2020-07-17 01:41:59 +01:00
|
|
|
#!/usr/bin/env python
|
2020-07-17 11:51:22 +01:00
|
|
|
"""
|
|
|
|
Created on Thu Jul 16 15:08:27 2020
|
|
|
|
|
|
|
|
@author: Aloma Blanch
|
|
|
|
"""
|
|
|
|
|
2020-07-23 17:06:35 +01:00
|
|
|
import matplotlib
|
2020-07-17 01:41:59 +01:00
|
|
|
import numpy as np
|
|
|
|
import pandas as pd
|
2020-07-17 23:10:24 +01:00
|
|
|
import matplotlib.pyplot as plt
|
2020-07-17 03:18:08 +01:00
|
|
|
import matplotlib.transforms as mtransforms
|
2020-07-17 01:41:59 +01:00
|
|
|
|
2020-07-17 23:10:24 +01:00
|
|
|
from math import floor
|
|
|
|
from statistics import mean
|
|
|
|
from scipy.signal import find_peaks
|
|
|
|
|
2020-10-20 14:59:43 +01:00
|
|
|
def cycle(folder,dt,N_ts,save_path):
|
|
|
|
pressure = np.loadtxt(folder + '/PHistRCR.dat',skiprows=1)
|
2020-07-17 23:10:24 +01:00
|
|
|
T = round(dt*N_ts,3)
|
2020-10-20 14:59:43 +01:00
|
|
|
time = np.linspace(0,T,N_ts+1)
|
2020-07-17 23:10:24 +01:00
|
|
|
# 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]',
|
2020-07-24 14:22:33 +01:00
|
|
|
title='Pressure at last outlet')
|
2020-07-17 23:10:24 +01:00
|
|
|
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')
|
2020-07-23 17:06:35 +01:00
|
|
|
return (floor(mean(peak_tdiff[1:])*1000)/1000,len(t_pk_loc))
|
2020-07-17 01:41:59 +01:00
|
|
|
|
2020-07-17 05:33:48 +01:00
|
|
|
def error_plot(folder,t_step,r_criteria,save_path):
|
2020-07-17 01:41:59 +01:00
|
|
|
# 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))
|
|
|
|
|
2020-07-17 05:33:48 +01:00
|
|
|
# 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)
|
2020-07-17 12:48:51 +01:00
|
|
|
# plt.show()
|
2020-07-17 05:33:48 +01:00
|
|
|
plt.savefig(save_path + '/Last_nonlin_res_error.pdf')
|
2020-07-17 01:41:59 +01:00
|
|
|
# Semilog scale
|
2020-07-17 05:33:48 +01:00
|
|
|
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)
|
2020-07-17 12:48:51 +01:00
|
|
|
# plt.show()
|
2020-07-17 05:33:48 +01:00
|
|
|
plt.savefig(save_path + '/Log_Last_nonlin_res_error.pdf')
|
|
|
|
fig.savefig(save_path + '/Log_Last_nonlin_res_error.jpg',dpi=150)
|
2020-07-17 01:41:59 +01:00
|
|
|
|
2020-07-17 05:33:48 +01:00
|
|
|
|
|
|
|
def periodicity(project,folder,dt,T_cyc,n_cyc,save_path):
|
2020-10-20 14:59:43 +01:00
|
|
|
pressure = np.loadtxt(folder+'/PHistRCR.dat',skiprows=1,)
|
|
|
|
time = np.linspace(0,T_cyc*n_cyc,round(T_cyc/dt*n_cyc)+1)
|
2020-07-17 01:41:59 +01:00
|
|
|
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()
|
2020-07-17 05:33:48 +01:00
|
|
|
ax.plot(time,pressure[:,-1]/1333.22,'b')
|
2020-07-23 17:06:35 +01:00
|
|
|
ax.plot(time[peak_P_pos], peak_P,'ro',label='Cycle pike')
|
2020-07-17 01:41:59 +01:00
|
|
|
ax.set(xlabel='time [s]', ylabel='Pressure [mmHg]',
|
2020-07-17 05:33:48 +01:00
|
|
|
title='Pressure at last outlet')
|
2020-07-17 01:41:59 +01:00
|
|
|
ax.spines['right'].set_visible(False)
|
|
|
|
ax.spines['top'].set_visible(False)
|
|
|
|
ax.legend(loc=0)
|
2020-07-17 12:48:51 +01:00
|
|
|
# plt.show()
|
2020-07-17 05:33:48 +01:00
|
|
|
plt.savefig(save_path + '/periodicity.pdf')
|
|
|
|
fig.savefig(save_path + '/periodicity.jpg',dpi=150)
|
2020-07-17 01:41:59 +01:00
|
|
|
|
2020-07-17 05:33:48 +01:00
|
|
|
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]))
|
2020-07-17 14:44:29 +01:00
|
|
|
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])]
|
2020-10-20 14:59:43 +01:00
|
|
|
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])]
|
2020-07-17 05:33:48 +01:00
|
|
|
return txt
|
|
|
|
|
|
|
|
def pressure(folder,N_ts,T_cyc,dt,n_cyc,save_path):
|
2020-10-20 14:59:43 +01:00
|
|
|
pressure = np.loadtxt(folder+'/PHistRCR.dat',skiprows=1,)
|
2020-07-17 02:02:02 +01:00
|
|
|
Nc = round(T_cyc/dt)
|
|
|
|
time = np.linspace(0,T_cyc,Nc)
|
|
|
|
fig, ax = plt.subplots()
|
2020-07-17 02:30:27 +01:00
|
|
|
SBP = np.empty(pressure.shape[1])
|
|
|
|
DBP = np.empty(pressure.shape[1])
|
|
|
|
MBP = np.empty(pressure.shape[1])
|
2020-07-17 02:02:02 +01:00
|
|
|
for i in range(0,pressure.shape[1]):
|
2020-07-17 02:43:04 +01:00
|
|
|
ax.plot(time,pressure[N_ts-Nc:N_ts,i]/1333.22,label='ROI-'+str(i+2))
|
2020-07-17 02:30:27 +01:00
|
|
|
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
|
2020-07-17 02:02:02 +01:00
|
|
|
ax.set(xlabel='time [s]', ylabel='Pressure [mmHg]',
|
2020-07-17 05:33:48 +01:00
|
|
|
title='Pressure at each outlet')
|
2020-07-17 02:02:02 +01:00
|
|
|
ax.spines['right'].set_visible(False)
|
|
|
|
ax.spines['top'].set_visible(False)
|
|
|
|
ax.legend(loc=0)
|
2020-07-17 12:48:51 +01:00
|
|
|
# plt.show()
|
2020-07-17 05:33:48 +01:00
|
|
|
plt.savefig(save_path + '/pressure.pdf')
|
|
|
|
fig.savefig(save_path + '/pressure.jpg',dpi=150)
|
2020-07-17 02:30:27 +01:00
|
|
|
return (DBP,MBP,SBP,PP)
|
2020-07-17 02:43:04 +01:00
|
|
|
|
|
|
|
|
2020-07-17 05:33:48 +01:00
|
|
|
def flow(folder,N_ts,T_cyc,dt,n_cyc,save_path):
|
2020-10-20 14:59:43 +01:00
|
|
|
flow = np.loadtxt(folder+'/QHistRCR.dat',skiprows=1,)
|
2020-07-17 02:43:04 +01:00
|
|
|
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]):
|
2020-10-20 14:59:43 +01:00
|
|
|
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]))
|
2020-07-17 02:43:04 +01:00
|
|
|
|
|
|
|
ax.set(xlabel='time [s]', ylabel='Flow [mL/s]',
|
2020-07-17 05:33:48 +01:00
|
|
|
title='Flow at each outlet')
|
2020-07-17 02:43:04 +01:00
|
|
|
ax.spines['right'].set_visible(False)
|
|
|
|
ax.spines['top'].set_visible(False)
|
|
|
|
ax.legend(loc=0)
|
2020-07-17 12:48:51 +01:00
|
|
|
# plt.show()
|
2020-07-17 05:33:48 +01:00
|
|
|
plt.savefig(save_path + '/flow.pdf')
|
|
|
|
fig.savefig(save_path + '/flow.jpg',dpi=150)
|
2020-07-17 02:43:04 +01:00
|
|
|
return Q
|
2020-07-17 02:30:27 +01:00
|
|
|
|
2020-07-17 05:33:48 +01:00
|
|
|
def inlet_flow_waveform(project_folder,t_btw_rst,N_ts,dt,T_cyc,n_cyc,save_path):
|
2020-07-17 03:18:08 +01:00
|
|
|
x = np.loadtxt(project_folder+'/ROI-1.flow')
|
|
|
|
t = x[:,0]
|
2020-10-20 14:59:43 +01:00
|
|
|
if (x[4,1] < 0):
|
|
|
|
Q = -x[:,1]
|
|
|
|
else:
|
|
|
|
Q = x[:,1]
|
2020-07-17 03:18:08 +01:00
|
|
|
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')
|
2020-07-17 05:33:48 +01:00
|
|
|
ax.plot(t_pts, Q_pts, 'ob',label='Time steps saved')
|
2020-07-17 03:18:08 +01:00
|
|
|
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]',
|
2020-07-17 05:33:48 +01:00
|
|
|
title='Inlet Flow Rate Waveform')
|
2020-07-17 03:18:08 +01:00
|
|
|
ax.set_ylim([-10, 90])
|
|
|
|
ax.spines['right'].set_visible(False)
|
|
|
|
ax.spines['top'].set_visible(False)
|
|
|
|
# Adding label to the points
|
2020-07-17 03:34:00 +01:00
|
|
|
|
|
|
|
time = []
|
|
|
|
for i in range(0,np.unique(np.round(t_pts,3)).shape[0]):
|
|
|
|
time.append('$t_'+str(i+1)+'$')
|
2020-07-17 03:18:08 +01:00
|
|
|
for x, y, t in zip(t_pts[(-n_cyc-1):], Q_pts[(-n_cyc-1):], time):
|
2020-07-17 05:33:48 +01:00
|
|
|
plt.text(x, y, t, transform=trans_offset, fontsize=12)
|
|
|
|
ax.legend(loc=0)
|
2020-07-17 12:48:51 +01:00
|
|
|
# plt.show()
|
2020-07-17 05:33:48 +01:00
|
|
|
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
|
|
|
|
|
2020-07-17 14:44:29 +01:00
|
|
|
|
|
|
|
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
|
2020-07-17 02:02:02 +01:00
|
|
|
|
2020-07-23 17:06:35 +01:00
|
|
|
def barPlot(project_folder,DBP,MBP,SBP,PP,Q_avg,save_path):
|
2020-07-24 14:22:33 +01:00
|
|
|
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:
|
2020-10-20 14:59:43 +01:00
|
|
|
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
|
2020-07-23 17:06:35 +01:00
|
|
|
|
2020-10-20 14:59:43 +01:00
|
|
|
def plot_bar(CFD,aimed,name,save_path,unit,decimals):
|
2020-07-23 17:06:35 +01:00
|
|
|
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)
|
2020-10-20 14:59:43 +01:00
|
|
|
def autolabel(rects,decimals):
|
2020-07-23 17:06:35 +01:00
|
|
|
"""Attach a text label above each bar in *rects*, displaying its height."""
|
|
|
|
for rect in rects:
|
|
|
|
height = rect.get_height()
|
2020-10-20 14:59:43 +01:00
|
|
|
ax.annotate(decimals.format(height),
|
2020-07-23 17:06:35 +01:00
|
|
|
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)
|
|
|
|
|
2020-10-20 14:59:43 +01:00
|
|
|
autolabel(rects1,decimals)
|
|
|
|
autolabel(rects2,decimals)
|
2020-07-23 18:37:44 +01:00
|
|
|
# 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')
|
|
|
|
|
2020-07-23 17:06:35 +01:00
|
|
|
fig.tight_layout()
|
|
|
|
# plt.show()
|
|
|
|
plt.savefig(save_path + '/'+name+'_bar.pdf')
|
|
|
|
fig.savefig(save_path + '/'+name+'_bar.jpg',dpi=150)
|
|
|
|
|
|
|
|
# DBP
|
2020-10-20 14:59:43 +01:00
|
|
|
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}')
|
2020-07-23 17:06:35 +01:00
|
|
|
|
|
|
|
# MBP
|
2020-10-20 14:59:43 +01:00
|
|
|
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}')
|
2020-07-23 17:06:35 +01:00
|
|
|
|
|
|
|
# SBP
|
2020-10-20 14:59:43 +01:00
|
|
|
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}')
|
2020-07-23 17:06:35 +01:00
|
|
|
|
|
|
|
# PP
|
2020-10-20 14:59:43 +01:00
|
|
|
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}')
|
2020-07-23 17:06:35 +01:00
|
|
|
|
2020-10-20 14:59:43 +01:00
|
|
|
# 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}')
|