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FCT_Fig9.par
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%**********************************************************************************
%
% CalC version 4.9.8, script "FCT_Fig9.par"
% Victor Matveev, January 19, 2004
%
% "Facilitation through Buffer Saturation:
% Constraints on Endogenous Buffering Properties"
% V. Matveev, A. Sherman and R. Zucker
% Biophys. J. (2004) 86:2691-2709
%
% This script produces the data for the parameter-sweep plots in Fig. 9A. It is
% based on the "FCT_Fig5.par", corresponding to the mobile buffer case, and requires
% a command-line parameter specifying the buffering capacity (kappa0). To reproduce
% Fig. 9A, execute
%
% calc FCT_Fig9.par 500
%
% the resulting file will be called "FCT_vs_Btotal_and_kon_fixed500", and will consist
% of 8 data columns, in the format "Btotal kon P1at1 P5at1 P1at2 P5at2 P1at3 P5at3",
% where "P1ati" and "P5ati" are the sizes of the 1st and 5th [Ca2+] transients at
% site "i". Then start gnuplot, and type
%
% splot 'FCT_vs_Btotal_and_kon_fixed500' u 1:2:($6/$5) w lines
%
% This will make a surface plot of the ratio of the 6th and 5st columns, equal to
% the P5/P1 value at site "2".
%==================================================================================
%
% See Fig. 5 for the explanation of the setting below:
Buffer.D = 0.0 % Immobile buffer
kmin = 0.025 % The binding rate will vary from 0.025/(uM ms)
kmax = 0.5 % to 0.5/(uM ms)
dK = 0.025 % with steps of 0.025/(uM ms)
BTmin = 1000 % The buffer concentration will be varied from 1 mM
BTmax = 22000 % to 22 mM, with steps of 1 mM (22 steps total)
dB = 1000
% Name of the output file (see FCT_Fig5.par):
outfile = "FCT_vs_Btotal_and_kon_fixed" kappa
% Apart from the presence of a second buffer, the simulations are equivalent to
% the ones contained in "FCT_Fig5.par"
path = "" % If running under Windows, specify here the path to the
% directory containing the script imported below
fname = path "FCT_Fig5.par"
include fname % Import the simulation parameters from the main script,
% which defines everything but the buffer's parameters:
%==================================================================================