SimVascular_report_PostProcess/functions.py

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#!/usr/bin/env python
"""
Created on Thu Jul 16 15:08:27 2020
@author: Aloma Blanch
"""
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import matplotlib
import numpy as np
import pandas as pd
import matplotlib.pyplot as plt
import matplotlib.transforms as mtransforms
from math import floor
from statistics import mean
from scipy.signal import find_peaks
def cycle(folder,dt,N_ts,save_path):
pressure = np.loadtxt(folder + '/PHistRCR.dat',skiprows=1)
T = round(dt*N_ts,3)
time = np.linspace(0,T,N_ts+1)
# Find peaks, keep only the maximums
peaks, _ = find_peaks(pressure[:,-1])
idx = np.where(pressure[peaks,-1] >= np.mean(pressure))
peaks_loc = peaks[idx]
P_peaks = pressure[peaks,-1][pressure[peaks,-1] >= np.mean(pressure)]
# Rmove the multiple picks found in the same location
idx_del = []
t_pk_loc = time[peaks_loc].tolist()
peak_tdiff = [t_pk_loc[n]-t_pk_loc[n-1] for n in range(1,len(t_pk_loc))]
for i in range(0,len(peak_tdiff)):
if peak_tdiff[i]<= dt*10:
idx_del.append(i)
t_pk_loc[i] = []
peak_tdiff[i] = []
t_pk_loc[:] = [x for x in t_pk_loc if x]
peak_tdiff[:] = [x for x in peak_tdiff if x]
P_peaks = np.delete(P_peaks,idx_del)
fig, ax = plt.subplots()
ax.plot(time,pressure[:,-1]/1333.22,'b')
ax.plot(t_pk_loc, P_peaks/1333.22, "or",label='peak location')
ax.set(xlabel='time [s]', ylabel='Pressure [mmHg]',
title='Pressure at last outlet')
ax.spines['right'].set_visible(False)
ax.spines['top'].set_visible(False)
ax.legend(loc=0)
# plt.show()
plt.savefig(save_path + '/Pressure_max_n_cycles.pdf')
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return (floor(mean(peak_tdiff[1:])*1000)/1000,len(t_pk_loc))
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def error_plot(folder,t_step,r_criteria,save_path):
# Load iterations and residual error
histor = folder + '/histor.dat'
input = open(histor, 'r')
output = open(folder + "/histor_better.dat", 'w')
output.writelines(line.strip() +'\n' for line in input)
input.close()
output.close()
error_info = pd.read_csv(folder + "/histor_better.dat", sep=' ', header=None, usecols=(0,1,2))
# Select only last iteration of residual error
error=[]
for n in range(1,error_info.shape[0]):
if (error_info[0][n]>error_info[0][n-1]):
error.append(error_info[2][n-1])
time = np.linspace(start = t_step, stop = len(error)*t_step, num = len(error))
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# Liniar Scale
fig, ax = plt.subplots()
ax.plot(time,error)
ax.plot(time,r_criteria*np.ones(len(error)),'r')
ax.set(xlabel='Time steps', ylabel='Residual error',
title='Last nonlinear residual error for each time step')
ax.spines['right'].set_visible(False)
ax.spines['top'].set_visible(False)
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# plt.show()
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plt.savefig(save_path + '/Last_nonlin_res_error.pdf')
# Semilog scale
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fig, ax = plt.subplots()
ax.semilogy(time,error)
ax.semilogy(time,r_criteria*np.ones(len(error)),'r')
ax.set(xlabel='Time steps', ylabel='Residual error',
title='Log - Last nonlinear residual error for each time step')
ax.spines['right'].set_visible(False)
ax.spines['top'].set_visible(False)
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# plt.show()
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plt.savefig(save_path + '/Log_Last_nonlin_res_error.pdf')
fig.savefig(save_path + '/Log_Last_nonlin_res_error.jpg',dpi=150)
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def periodicity(project,folder,dt,T_cyc,n_cyc,save_path):
pressure = np.loadtxt(folder+'/PHistRCR.dat',skiprows=1,)
time = np.linspace(0,T_cyc*n_cyc,round(T_cyc/dt*n_cyc)+1)
peak_P = []
peak_P_pos = []
Nc = round(T_cyc/dt)
for i in range(0,n_cyc):
peak_P.append(np.amax(pressure[i*Nc:Nc*(i+1),-1])/1333.22)
peak_P_pos.append(np.where(pressure[i*Nc:Nc*(i+1),-1] == np.amax(pressure[i*Nc:Nc*(i+1),-1]))[0][0]+Nc*i)
peak_Pdiff = [peak_P[n]-peak_P[n-1] for n in range(1,len(peak_P))]
peak_Pdiff = list(map(abs, peak_Pdiff))
fig, ax = plt.subplots()
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ax.plot(time,pressure[:,-1]/1333.22,'b')
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ax.plot(time[peak_P_pos], peak_P,'ro',label='Cycle pike')
ax.set(xlabel='time [s]', ylabel='Pressure [mmHg]',
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title='Pressure at last outlet')
ax.spines['right'].set_visible(False)
ax.spines['top'].set_visible(False)
ax.legend(loc=0)
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# plt.show()
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plt.savefig(save_path + '/periodicity.pdf')
fig.savefig(save_path + '/periodicity.jpg',dpi=150)
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if (peak_Pdiff[-1]<=1):
print('The numerical simulation \'{0}\' has achieve periodicity!\nSystolic Blood Pressure (SBP):\nsecond-last cycle = {1:.2f} mmHg,\nlast cycle = {2:.2f} mmHg,\n\u0394mmHg = {3:.2f} mmHg'.format(project,peak_P[-2],peak_P[-1],peak_Pdiff[-1]))
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txt = ['The numerical simulation \'{0}\' has achieved periodicity.'.format(project), 'Systolic Blood Pressure (SBP):', 'Second-last cycle = {0:.2f} mmHg'.format(peak_P[-2]), 'Last cycle = {0:.2f} mmHg'.format(peak_P[-1]), 'Delta_mmHg = {0:.2f} mmHg'.format(peak_Pdiff[-1])]
else:
print('The numerical simulation \'{0}\' has not achieve periodicity...\nSystolic Blood Pressure (SBP):\nsecond-last cycle = {1:.2f} mmHg,\nlast cycle = {2:.2f} mmHg,\n\u0394mmHg = {3:.2f} mmHg'.format(project,peak_P[-2],peak_P[-1],peak_Pdiff[-1]))
txt = ['The numerical simulation \'{0}\' has achieved periodicity.'.format(project), 'Systolic Blood Pressure (SBP):', 'Second-last cycle = {0:.2f} mmHg'.format(peak_P[-2]), 'Last cycle = {0:.2f} mmHg'.format(peak_P[-1]), 'Delta_mmHg = {0:.2f} mmHg'.format(peak_Pdiff[-1])]
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return txt
def pressure(folder,N_ts,T_cyc,dt,n_cyc,save_path):
pressure = np.loadtxt(folder+'/PHistRCR.dat',skiprows=1,)
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Nc = round(T_cyc/dt)
time = np.linspace(0,T_cyc,Nc)
fig, ax = plt.subplots()
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SBP = np.empty(pressure.shape[1])
DBP = np.empty(pressure.shape[1])
MBP = np.empty(pressure.shape[1])
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for i in range(0,pressure.shape[1]):
ax.plot(time,pressure[N_ts-Nc:N_ts,i]/1333.22,label='ROI-'+str(i+2))
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SBP[i] = (np.amax(pressure[N_ts-Nc:N_ts,i]/1333.22))
DBP[i] = (np.amin(pressure[N_ts-Nc:N_ts,i]/1333.22))
MBP[i] = (mean(pressure[N_ts-Nc:N_ts,i]/1333.22))
PP = SBP-DBP
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ax.set(xlabel='time [s]', ylabel='Pressure [mmHg]',
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title='Pressure at each outlet')
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ax.spines['right'].set_visible(False)
ax.spines['top'].set_visible(False)
ax.legend(loc=0)
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# plt.show()
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plt.savefig(save_path + '/pressure.pdf')
fig.savefig(save_path + '/pressure.jpg',dpi=150)
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return (DBP,MBP,SBP,PP)
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def flow(folder,N_ts,T_cyc,dt,n_cyc,save_path):
flow = np.loadtxt(folder+'/QHistRCR.dat',skiprows=1,)
Nc = round(T_cyc/dt)
time = np.linspace(0,T_cyc,Nc)
fig, ax = plt.subplots()
Q = np.empty(flow.shape[1])
for i in range(0,flow.shape[1]):
ax.plot(time,flow[N_ts-Nc+1:N_ts+1,i],label='ROI-'+str(i+2))
Q[i] = (mean(flow[N_ts-Nc+1:N_ts+1,i]))
ax.set(xlabel='time [s]', ylabel='Flow [mL/s]',
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title='Flow at each outlet')
ax.spines['right'].set_visible(False)
ax.spines['top'].set_visible(False)
ax.legend(loc=0)
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# plt.show()
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plt.savefig(save_path + '/flow.pdf')
fig.savefig(save_path + '/flow.jpg',dpi=150)
return Q
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def inlet_flow_waveform(project_folder,t_btw_rst,N_ts,dt,T_cyc,n_cyc,save_path):
x = np.loadtxt(project_folder+'/ROI-1.flow')
t = x[:,0]
if (x[4,1] < 0):
Q = -x[:,1]
else:
Q = x[:,1]
Nt_pts = np.linspace(t_btw_rst,N_ts,int(N_ts/t_btw_rst))
t_pts = Nt_pts*dt
# Put all the time values on a single cardiac cylce
for n in range(len(t_pts)):
tmp=divmod(t_pts[n],T_cyc)
t_pts[n]=tmp[1]
if round(tmp[1],3) == 0:
t_pts[n]=T_cyc
# Interpolate the flow rate to obtain the location of the point
Q_pts = np.interp(t_pts, t, Q)
fig, ax = plt.subplots()
ax.plot(t, Q, 'r')
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ax.plot(t_pts, Q_pts, 'ob',label='Time steps saved')
trans_offset = mtransforms.offset_copy(ax.transData, fig=fig,
x=-0, y=0.15, units='inches')
ax.set(xlabel='Time [s]', ylabel='Flow Rate - Q [mL/s]',
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title='Inlet Flow Rate Waveform')
ax.set_ylim([-10, 90])
ax.spines['right'].set_visible(False)
ax.spines['top'].set_visible(False)
# Adding label to the points
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time = []
for i in range(0,np.unique(np.round(t_pts,3)).shape[0]):
time.append('$t_'+str(i+1)+'$')
for x, y, t in zip(t_pts[(-n_cyc-1):], Q_pts[(-n_cyc-1):], time):
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plt.text(x, y, t, transform=trans_offset, fontsize=12)
ax.legend(loc=0)
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# plt.show()
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plt.savefig(save_path + '/inlet_waveform.pdf')
fig.savefig(save_path + '/inlet_waveform.jpg',dpi=150)
print('{0} time steps saved, available to visualize in ParaView.'.format(np.unique(np.round(t_pts,3)).shape[0]))
txt = '{0} time steps saved, available to visualize in ParaView.'.format(np.unique(np.round(t_pts,3)).shape[0])
return txt
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def rcr(project_folder):
rcr_lines = []
with open (project_folder + '/rcrt.dat', "rt") as myfile:
for myline in myfile:
rcr_lines.append(myline)
n_out = int((len(rcr_lines)-1)/6)
Rc_C_Rd = np.empty([n_out,3])
for i in range(0,n_out):
Rc_C_Rd[i][0] = float(rcr_lines[2+i*6][:-1])
Rc_C_Rd[i][1] = float(rcr_lines[3+i*6][:-1])
Rc_C_Rd[i][2] = float(rcr_lines[4+i*6][:-1])
return Rc_C_Rd
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def barPlot(project_folder,DBP,MBP,SBP,PP,Q_avg,save_path):
aimed_all = [1] #No li agrada fer append en una llista buida, no recordo perquè i segur que es pot fer millor
f = open(project_folder+'/aimed.txt', 'r') #obrir el fitxer
for line in f:
aimed_all.append(line.split()) #fas una llista amb cada valor de la línia carregan-te els espais buits
del aimed_all[0] #esborrar el primer valor que has posat perquè no estigues buida la llista
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def plot_bar(CFD,aimed,name,save_path,unit,decimals):
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labels = []
for i in range(0,len(CFD)):
labels.append('ROI-'+str(i+2))
x = np.arange(len(labels)) # the label locations
width = 0.38 # the width of the bars
fig, ax = plt.subplots()
rects1 = ax.bar(x - width/2, CFD, width, label='CFD',color='k')
rects2 = ax.bar(x + width/2, aimed, width, label='Aimed',color='white', edgecolor='black', hatch='/')
ax.set_ylabel(name + unit)
ax.set_title(name)
ax.set_xticks(x)
ax.set_xticklabels(labels)
ax.legend()
high = max(max(aimed,CFD))
ax.set_ylim(top = 1.7*high)
def autolabel(rects,decimals):
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"""Attach a text label above each bar in *rects*, displaying its height."""
for rect in rects:
height = rect.get_height()
ax.annotate(decimals.format(height),
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xy=(rect.get_x() + rect.get_width() / 2, height),
xytext=(0,3), # 3 points vertical offset
textcoords="offset points",
ha='center', va='bottom',
fontsize = 7.5)
autolabel(rects1,decimals)
autolabel(rects2,decimals)
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# Create labels
err = []
zip_object = zip(CFD, aimed)
for x1_i, x2_i in zip_object:
err.append(round((x1_i-x2_i)/x2_i*100,2))
# Text on the top of each barplot
for i in range(len(x)):
plt.text(x = x[i]- width/2, y = max(CFD[i],aimed[i])+0.15*max(max(CFD,aimed)), s = str(err[i])+'%', fontsize = 8, color='r')
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fig.tight_layout()
# plt.show()
plt.savefig(save_path + '/'+name+'_bar.pdf')
fig.savefig(save_path + '/'+name+'_bar.jpg',dpi=150)
# DBP
CFD = [float(i) for i in DBP]
aimed = [float(i) for i in aimed_all[0]]
plot_bar(CFD,aimed,'DBP',save_path,' [mmHg]','{0:.1f}')
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# MBP
CFD = [float(i) for i in MBP]
aimed = [float(i) for i in aimed_all[1]]
plot_bar(CFD,aimed,'MBP',save_path,' [mmHg]','{0:.1f}')
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# SBP
CFD = [float(i) for i in SBP]
aimed = [float(i) for i in aimed_all[2]]
plot_bar(CFD,aimed,'SBP',save_path,' [mmHg]','{0:.1f}')
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# PP
CFD = [float(i) for i in PP]
aimed = [float(i) for i in aimed_all[3]]
plot_bar(CFD,aimed,'PP',save_path,' [mmHg]','{0:.1f}')
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# Q_avg
CFD = [float(i) for i in Q_avg]
aimed = [float(i) for i in aimed_all[4]]
plot_bar(CFD,aimed,'Q_avg',save_path,' [mL/s]','{0:.2f}')