing that stopped when
stimulation ceased. When glial uptake was reduced,
K+ released from neurons could accumulate in the
interstitium and keep the neuron depolarized so that strong
depolarizing pulses injected into the soma were followed either by
afterdischarge or SD. SD-like depolarization was ignited when
depolarization spreading into the apical dendrite, activated persistent
Na+ current and NMDA-controlled current. With
membrane parameters constant, varying the injected stimulating current
influenced SD onset but neither the depolarization nor the increase in
extracellular K+. Glial "leak" conductance
influenced SD duration and SD ignition point. Varying maximal
conductances (representing channel density) also influenced SD onset
time but not the amplitude of the depolarization. Hypoxia was simulated
by turning off the Na-K exchange pump, and this resulted in SD-like
depolarization. The results confirm that, once ignited, SD runs an
all-or-none trajectory, the level of depolarization is governed by
feedback involving ion shifts and glutamate acting on ion channels and
not by the number of channels open, and SD is ignited if the net
persistent membrane current in the apical dendrites turns inward.
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