Generated Code
The following is python code generated by the CellML API from this CellML file. (Back to language selection)
The raw code is available.
# Size of variable arrays:
sizeAlgebraic = 8
sizeStates = 1
sizeConstants = 12
from math import *
from numpy import *
def createLegends():
legend_states = [""] * sizeStates
legend_rates = [""] * sizeStates
legend_algebraic = [""] * sizeAlgebraic
legend_voi = ""
legend_constants = [""] * sizeConstants
legend_voi = "time in component environment (second)"
legend_algebraic[0] = "F_isom in component contraction (newton)"
legend_constants[11] = "c in component contraction (newton)"
legend_states[0] = "L_ce in component contraction (metre)"
legend_constants[0] = "L_ce_opt in component contraction (metre)"
legend_algebraic[1] = "L in component contraction (metre)"
legend_constants[1] = "width in component contraction (metre)"
legend_constants[2] = "Factor in component contraction (per_second)"
legend_constants[3] = "A_REL in component contraction (newton)"
legend_constants[4] = "B_REL in component contraction (dimensionless)"
legend_algebraic[7] = "v_ce in component contraction (metre_per_second)"
legend_algebraic[5] = "F in component contraction (newton)"
legend_constants[5] = "F_max in component contraction (newton)"
legend_constants[6] = "q in component contraction (dimensionless)"
legend_algebraic[4] = "c1 in component contraction (per_second)"
legend_algebraic[2] = "c2 in component contraction (newton)"
legend_algebraic[6] = "c3 in component contraction (per_newton_second)"
legend_constants[7] = "slope in component contraction (newton)"
legend_constants[8] = "F_asympt in component contraction (dimensionless)"
legend_algebraic[3] = "L_see in component contraction (metre)"
legend_constants[9] = "L_slack in component contraction (metre)"
legend_constants[10] = "alpha in component contraction (newton_per_metre)"
legend_rates[0] = "d/dt L_ce in component contraction (metre)"
return (legend_states, legend_algebraic, legend_voi, legend_constants)
def initConsts():
constants = [0.0] * sizeConstants; states = [0.0] * sizeStates;
states[0] = 0.05
constants[0] = 0.055
constants[1] = 0.888
constants[2] = 1
constants[3] = 0.41
constants[4] = 5.2
constants[5] = 3277.4
constants[6] = 1
constants[7] = 2
constants[8] = 1.5
constants[9] = 0.42
constants[10] = 1449.027
constants[11] = -1.00000/(power(constants[1], 2.00000))
return (states, constants)
def computeRates(voi, states, constants):
rates = [0.0] * sizeStates; algebraic = [0.0] * sizeAlgebraic
algebraic[0] = (constants[11]*(power(states[0]/constants[0], 2.00000))-(2.00000*constants[11]*states[0])/constants[0])+constants[11]+1.00000
algebraic[1] = custom_piecewise([less_equal(voi , 1.00000), 1.00000 , greater(voi , 1.00000) & less(voi , 5.00000), 0.920000 , True, 0.900000])
algebraic[3] = algebraic[1]-states[0]
algebraic[5] = constants[10]*(algebraic[3]-constants[9])
algebraic[7] = -constants[2]*states[0]*(((algebraic[0]+constants[3])*constants[4])/(1.00000*(algebraic[5]/(constants[5]*constants[6]))+constants[3])-constants[4])
rates[0] = algebraic[7]
return(rates)
def computeAlgebraic(constants, states, voi):
algebraic = array([[0.0] * len(voi)] * sizeAlgebraic)
states = array(states)
voi = array(voi)
algebraic[0] = (constants[11]*(power(states[0]/constants[0], 2.00000))-(2.00000*constants[11]*states[0])/constants[0])+constants[11]+1.00000
algebraic[1] = custom_piecewise([less_equal(voi , 1.00000), 1.00000 , greater(voi , 1.00000) & less(voi , 5.00000), 0.920000 , True, 0.900000])
algebraic[3] = algebraic[1]-states[0]
algebraic[5] = constants[10]*(algebraic[3]-constants[9])
algebraic[7] = -constants[2]*states[0]*(((algebraic[0]+constants[3])*constants[4])/(1.00000*(algebraic[5]/(constants[5]*constants[6]))+constants[3])-constants[4])
algebraic[2] = algebraic[0]*constants[8]
algebraic[4] = (constants[2]*constants[4]*(power(algebraic[0]+algebraic[2], 2.00000)))/((algebraic[0]+constants[3])*constants[7])
algebraic[6] = algebraic[4]/(algebraic[0]+algebraic[2])
return algebraic
def custom_piecewise(cases):
"""Compute result of a piecewise function"""
return select(cases[0::2],cases[1::2])
def solve_model():
"""Solve model with ODE solver"""
from scipy.integrate import ode
# Initialise constants and state variables
(init_states, constants) = initConsts()
# Set timespan to solve over
voi = linspace(0, 10, 500)
# Construct ODE object to solve
r = ode(computeRates)
r.set_integrator('vode', method='bdf', atol=1e-06, rtol=1e-06, max_step=1)
r.set_initial_value(init_states, voi[0])
r.set_f_params(constants)
# Solve model
states = array([[0.0] * len(voi)] * sizeStates)
states[:,0] = init_states
for (i,t) in enumerate(voi[1:]):
if r.successful():
r.integrate(t)
states[:,i+1] = r.y
else:
break
# Compute algebraic variables
algebraic = computeAlgebraic(constants, states, voi)
return (voi, states, algebraic)
def plot_model(voi, states, algebraic):
"""Plot variables against variable of integration"""
import pylab
(legend_states, legend_algebraic, legend_voi, legend_constants) = createLegends()
pylab.figure(1)
pylab.plot(voi,vstack((states,algebraic)).T)
pylab.xlabel(legend_voi)
pylab.legend(legend_states + legend_algebraic, loc='best')
pylab.show()
if __name__ == "__main__":
(voi, states, algebraic) = solve_model()
plot_model(voi, states, algebraic)
