// Rubinstein model of Ranvier Node's action potentials as in // Rubinstein JT (1995) Biophys J 68: 779-785. // Mino H, Rubinstein JT, White JA (2002) Ann Biomed Eng 30: 578-587. // Bruce IC (2007) Ann Biomed Eng 35: 315-318; // Voltage is shifted so that resting voltage = 0 mV (the reversal of the leak) // This script simulates 1000 sweeps per stimulus and calculates // firing efficiency, mean firing time and firing time variance // 100 (nsim) simultaneous sweeps, 10 times // Lines 44, 60, 61, 112 and 113 are intended to make a voltage trace // It is advisable to reduce nsim before uncommenting them // // Coupled activation particles, 8-state Na channel // Diffusion Approximation with steady state values of variables in the random term nsim=100; gNa=0.02569*265; //mS/cm2 ENa=144; //mV Cm=0.0000714*265; Rm=1953.49/265; NNa=1000; Tstop=1; dt=0.001; //ms points = round(Tstop/dt) Idel=0; Idur=0.1; //ms, ms threshold=80; rand('normal'); NaNs=0; currents=[5:0.1:6.5]; Eff=[]; meanFT=[]; varFT=[]; NaNs=[]; tic() for curr=1:size(currents,'*') Iamp=ones(1,nsim)*currents(curr); firetimes=[]; NNaNs=0; for nn=1:10 p=1; // Uncomment this only with a small nsim // vrec = zeros(points,nsim); v = 0*ones(1,nsim); am=1.872*(v-25.41)./(1-exp((25.41-v)/6.06)); bm=3.973*(21-v)./(1-exp((v-21)/9.41)); ah=-0.549*(27.74+v)./(1-exp((v+27.74)/9.06)); bh=(22.57)./(1+exp((56-v)/12.5)); M=am./bm; H=ah./bh; statesum=(1+H).*(1+M)^3; s=[ones(1,nsim);3*M;3*M.^2;M.^3;H;3*M.*H;3*M.^(2).*H;M^(3).*H]./(ones(8,1)*statesum); firetime=zeros(1,nsim); firing=zeros(1,nsim); for t = dt:dt:Tstop //vrec(p,:) = v; //uncomment with small nsim //p=p+1; if or(~firing&v>=threshold) then ind=find(v>=threshold&~firing); firetime(ind)=t; firing(ind)=1; end am=1.872*(v-25.41)./(1-exp((25.41-v)/6.06)); bm=3.973*(21-v)./(1-exp((v-21)/9.41)); ah=-0.549*(27.74+v)./(1-exp((v+27.74)/9.06)); bh=(22.57)./(1+exp((56-v)/12.5)); Iapp=Iamp*(t>Idel&t<(Idel+Idur)); Imemb=-Iapp+gNa.*s(8,:).*(v-ENa)+v/Rm; // deterministic transition matrix transition=[3*am.*s(1,:)-(2*am+bm+ah).*s(2,:)+2*bm.*s(3,:)+bh.*s(6,:); 2*am.*s(2,:)-(2*bm+am+ah).*s(3,:)+3*bm.*s(4,:)+bh.*s(7,:); am.*s(3,:)-(3*bm+ah).*s(4,:)+bh.*s(8,:); -(3*am+bh).*s(5,:)+bm.*s(6,:)+ah.*s(1,:); 3*am.*s(5,:)-(2*am+bm+bh).*s(6,:)+2*bm.*s(7,:)+ah.*s(2,:); 2*am.*s(6,:)-(2*bm+am+bh).*s(7,:)+3*bm.*s(8,:)+ah.*s(3,:); am.*s(7,:)-(3*bm+bh).*s(8,:)+ah.*s(4,:)]; //The stochastic terms (R) are not function of state variables R=rand(10,nsim).*sqrt((dt/NNa)*[6*am.*bh.*bm.^3; 12*am.^(2).*bh.*bm.^2; 6*am.^(3).*bh.*bm; 2*ah.*bh.*bm.^3; 6*ah.*bh.*am.*bm.^2; 6*ah.*bh.*am.^(2).*bm; 2*ah.*bh.*am.^3; 6*am.*ah.*bm.^3; 12*am.^(2).*ah.*bm.^2; 6*am.^(3).*ah.*bm]./(ones(10,1)*((ah+bh).*(am+bm).^3))); //Stochastic terms that correspond to state variables 2-8 Wt=[-R(1,:)+R(2,:)+R(5,:); -R(2,:)+R(3,:)+R(6,:); -R(3,:)+R(7,:); R(8,:)-R(4,:); -R(8,:)+R(9,:)-R(5,:); -R(9,:)+R(10,:)-R(6,:); -R(10,:)-R(7,:)]; s(2:8,:)=s(2:8,:)+dt*transition+Wt; s(1,:)=ones(1,nsim)-sum(s(2:8,:),'r'); v=v-dt*Imemb/Cm; end printf("round %d Iamp %g\n",nn,currents(curr)) //clf //uncomment with small nsim //plot(dt:dt:Tstop,vrec) firetimes=[firetimes firetime]; NNaNs=NNaNs + sum(1*(isinf(v)|isnan(v))); end Eff=[Eff;size(find(firetimes<>0),'*')]; meanFT=[meanFT;mean(firetimes(find(firetimes<>0)))]; if size(find(firetimes<>0),'*')>1 then varFT=[varFT;variance(firetimes(find(firetimes<>0)))]; else varFT=[varFT;0]; end NaNs=[NaNs;NNaNs]; end realt=toc(); printf("time = %g\n",realt) write_csv([currents' Eff meanFT varFT NaNs],sprintf('EffN-Rb8DAss-N%g-dt%g-%gs.csv',NNa,dt,realt),',',".") scf(0); clf subplot(3,1,1) plot(currents,Eff) subplot(3,1,2) plot(currents,meanFT) subplot(3,1,3) plot(currents,varFT)