TCLab E - Hybrid Model Estimation

The TCLab is a hands-on application of machine learning and advanced temperature control with two heaters and two temperature sensors. The labs reinforce principles of model development, estimation, and advanced control methods. This is the fifth exercise and it involves estimating parameters in a multi-variate energy balance model with added empirical elements. The predictions are aligned to the measured values through an optimizer that adjusts the parameters to minimize a sum of squared error or sum of absolute values objective. This lab builds upon the TCLab C by using the estimation of parameters in an energy balance but also adding additional equations that give a 2nd order response. The 2nd order response comes from splitting the finite element model of the heaters and temperature sensors. This creates a total of 4 differential equations with parameters that are adjusted to minimize the difference between the predicted and measured temperatures.

Lab Problem Statement

Data and Solutions


import numpy as np
import pandas as pd
import tclab
import time
import matplotlib.pyplot as plt

# generate step test data on Arduino
filename = 'tclab_dyn_data2.csv'

# heater steps
Q1d = np.zeros(601)
Q1d[10:200] = 80
Q1d[200:280] = 20
Q1d[280:400] = 70
Q1d[400:] = 50

Q2d = np.zeros(601)
Q2d[120:320] = 100
Q2d[320:520] = 10
Q2d[520:] = 80

# Connect to Arduino
a = tclab.TCLab()
fid = open(filename,'w')
fid.write('Time,H1,H2,T1,T2\n')
fid.close()

# run step test (10 min)
for i in range(601):
    # set heater values
    a.Q1(Q1d[i])
    a.Q2(Q2d[i])
    print('Time: ' + str(i) + \
          ' H1: ' + str(Q1d[i]) + \
          ' H2: ' + str(Q2d[i]) + \
          ' T1: ' + str(a.T1)   + \
          ' T2: ' + str(a.T2))
    # wait 1 second
    time.sleep(1)
    fid = open(filename,'a')
    fid.write(str(i)+','+str(Q1d[i])+','+str(Q2d[i])+',' \
              +str(a.T1)+','+str(a.T2)+'\n')
# close connection to Arduino
a.close()

# read data file
data = pd.read_csv(filename)

# plot measurements
plt.figure()
plt.subplot(2,1,1)
plt.plot(data['Time'],data['H1'],'r-',label='Heater 1')
plt.plot(data['Time'],data['H2'],'b--',label='Heater 2')
plt.ylabel('Heater (%)')
plt.legend(loc='best')
plt.subplot(2,1,2)
plt.plot(data['Time'],data['T1'],'r.',label='Temperature 1')
plt.plot(data['Time'],data['T2'],'b.',label='Temperature 2')
plt.ylabel('Temperature (degC)')
plt.legend(loc='best')
plt.xlabel('Time (sec)')
plt.savefig('tclab_dyn_meas2.png')

plt.show()

import numpy as np
import matplotlib.pyplot as plt
import pandas as pd
from gekko import GEKKO

# Import or generate data
filename = 'tclab_dyn_data2.csv'
try:
    data = pd.read_csv(filename)
except:
    url = 'https://apmonitor.com/do/uploads/Main/tclab_dyn_data2.txt'
    data = pd.read_csv(url)

# Create GEKKO Model
m = GEKKO()
m.time = data['Time'].values

# Parameters to Estimate
U = m.FV(value=10,lb=1,ub=20)
tau = m.FV(value=20,lb=15,ub=25)
alpha1 = m.FV(value=0.01,lb=0.003,ub=0.03)  # W / % heater
alpha2 = m.FV(value=0.005,lb=0.002,ub=0.02) # W / % heater

# STATUS=1 allows solver to adjust parameter
U.STATUS = 1  
tau.STATUS = 1
alpha1.STATUS = 1
alpha2.STATUS = 1

# Measured inputs
Q1 = m.MV(value=data['H1'].values)
Q2 = m.MV(value=data['H2'].values)

# State variables
TH1 = m.SV(value=data['T1'].values)
TH2 = m.SV(value=data['T2'].values)

# Measurements for model alignment
TC1 = m.CV(value=data['T1'].values,lb=0,ub=200)
TC1.FSTATUS = 1    # minimize fstatus * (meas-pred)^2

TC2 = m.CV(value=data['T2'].values,lb=0,ub=200)
TC2.FSTATUS = 1    # minimize fstatus * (meas-pred)^2

Ta = m.Param(value=19.0+273.15)     # K
mass = m.Param(value=4.0/1000.0)    # kg
Cp = m.Param(value=0.5*1000.0)      # J/kg-K    
A = m.Param(value=10.0/100.0**2)    # Area not between heaters in m^2
As = m.Param(value=2.0/100.0**2)    # Area between heaters in m^2
eps = m.Param(value=0.9)            # Emissivity
sigma = m.Const(5.67e-8)            # Stefan-Boltzmann

# Heater temperatures in Kelvin
T1 = m.Intermediate(TH1+273.15)
T2 = m.Intermediate(TH2+273.15)

# Heat transfer between two heaters
Q_C12 = m.Intermediate(U*As*(T2-T1)) # Convective
Q_R12 = m.Intermediate(eps*sigma*As*(T2**4-T1**4)) # Radiative

# Semi-fundamental correlations (energy balances)
m.Equation(TH1.dt() == (1.0/(mass*Cp))*(U*A*(Ta-T1) \
                    + eps * sigma * A * (Ta**4 - T1**4) \
                    + Q_C12 + Q_R12 \
                    + alpha1*Q1))

m.Equation(TH2.dt() == (1.0/(mass*Cp))*(U*A*(Ta-T2) \
                    + eps * sigma * A * (Ta**4 - T2**4) \
                    - Q_C12 - Q_R12 \
                    + alpha2*Q2))

# Empirical correlations (lag equations to emulate conduction)
m.Equation(tau * TC1.dt() == -TC1 + TH1)
m.Equation(tau * TC2.dt() == -TC2 + TH2)

# Options
m.options.IMODE   = 5 # MHE
m.options.EV_TYPE = 2 # Objective type
m.options.NODES   = 2 # Collocation nodes
m.options.SOLVER  = 3 # IPOPT

# Solve
m.solve(disp=True)

# Parameter values
print('U     : ' + str(U.value[0]))
print('tau   : ' + str(tau.value[0]))
print('alpha1: ' + str(alpha1.value[0]))
print('alpha2: ' + str(alpha2.value[0]))

# Create plot
plt.figure()
ax=plt.subplot(2,1,1)
ax.grid()
plt.plot(data['Time'],data['T1'],'ro',label=r'$T_1$ measured')
plt.plot(m.time,TH1.value,'k-',label=r'$T_1$ heater')
plt.plot(m.time,TC1.value,color='purple',linestyle='--',\
         lw=3,label=r'$T_1$ sensor')
plt.plot(data['Time'],data['T2'],'bx',label=r'$T_2$ measured')
plt.plot(m.time,TH2.value,'k-',label=r'$T_2$ heater')
plt.plot(m.time,TC2.value,color='orange',linestyle='--',\
         lw=3,label=r'$T_2$ sensor')
plt.ylabel('Temperature (degC)')
plt.legend(loc=2)
ax=plt.subplot(2,1,2)
ax.grid()
plt.plot(data['Time'],data['H1'],'r-',\
         lw=3,label=r'$Q_1$')
plt.plot(data['Time'],data['H2'],'b:',\
         lw=3,label=r'$Q_2$')
plt.ylabel('Heaters')
plt.xlabel('Time (sec)')
plt.legend(loc='best')
plt.show()

Note: Switch to make_mp4 = True to make an MP4 movie animation. This requires imageio and ffmpeg (install available through Python). It creates a folder named figures in your run directory. You can delete this folder after the run is complete.

import numpy as np
import time
import matplotlib.pyplot as plt
import random
# get gekko package with:
#   pip install gekko
from gekko import GEKKO
# get tclab package with:
#   pip install tclab
from tclab import TCLab

# Connect to Arduino
a = TCLab()

# Make an MP4 animation?
make_mp4 = False
if make_mp4:
    import imageio  # required to make animation
    import os
    try:
        os.mkdir('./figures')
    except:
        pass

# Final time
tf = 10 # min
# number of data points (1 pt every 3 seconds)
n = tf * 20 + 1

# Configure heater levels
# Percent Heater (0-100%)
Q1s = np.zeros(n)
Q2s = np.zeros(n)
# Heater random steps every 50 sec
# Alternate steps by Q1 and Q2
Q1s[3:]    = 100.0
Q1s[50:]   = 0.0
Q1s[100:]  = 80.0

Q2s[25:]   = 60.0
Q2s[75:]   = 100.0
Q2s[125:]  = 25.0

# rapid, random changes every 5 cycles between 50 and 100
for i in range(130,180):
    if i%10==0:
        Q1s[i:i+10] = random.random() * 100.0
    if (i+5)%10==0:
        Q2s[i:i+10] = random.random() * 100.0

# Record initial temperatures (degC)
T1m = a.T1 * np.ones(n)
T2m = a.T2 * np.ones(n)
# Store MHE values for plots
Tmhe1 = T1m[0] * np.ones(n)
Tmhe2 = T2m[0] * np.ones(n)
Umhe = 10.0 * np.ones(n)
taumhe = 5.0 * np.ones(n)
amhe1 = 0.01 * np.ones(n)
amhe2 = 0.0075 * np.ones(n)

#########################################################
# Initialize Model as Estimator
#########################################################
m = GEKKO(name='tclab-mhe',remote=False)

# 60 second time horizon, 20 steps
m.time = np.linspace(0,60,21)

# Parameters to Estimate
U = m.FV(value=10,name='u')
U.STATUS = 0  # don't estimate initially
U.FSTATUS = 0 # no measurements
U.DMAX = 1
U.LOWER = 5
U.UPPER = 15

tau = m.FV(value=5,name='tau')
tau.STATUS = 0  # don't estimate initially
tau.FSTATUS = 0 # no measurements
tau.DMAX = 1
tau.LOWER = 4
tau.UPPER = 8

alpha1 = m.FV(value=0.01,name='a1')   # W / % heater
alpha1.STATUS = 0  # don't estimate initially
alpha1.FSTATUS = 0 # no measurements
alpha1.DMAX = 0.001
alpha1.LOWER = 0.003
alpha1.UPPER = 0.03

alpha2 = m.FV(value=0.0075,name='a2') # W / % heater
alpha2.STATUS = 0  # don't estimate initially
alpha2.FSTATUS = 0 # no measurements
alpha2.DMAX = 0.001
alpha2.LOWER = 0.002
alpha2.UPPER = 0.02

# Measured inputs
Q1 = m.MV(value=0,name='q1')
Q1.STATUS = 0  # don't estimate
Q1.FSTATUS = 1 # receive measurement

Q2 = m.MV(value=0,name='q2')
Q2.STATUS = 0  # don't estimate
Q2.FSTATUS = 1 # receive measurement

# State variables
TH1 = m.SV(value=T1m[0],name='th1')
TH2 = m.SV(value=T2m[0],name='th2')

# Measurements for model alignment
TC1 = m.CV(value=T1m[0],name='tc1')
TC1.STATUS = 1     # minimize error between simulation and measurement
TC1.FSTATUS = 1    # receive measurement
TC1.MEAS_GAP = 0.1 # measurement deadband gap
TC1.LOWER = 0
TC1.UPPER = 200

TC2 = m.CV(value=T2m[0],name='tc2')
TC2.STATUS = 1     # minimize error between simulation and measurement
TC2.FSTATUS = 1    # receive measurement
TC2.MEAS_GAP = 0.1 # measurement deadband gap
TC2.LOWER = 0
TC2.UPPER = 200

Ta = m.Param(value=23.0+273.15)     # K
mass = m.Param(value=4.0/1000.0)    # kg
Cp = m.Param(value=0.5*1000.0)      # J/kg-K    
A = m.Param(value=10.0/100.0**2)    # Area not between heaters in m^2
As = m.Param(value=2.0/100.0**2)    # Area between heaters in m^2
eps = m.Param(value=0.9)            # Emissivity
sigma = m.Const(5.67e-8)            # Stefan-Boltzmann

# Heater temperatures
T1 = m.Intermediate(TH1+273.15)
T2 = m.Intermediate(TH2+273.15)

# Heat transfer between two heaters
Q_C12 = m.Intermediate(U*As*(T2-T1)) # Convective
Q_R12 = m.Intermediate(eps*sigma*As*(T2**4-T1**4)) # Radiative

# Semi-fundamental correlations (energy balances)
m.Equation(TH1.dt() == (1.0/(mass*Cp))*(U*A*(Ta-T1) \
                    + eps * sigma * A * (Ta**4 - T1**4) \
                    + Q_C12 + Q_R12 \
                    + alpha1*Q1))

m.Equation(TH2.dt() == (1.0/(mass*Cp))*(U*A*(Ta-T2) \
                    + eps * sigma * A * (Ta**4 - T2**4) \
                    - Q_C12 - Q_R12 \
                    + alpha2*Q2))

# Empirical correlations (lag equations to emulate conduction)
m.Equation(tau * TC1.dt() == -TC1 + TH1)
m.Equation(tau * TC2.dt() == -TC2 + TH2)

# Global Options
m.options.IMODE   = 5 # MHE
m.options.EV_TYPE = 2 # Objective type
m.options.NODES   = 3 # Collocation nodes
m.options.SOLVER  = 3 # IPOPT
m.options.COLDSTART = 1 # COLDSTART on first cycle
##################################################################
# Create plot
plt.figure(figsize=(10,7))
plt.ion()
plt.show()

# Main Loop
start_time = time.time()
prev_time = start_time
tm = np.zeros(n)

try:
    for i in range(1,n):
        # Sleep time
        sleep_max = 3.0
        sleep = sleep_max - (time.time() - prev_time)
        if sleep>=0.01:
            time.sleep(sleep-0.01)
        else:
            time.sleep(0.01)

        # Record time and change in time
        t = time.time()
        dt = t - prev_time
        prev_time = t
        tm[i] = t - start_time

        # Read temperatures in Celsius
        T1m[i] = a.T1
        T2m[i] = a.T2

        # Insert measurements
        TC1.MEAS = T1m[i]
        TC2.MEAS = T2m[i]
        Q1.MEAS = Q1s[i-1]
        Q2.MEAS = Q2s[i-1]

        # Start estimating U after 10 cycles (20 sec)
        if i==10:
            U.STATUS = 1
            tau.STATUS = 1
            alpha1.STATUS = 1
            alpha2.STATUS = 1

        # Predict Parameters and Temperatures with MHE
        m.solve(disp=True)

        if m.options.APPSTATUS == 1:
            # Retrieve new values
            Tmhe1[i] = TC1.MODEL
            Tmhe2[i] = TC2.MODEL
            Umhe[i]  = U.NEWVAL
            taumhe[i] = tau.NEWVAL
            amhe1[i] = alpha1.NEWVAL
            amhe2[i] = alpha2.NEWVAL
        else:
            # Solution failed, copy prior solution
            Tmhe1[i] = Tmhe1[i-1]
            Tmhe2[i] = Tmhe1[i-1]
            Umhe[i]  = Umhe[i-1]
            taumhe[i] = taumhe[i-1]
            amhe1[i] = amhe1[i-1]
            amhe2[i] = amhe2[i-1]

        # Write new heater values (0-100)
        a.Q1(Q1s[i])
        a.Q2(Q2s[i])

        # Plot
        plt.clf()
        ax=plt.subplot(3,1,1)
        ax.grid()
        plt.plot(tm[0:i],T1m[0:i],'ro',label=r'$T_1$ measured')
        plt.plot(tm[0:i],Tmhe1[0:i],'k-',label=r'$T_1$ MHE')
        plt.plot(tm[0:i],T2m[0:i],'bx',label=r'$T_2$ measured')
        plt.plot(tm[0:i],Tmhe2[0:i],'k--',label=r'$T_2$ MHE')
        plt.ylabel('Temperature (degC)')
        plt.legend(loc=2)
        ax=plt.subplot(3,1,2)
        ax.grid()
        plt.plot(tm[0:i],Umhe[0:i],'k-',label='Heat Transfer Coeff')
        plt.plot(tm[0:i],taumhe[0:i],'g:',label='Time Constant')        
        plt.plot(tm[0:i],amhe1[0:i]*1000,'r--',label=r'$\alpha_1$x1000')
        plt.plot(tm[0:i],amhe2[0:i]*1000,'b--',label=r'$\alpha_2$x1000')
        plt.ylabel('Parameters')
        plt.legend(loc='best')
        ax=plt.subplot(3,1,3)
        ax.grid()
        plt.plot(tm[0:i],Q1s[0:i],'r-',label=r'$Q_1$')
        plt.plot(tm[0:i],Q2s[0:i],'b:',label=r'$Q_2$')
        plt.ylabel('Heaters')
        plt.xlabel('Time (sec)')
        plt.legend(loc='best')
        plt.draw()
        plt.pause(0.05)
        if make_mp4:
            filename='./figures/plot_'+str(i+10000)+'.png'
            plt.savefig(filename)

    # Turn off heaters
    a.Q1(0)
    a.Q2(0)
    # Save figure
    plt.savefig('tclab_mhe.png')

    # generate mp4 from png figures in batches of 350
    if make_mp4:
        images = []
        iset = 0
        for i in range(1,n):
            filename='./figures/plot_'+str(i+10000)+'.png'
            images.append(imageio.imread(filename))
            if ((i+1)%350)==0:
                imageio.mimsave('results_'+str(iset)+'.mp4', images)
                iset += 1
                images = []
        if images!=[]:
            imageio.mimsave('results_'+str(iset)+'.mp4', images)

# Allow user to end loop with Ctrl-C          
except KeyboardInterrupt:
    # Disconnect from Arduino
    a.Q1(0)
    a.Q2(0)
    print('Shutting down')
    a.close()
    plt.savefig('tclab_mhe.png')

# Make sure serial connection still closes when there's an error
except:          
    # Disconnect from Arduino
    a.Q1(0)
    a.Q2(0)
    print('Error: Shutting down')
    a.close()
    plt.savefig('tclab_mhe.png')
    raise

See also:

Advanced Control Lab Overview

Virtual TCLab on Google Colab

GEKKO Documentation

TCLab Documentation

TCLab Files on GitHub

Basic (PID) Control Lab

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