CHEMICAL ENGINEERING TRANSACTIONS  
 

VOL. 76, 2019 

A publication of 

 

The Italian Association 
of Chemical Engineering 
Online at www.aidic.it/cet 

Guest Editors: Petar S. Varbanov, Timothy G. Walmsley, Jiří J. Klemeš, Panos Seferlis 
Copyright © 2019, AIDIC Servizi S.r.l. 

ISBN 978-88-95608-73-0; ISSN 2283-9216 

Bypass Control System Design for HENs Based on 

Frequency Domain Analysis 

Lin Sun*, Zheng-hua Yang, Xiong-lin Luo 

Department of Automation, China University of Petroleum, Beijing, 102249, China 

sunlin@cup.edu.cn  

In this paper, a new approach to address bypass control system design for heat exchanger networks (HENs) is 

proposed based on frequency domain analysis. The classical bypass control system design methodology relies 

on the calculation of the relative gain array (RGA) which is commonly used as a measure of the interaction. The 

main drawbacks of this approach are the difficulties of analyzing the unstable process, and the complexity of 

measuring stability. Instead, the key idea of this work is to take stability margins into consideration when potential 

bypasses and controlled variables are paired. Firstly, on the basis of dynamic model, small singular values of 

the return difference matrix are presented for the simultaneous analysis of stability margin and flexibility. 

Secondly, the non-square relative gain array (ns-RGA) in the frequency domain is applied to study the 

interactions of potential bypasses and controlled variables, and some pairing rules are proposed. Thirdly 

parameters of PID controller are designed while phase margin and gain margin are in proper region, then the 

final pairing scheme is determined. Case studies illustrated the necessity to consider stability margins during 

the process of the bypass control system. 

1. Introduction 

The application of bypasses has been demonstrated for effective control of a target temperature. However, on 

one hand, as strong interaction exists in streams, HENs designed according to the chemical process often do 

not have enough bypasses. On the other hand, bypasses will also affect stability and optimality of HENs. 

Therefore, the BCS design is a challenging problem.  

Stability margins often refer to gain margin and phase margin and are studied in many works. Structural singular 

value μ is proposed to calculate stability margins (Doyle, 1982). Safonov (1982) developed a readily computable 

lower bound for diagonally perturbed systems. Wang et al. (2014) pointed out that the distance between 

operating point and Hopf singular point is used as a measure of stability. Lehtomaki et al. (1981) proposed the 

concept of minimum singular value of return difference matrix which pays attention on gain margin and phase 

margin simultaneously. This paper intends to study the application of minimum singular value of return difference 

matrix in HENs. 

Flexibility is a fundamental requirement of HENs and previous works on flexible analysis and designs are under 

the assumption that all control variables can be adjusted and HENs is stable. However, flexible HENs may come 

to be unstable with the existence of disturbance. Jiang et al. (2014) took stability into consideration when 

analyzing flexibility and they have a conclusion that flexible region contains unstable parts. However, they did 

not study the relationship between stability margins and flexibility. 

Bypasses are widely used for optimizing the operation of HENs to maintain the control requirements. A key 

issue of BCS is particularly relevant to select the appropriate potential bypasses and controlled variables. 

Relative gain array (RGA) was introduced by Bristol (1966) and is commonly used as a measure of interaction. 

Flexibility and controllability are taken into consideration at the process of BCS simultaneously. A computational 

framework is proposed for the synthesis of HENs where flexibility and controllability are studied simultaneously 

(Escobar et al., 2013). A sequential procedure for flexible HEN synthesis and control structure design has been 

proposed by Braccia et al. (2018). RGA in the frequency domain is proposed (Xu et al., 2016) and can used to 

analyze the unstable process. Therefore, this work plans to introduce RGA in the frequency domain to HENs. 

 
 
 
 
 
 
 
 
 
 
                                                                                                                                                                 DOI: 10.3303/CET1976128 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
Paper Received: 28/02/2019; Revised: 03/06/2019; Accepted: 04/06/2019 
Please cite this article as: Sun L., Yang Z.-H., Luo X.-L., 2019, Bypass Control System Design for HENs Based on Frequency Domain Analysis, 
Chemical Engineering Transactions, 76, 763-768  DOI:10.3303/CET1976128 
  

763



PID controller is widely placed to ensure control performance. Nonetheless, the design of PID controller has not 

been an integral part of BCS design. There are several design schemes for optimally tuning PID parameters. 

PID parameters adjustment method is proposed in HENs under fouling conditions (Trafczynski et al., 2016). 

Carvalho et al. (2018) introduced tune strategies for overcoming fouling effects in PID controlled heat 

exchangers. Basically, they are based on the time-domain.  

This paper investigates the incorporation of stability margins and BCS design. A method is presented to design 

optimal bypasses while achieving proper stability margins based on frequency domain analysis. Firstly, stability 

margins of HENs are analysed. Secondly, RGA in the frequency domain is applied to obtain the interaction of 

potential bypasses and controlled variables, and some pairing rules are given. Thirdly PID parameters are 

projected to design so that a single control system achieves proper stability margins. 

2. Stability margin analysis of HENs  

Stability is a prerequisite for a control system and stability criterion of open-loop system can be obtained 

according to Argument Principle, 

0=+= ZRP  (1) 

Where P is the number of open-loop system poles in the right half-plane, Z is the number of open-loop system 

zeros in the right half-plane, and R is the number of turns of Nyquist curve surrounding the origin. When P is 

equal to 0, the open-loop system is stable.  

This paper will study stability margins of HENs based on the inverse return difference matrix (Li et al., 2014). 

2
arcsin2

)1lg(20

m
PM

mGM

=

+=
 

(2) 

Where m is minimum singular value of the inverse return difference matrix of HENs, PM is phase margin and 

GM is gain margin. 

Stability and flexibility have been analyzed by Jiang et al. (2014) simultaneously. However, they did not take a 

deep insight into different stable points with different flexibility as shown in Figure 1. 

 

θ1
N +FΔθ1

+

θ1

θ2

θc

θ2
N +F1Δθ2

+

θ1
N +FΔθ2

+

θ2
N +FΔθ2

-

θ2
N +F1Δθ2

-

θ1
N +FΔθ1

-θ1
N +F1Δθ1

-
θ1

N +F1Δθ1
+

θ1
c

θ2
N 

θ1
N 

GM1

GM

 

Figure 1: Flexible region with different stability margins 

In Figure 1, flexibility index, gain margin and phase margin of HENs are F, GM and PM respectively when the 

design variable is d. Flexibility index, gain margin and phase margin of HENs are F1, GM1 and PM1 respectively 

when design variable is d1 .  

A simple HENs provided by Sun et al. (2011) will be used to illustrate the relationship between stability margins 

and flexibility index. The nominal data is listed in Table 1 and the structure is showed in Figure 2. 

764



H1 1 2 c1

h1 C1

h2 C2

190℃
100℃

80℃

80℃
140℃

20℃

70℃ 30℃

160℃

130℃

 

Figure 2: The structure of HENs 

Table 1: The parameters of the hot and cold fluid 

Stream 

number 
Input temperature/℃ Output temperature/℃ Heat capacity/(MW/℃) 

Hot(H1) 190 30 0.10 

Cold1(C1) 80 160 0.15 

Cold2(C2) 20 130 0.05 

 

When the area of heat exchanger 1 and heat exchanger 2 is 1258.71 m2 and 428.57m2, the Nyquist curve is 

shown in Figure 3a. 

0 0.1 0.2-0.1

2

4

6

8

Real axis

Imaginary axis

0

-2

-4

-6

-8

×10-4

×10-5

 

 

19.4 19.6 19.8 20.0 20.2 20.4 20.6

0.6

0.7

0.8

0.9

1.0

1.1

1.2

F
I

GM/db  

Figure 3a: Nyquist curve of HENs Figure 3b: Relationship between flexibility index and gain margin 

As shown in Figure 3a, the number of turns of Nyquist curve enveloping (0,0j) is 0, and the number of open-

loop system zeros in the right half-plane is 0, so the HENs is stable. 

In order to have better dynamic characteristics, gain margin of control systems is generally taken as Am=[3, 6], 

and phase margin is taken as φm= [30°, 60°]. It can be known from Figure 3b that when the FI is more than 1, 

gain margin is more than 6db. So the HENs is over stable and PID controller should be placed to improve 

stability margins at the process of BCS design.  

3. HEN control system design 

3.1 HEN frequency domain RGA 

Non-square RGA (ns-RGA) is used to measure the interactions of different variables for the number of controlled 

and manipulated variables is usually unequal in HENs. Compared with conventional ns-RGA in the time domain, 

in this paper s is replaced by jω, then G(s) in the time domain becomes G(jω) in the frequency domain. Assumed 

that there are q controlled variables and n potential bypasses in HENs. Ns-RGA in the frequency domain can 

be calculated by Eq(3) for q times. 

T
jGjGΛ )]([)()( 


=  (3) 

The symbol  means an element-by-element multiplication (Schur product). Gϕ(jω) is the pseudo-inverse matrix 
of G(jω).  

765



Each element in Eq(3) is plural number and cannot quantitatively analyse the impact of each potential bypass 

on the controlled variable. Then interaction measurement index (IMI) and the unit circle diagram in complex 

plane are proposed (Xu et al., 2016). 

Steps of calculating IMI in HENs is as following, 

Step 1: Choosing proper controlled variables and potential bypasses of HENs, then calculate the Λ(ω). 

Step 2: Assumed that the element Λip(ω) in Λ(ω) is described as a(ω)+ b(ω)j, and then the distance between 
Λip(ω) and (1,0j) is formulated as λip(ω). Then IMI is calculated in Eq(4), 


−

=
n

dD
n






 0
)(

1
ip

0

ip
 (4) 

The method based on the unit circle diagram in complex plane is as following, 

Step 1: Choosing the controlled variables and potential bypasses of HENs, then calculates the Λ(ω). 

Step 2: Since Λ(ω) is a function of ω, the integral mean of Λ(ω) to ω is calculated in Eq(5). And Λ0 is defined as 

average ns-RGA in the frequency domain. 


−

=
n

dΛΛ
n






 0
)(

1

0

0
 (5) 

In this paper the ω0 is 0, and the ωn is the bandwidth. 

Based on ns-RGA in the frequency domain, some principles are obtained when potential bypasses and 

controlled variables in a control loop are paired. 

(1) Removing the potential bypasses with interaction measurement indexes of 1 or close to 1. 

(2) Drawing the remaining bypasses on unit circle of complex plane and removing the bypasses in the III and 

IV regions. 

(3) Selecting the point close to the (1, 0j) point on unit circle of complex plane as the potential optimal bypass. 

3.2 Controller parameters design 

The interaction of potential bypasses and controlled variables is analyzed in section 3.1. However, controller 

parameters are neglected making it hard to meet stability margins.  

Assume that HENs is a second-order system, and its frequency characteristics are describe as Eq(6), 






ja

jcd
jG

+

+
=

2
-b

)(  (6) 

The frequency characteristics of PI controller is shown in Eq(7), 

j
K

KjG I
Pc


 −=)(  (7) 

The frequency characteristics of control system is shown in Eq(8), 

)(
)-b(

)()(
2

j
K

K
ja

jcd
jGjG I

pc



 −

+

+
=

 
(8) 

Controller parameters KP and KI are non-negative. Assumed that gain margin and phase margin are Am and φm 

respectively. The crossover frequency and cut-off frequency are ωx and ωc. 













+

−+
=

+

+−
−=

)(

)(

)(

)(

22

x

2

xx

3

xx

22

x

2

2

x

2

x

dcA

bcadc
K

dcA

acdbd
K

m

I

m

P







  

(9) 

 













+

+−
+

+

+−
=

+

+−
−

+

+−
=

22

c

2

3

cccc

22

c

2

2

c

2

cc

222

2

c

2

c

222

2

cc

))(cos())(sin(

))(cos())(sin(

dc

cbcad

dc

acdbd
K

dc

acdbd

dc

cbcad
K

mm
I

mm
P















 

(10) 

Therefore, a proper region of KP and KI can be calculated by Eq(9) and Eq(10) to meet the requirements of 

stability margins.  

766



A control loop should meet the stability requirements. Figure 4 shows the steps of BCS design in HENs based 

on frequency domain analysis. 

 

Begin

End

The one with positive KP and KI is set as 

the optimal bypass of controlled 

temperature i

Yes
KP or KI is 

negetive

Calculating KP and KI according to Eq(9) 

and Eq(10)

Dip and Λ are obtained according to Eq(4) 

and Eq(5)

 Removing the potential bypasses with IMI 

of 1 or close to 1

Determining the optimal bypass according 

to pairing rules (2) and (3)

No

 

Figure 4: Control system process design of HENs 

4. Case study 

A simple HENs provided by Sun et al. (2011). The controlled target is the output temperature of hot stream and 

there are four potential bypasses in this HEN. The IMI in the frequency domain are shown in Table 2. According 

to pairing rules, Ns-RGA in the frequency domain described on the unit circle diagram are shown in Figure 5a. 

From the Figure 5a, the hot stream of heat exchanger 2 is the potential optimal bypass. 

Table 2: IMI and ns-RGA in the frequency domain 

Potential bypasses 
Hot stream of heat 

exchanger 1 

Cold stream of heat 

exchanger 1 

Hot stream of heat 

exchanger 2 

Cold stream of heat 

exchanger 2 

IMI 0.6356 0.9623 0.4805 0.8886 

 

I

III

IIIV

(1,0)
(-1,0)

(0.1174-0.0258i)
(0.0589-0.0752i)

(0.2373+0.011i)

 

 

0 200 400 600 800 1000 1200
69.60

69.65

69.70

69.75

69.80

69.85

69.90

69.95

70.00

70.05

o
u

tp
u

t 
te

m
p

e
ra

tu
re

time /s

 in this paper

 Hou et al. (2011)

 

Figure 5a: Average ns-RGA in the frequency domain Figure 5b: Output temperature of hot stream 

767



KP and KI are designed according to Eq(9) and Eq(10). When KP and KI is 0.5334 and 0.942, respectively, the 

gain margin and phase margin are 52db and 36°. KP and KI are non-negative. So the hot stream of heat 

exchanger 2 is the optimal bypass. 

Hou et al. (2011) have studied structural controllability to design optimal bypass location and the result of optimal 

bypass is hot stream of heat exchanger 1 based on structural controllability. Therefore, when the input 

temperature of hot stream is changed from 190℃ to 185℃, the output temperature of hot stream under the 

control of Hou et al. (2011) and this paper is shown in Figure 5b. It can be concluded from Figure 5b that output 

temperature in this paper has faster response speed and smaller overshoot than the method in Hou et al. (2011); 

hence the control performance is better.  

5. Conclusions 

In this work bypass control system design based on frequency domain analysis considering stability margins 

has been addressed because previous studies only explored ns-RGA in the time domain using steady-state 

HENs. Then ns-RGA in the frequency domain is proposed to optimize potential bypasses. The main conclusions 

of this paper are as follows: 

(1) It is proved that the flexible HENs is over stable, and stability margins should be considered when designing 

the control system. 

(2) The IMI and ns-RGA in the frequency domain is used to analyze the optimal bypass combined the dynamic 

characteristics. On the basis of optimal bypasses and tuning strategies in PI controlled HENs, the control system 

will have a proper stability margins with gain margin of 3db-6db and phase margin of 30°-60°.  

(3) This method will have a better control performance compared with other method based on ns-RGA in the 

time domain. 

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