- Author:
- Shelley Fong <s.fong@auckland.ac.nz>
- Date:
- 2022-04-22 11:17:29+12:00
- Desc:
- Changing units to s for alpha and beta gate parameters
- Permanent Source URI:
- https://models.cellml.org/workspace/831/rawfile/e7c127c432a07fe8bbb82b7967315cb200f6494d/parameter_finder/find_BG_parameters.py
# This script calculates the bond graph parameters for all reactions of the
# a given module. Specify the directory.
# based on SERCA model of Pan et al, which is based on Tran et al. (2009).
# Parameters calculated in module's directory, by using the kinetic
# parameters and stoichiometric matrix.
# return W from kinetic_parameters
import os
import csv
import json
import math
import numpy as np
import sympy
from sympy import Matrix, S, nsimplify
from scipy.linalg import null_space
from fractions import Fraction
def read_IDs(path):
data = []
with open(path, 'r') as f:
reader = csv.reader(f)
for row in reader:
data.append(row[0])
f.close()
return data
def load_matrix(stoich_path):
matrix = []
with open(stoich_path, 'r') as f:
reader = csv.reader(f, delimiter=',')
for row in reader:
matrix.append([float(r) for r in row])
f.close()
return matrix
# def rational_nullspace(A, max_denom = 10):
# v = null_space(A)
# vFrac = [[Fraction(num).limit_denominator(max_denominator=max_denom) for num in row] for row in v]
#
# vRat = [] #np.zeros([len(vFrac),len(vFrac[0])])
# if not v.any():
# return []
# all_denom = [[res.denominator for res in row] for row in vFrac]
# if all_denom.count(all_denom[0]) == len(all_denom):# identical
# for row in vFrac:
# largest_denom = max([res.denominator for res in row])
# vRat.append( [vi.numerator for vi in row] )
# return vRat
# else:
# print('denominators for fractions of rational nullspace are not identical')
# return []
if __name__ == "__main__":
## booleans
write_parameters_file = True
include_constraints = True
include_type2_reactions = True
## Set directories
current_dir = os.getcwd()
data_dir = current_dir + '\data'
output_dir = current_dir + '\output'
modname = os.path.dirname(current_dir).split('\\')[-1].split('BG_')[-1]
if not os.path.exists(output_dir):
os.mkdir(output_dir)
if ('beta1' in current_dir) and False:
matstr = '_withR_LR_scheme4'
else:
matstr = ''
## Define constants
R = 8.314 # unit J / mol / K
T = 310
F = 96485
cNao = 140 # unit mM
cNai = 10 # unit mM
cKo = 5.4
cKi = 145
N_A = 6.022e23
A_cap = 1.534e-4 # Unit cm ^ 2
Cm = 60e-6 # [ =] uF
SA = 1100 # um2, Kernik iPSC
TCC_density = 6 # from Pan [=] 1/um2
numChannels = TCC_density*SA # number of channels per cell
V_myo = 3.71 # pL, for Kernik iPSCell
V_o = V_myo*0.88 # Using cleft volume calc from LRd
V = dict()
V['V_myo'] = V_myo
V['V_o'] = V_o
V['F'] = F
V['R'] = R
V['T'] = T
V['Cm'] = Cm
V['N_A'] = N_A
V['A_cap'] = A_cap
V['cNao'] = cNao
V['cNai'] = cNai
V['cKi'] = cKi
V['cKo'] = cKo
V['numChannels'] = numChannels
## Load forward matrix
if include_type2_reactions:
stoich_path = data_dir + '\\all_forward_matrix%s.txt' % matstr
else:
stoich_path = data_dir + '\\all_noType2_forward_matrix.txt'
N_f = load_matrix(stoich_path)
## Load reverse matrix
if include_type2_reactions:
stoich_path = data_dir + '\\all_reverse_matrix%s.txt' % matstr
else:
stoich_path = data_dir + '\\all_noType2_reverse_matrix.txt'
N_r = load_matrix(stoich_path)
N_fT = np.transpose(N_f)
N_rT = np.transpose(N_r)
## Calculate stoichiometric matrix
# I matrix to align with placement of kappa down the column.
# x-axis of stoich matrix (R1a, R1b etc) coincides with the kp km of that kinetic reaction
N = [[N_r[j][i] - N_f[j][i] for i in range(len(N_f[0]))] for j in range(len(N_f))]
N_T = [[N_rT[j][i] - N_fT[j][i] for i in range(len(N_fT[0]))] for j in range(len(N_fT))]
num_rows = len(N)
num_cols = len(N[0])
dims = dict()
dims['num_rows'] = num_rows
dims['num_cols'] = num_cols
I = np.identity(num_cols)
M = np.append(np.append(I, N_fT, 1), np.append(I, N_rT, 1), 0)
func = __import__('kinetic_parameters_%s' % modname)
[k_kinetic, N_cT, K_C, W] = func.kinetic_parameters(M, include_type2_reactions, dims, V)
if not include_constraints:
N_cT = []
try:
M = np.append(M, N_cT, 0)
k = np.append(k_kinetic, K_C, 0)
except:
k = k_kinetic
# Calculate bond graph constants from kinetic parameters
# Note: units of kappa are fmol/s, units of K are fmol^-1
lambda_expo = np.matmul(np.linalg.pinv(M), [math.log(ik) for ik in k])
lambdaW = [math.exp(l) for l in lambda_expo]
# Check that kinetic parameters are reproduced by bond graph parameters
k_est = np.matmul(M, [math.log(k) for k in lambdaW])
k_est = [math.exp(k) for k in k_est]
diff = [(k[i] - k_est[i]) / k[i] for i in range(len(k))]
error = np.sum([abs(d) for d in diff])
# Checks
N_rref = sympy.Matrix(N).rref()
R = nsimplify(Matrix(N), rational=True).nullspace() # rational_nullspace(N, max_denom=len(N[0]))
if R:
R = np.transpose(np.array(R).astype(np.float64))[0]
# Check that there is a detailed balance constraint
Z = nsimplify(Matrix(M), rational=True).nullspace() # rational_nullspace(M, 2)
if Z:
Z = np.transpose(np.array(Z).astype(np.float64))[0]
kf = k_kinetic[:num_cols]
kr = k_kinetic[num_cols:]
K_eq = [kf[i] / kr[i] for i in range(len(kr))]
try:
zero_est = np.matmul(np.transpose(R), K_eq)
zero_est_log = np.matmul(np.transpose(R), [math.log(k) for k in K_eq])
except:
print('undefined R nullspace')
# if not R_mat:
# warning('R_mat is empty: matrix is full rank')
lambdak = [lambdaW[i] / W[i] for i in range(len(W))]
kappa = lambdak[:len(N[0])]
K = lambdak[len(N[0]):]
rxnID = read_IDs('data\\rxnID.txt')
Kname = read_IDs('data\\Kname.txt')
zname = read_IDs('data\\zname.txt')
zval = read_IDs('data\\z_value.txt')
# ### print outputs ###
for ik in range(len(kappa)):
print('var kappa_%s: fmol_per_sec {init: %g, pub: out};' % (rxnID[ik], kappa[ik]))
for ik in range(len(Kname)):
print('var K_%s: per_fmol {init: %g, pub: out};' % (Kname[ik], K[ik]))
for ik in range(len(zname)):
print('var %s: dimensionless {init: %s, pub: out};' % (zname[ik], zval[ik]))
file = open(output_dir + '/all_parameters_out.json', 'w')
data = {"K": K, "kappa": kappa, "k_kinetic": k_kinetic}
json.dump(data, file)
cellmlfilepath = os.getcwd() + '\\output\\TEMP.cellml.txt'
with open(cellmlfilepath, 'w') as cid:
cid.write('def model individual_%s as\n def import using "units_and_constants/units_BG.cellml" for\n\
unit mM using unit mM;\nunit fmol using unit fmol;\nunit per_fmol using unit per_fmol;\n\
unit J_per_mol using unit J_per_mol;\nunit fmol_per_sec using unit fmol_per_sec;\n\
unit C_per_mol using unit C_per_mol;\n unit J_per_C using unit J_per_C;\n\
unit microm3 using unit microm3;\n unit fF using unit fF;\n\
unit fC using unit fC;\n unit fA using unit fA;\n\
unit per_second using unit per_second;\n unit millivolt using unit millivolt;\n\
unit per_sec using unit per_sec;\n unit J_per_K_per_mol using unit J_per_K_per_mol;\n\
unit fmol_per_L using unit fmol_per_L;\n unit fmol_per_L_per_sec using unit fmol_per_L_per_sec;\n\
unit per_sec_per_fmol_per_L using unit per_sec_per_fmol_per_L;\n unit uM using unit uM;\n\
unit mM_per_sec using unit mM_per_sec;\n unit uM_per_sec using unit uM_per_sec;\n\
unit pL using unit pL;\n unit m_to_u using unit m_to_u;\n enddef;\n' % (modname))
cid.write('def import using "units_and_constants/constants_BG.cellml" for\n\
comp constants using comp constants;\nenddef;\n\n')
cid.write(" def comp environment as\n\
var time: second {pub: out};\n\
// initial values\n")
for Kn in Kname:
cid.write('var q_%s: fmol {init: 1e-888, pub: out};\n' % (Kn))
# cid.write('// Global value\n')
# for Kn in Kname:
# cid.write('var q_%s: fmol {pub: out};\n'%Kn)
cid.write('// From submodule\n')
for rx in rxnID:
cid.write('var v_%s: fmol_per_sec {pub: in};\n' % (rx))
for Kn in Kname:
cid.write('ode(q_%s, time) = vvv;\n' % (Kn))
cid.write('enddef;\n\n')
cid.write('def comp %s_parameters as\n' % (modname))
for ik in range(len(kappa)):
cid.write('var kappa_%s: fmol_per_sec {init: %g, pub: out};\n' % (rxnID[ik], kappa[ik]))
for ik in range(len(Kname)):
cid.write('var K_%s: per_fmol {init: %g, pub: out};\n' % (Kname[ik], K[ik]))
cid.write('enddef;\n')
cid.write('def comp %s as\n' % (modname))
cid.write(' var time: second {pub: in};\n\
var R: J_per_K_per_mol {pub: in};\n\
var T: kelvin {pub: in};\n\
// parameters\n')
for ik in range(len(kappa)):
cid.write('var kappa_%s: fmol_per_sec {pub: in};\n' % (rxnID[ik]))
for ik in range(len(Kname)):
cid.write('var K_%s: per_fmol {pub: in};\n' % (Kname[ik]))
cid.write('// Input from global environment\n')
for Kn in Kname:
cid.write('var q_%s: fmol {pub: in};\n' % Kn)
# cid.write('// Output to global environment\n')
# for Kn in Kname:
# # cid.write('var q_%s: fmol {init: 1e-16, pub: out};\n'%(Kn))
# cid.write('var v_%s: fmol_per_sec {pub: out};\n'%(Kn))
cid.write('// Constitutive parameters\n')
for Kn in Kname:
cid.write('var mu_%s: J_per_mol;\n' % (Kn))
for rx in rxnID:
cid.write('var v_%s: fmol_per_sec {pub: out};\n' % (rx))
for Kn in Kname:
cid.write('mu_%s = R*T*ln(K_%s*q_%s);\n' % (Kn, Kn, Kn))
for rx in rxnID:
cid.write('v_%s = ppp;\n' % (rx))
# for Kn in Kname:
# cid.write('v_%s = rrr;\n' %Kn)
# for Kn in Kname:
# cid.write('ode(q_%s, time) = qqq;\n'%Kn)
cid.write('enddef;\n')
cid.write('def map between environment and %s for\n' % modname)
cid.write('vars time and time;\n')
for Kn in Kname:
cid.write('vars q_%s and q_%s;\n' % (Kn, Kn))
for rx in rxnID:
cid.write('vars v_%s and v_%s;\n' % (rx, rx))
cid.write('enddef;\n')
cid.write('def map between %s and %s_parameters for\n' % (modname, modname))
for ik in rxnID:
cid.write('vars kappa_%s and kappa_%s;\n' % (ik, ik))
for mod in Kname:
cid.write('vars K_%s and K_%s;\n' % (mod, mod))
cid.write('enddef;\n')
cid.write('def map between constants and %s for\n' % modname)
cid.write('vars R and R;\n vars T and T;\n')
cid.write('enddef;\n')
cid.write('enddef;\n')
cid.close()
print('error =', (error))
