TITLE R-type calcium channel for nucleus accumbens neuron : see comments at end of file UNITS { (mV) = (millivolt) (mA) = (milliamp) (S) = (siemens) (molar) = (1/liter) (mM) = (millimolar) FARADAY = (faraday) (coulomb) R = (k-mole) (joule/degC) } NEURON { SUFFIX car USEION ca READ cai, cao WRITE ica RANGE pcarbar, ica } PARAMETER { pcarbar = 2.6e-5(cm/s) : vh = 100 mV, 120 ms pulse to 0 mv mvhalf = -10.3 (mV) : Churchill 1998, fig 7 mslope = -6.6 (mV) : Churchill 1998, fig 7 mtau = 5.1 (ms) : Foehring 2000, pg 2230 mshift = 9.163 (mV) hvhalf = -33.3 (mV) : Foehring 2000, fig 7C hslope = 17.0 (mV) : Foehring 2000, fig 7 hshift = 11.819 (mV) qfact = 2.16 : both m & h recorded at 22 C } ASSIGNED { v (mV) ica (mA/cm2) eca (mV) celsius (degC) cai (mM) cao (mM) minf hinf } STATE { m h } BREAKPOINT { SOLVE states METHOD cnexp ica = ghk(v,cai,cao) * pcarbar * m * m * m * h : Wang 1991 } : the current looks similar to t-type INITIAL { settables(v) m = minf h = hinf } DERIVATIVE states { settables(v) m' = (minf - m) / (mtau/qfact) h' = (hinf - h) / (htau(v)/qfact) } FUNCTION_TABLE htau(v(mV)) (ms) : Brevi 2001 fig 11 PROCEDURE settables( v (mV) ) { TABLE minf, hinf DEPEND mshift, hshift FROM -100 TO 100 WITH 201 minf = 1 / ( 1 + exp( (v-mvhalf-mshift) / mslope) ) hinf = 1 / ( 1 + exp( (v-hvhalf-hshift) / hslope) ) } :::::::::::::::::::::::::::::::::::::::::::::::::::::::::::::: : ghk() borrowed from cachan.mod share file in Neuron FUNCTION ghk(v(mV), ci(mM), co(mM)) (.001 coul/cm3) { LOCAL z, eci, eco z = (1e-3)*2*FARADAY*v/(R*(celsius+273.15)) eco = co*efun(z) eci = ci*efun(-z) :high cao charge moves inward :negative potential charge moves inward ghk = (.001)*2*FARADAY*(eci - eco) } FUNCTION efun(z) { if (fabs(z) < 1e-4) { efun = 1 - z/2 }else{ efun = z/(exp(z) - 1) } } COMMENT Churchill D, Macvicar BA (1998) Biophysical and pharmacological characterization of voltage-dependent Ca2+ channels in neurons isolated from rat nucleus accumbens. J Neurophysiol 79:635-647. Foehring RC, Mermelstein PG, Song WJ, Ulrich S, Surmeier DJ (2000) Unique properties of R-type calcium currents in neocortical and neostriatal neurons. J Neurophysiol 84:2225-2236. Wang XJ, Rinzel J, Rogawski MA (1991) A model of the T-type calcium current and the low-threshold spike in thalamic neurons. J Neurophysiol 66:839-850. Koch, C., and Segev, I., eds. (1998). Methods in Neuronal Modeling: From Ions to Networks, 2 edn (Cambridge, MA, MIT Press). Hille, B. (1992). Ionic Channels of Excitable Membranes, 2 edn (Sunderland, MA, Sinauer Associates Inc.). Brevi S, de Curtis M, Magistretti J (2001) Pharmacologial and biophysical characterization of voltage-gated calcium currents in the endopiriform nucleus of the guinea pig. J Neuophysiol 85:2076-2087. This is the toxin-resistant current in fig 7 from Churchill. The standard HH model uses a linear approximation to the driving force for an ion: (Vm - ez). This is ok for na and k, but not ca - calcium rectifies at high potentials because 1. internal and external concentrations of ca are so different, making outward current flow much more difficult than inward 2. calcium is divalent so rectification is more sudden than for na and k. (Hille 1992, pg 107) Accordingly, we need to replace the HH formulation with the GHK model, which accounts for this phenomenon. The GHK equation is eq 6.6 in Koch 1998, pg 217 - it expresses Ica in terms of Ca channel permeability (Perm,ca) times a mess. The mess can be circumvented using the ghk function below, which is included in the Neuron share files. Perm,ca can be expressed in an HH-like fashion as Perm,ca = pcabar * mca * mca (or however many m's and h's) where pcabar has dimensions of permeability but can be thought of as max conductance (Koch says it should be about 10^7 times smaller than the HH gbar - dont know) and mca is analagous to m (check out Koch 1998 pg 144) Calcium current can then be modeled as ica = pcabar * mca * mca * ghk() Jason Moyer 2004 - jtmoyer@seas.upenn.edu ENDCOMMENT