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TELKOMNIKA Indonesian Journal of Electrical Engineering
Vol.12, No.1, January 2014, pp. 422 ~ 432
DOI: http://dx.doi.org/10.11591/telkomnika.v12i1.4146  422
Received June 27, 2013; Revised August 28, 2013; Accepted September 20, 2013
Stabilizing Planar Inverted Pendulum System Based on
Fuzzy Nine-point Controller
Tang Yong-chuan, Liu Feng*, Qi Qian, Yang Yang
College of Computer and Information Science, Southwest University; Chongqing Engineering Research
Center for Instrument and Control Equipment
No.2, Tiansheng Road, Beibei District, Chongqing 400715, P.R.China; +86 23 68252940
*Corresponding author, e-mail: liuf@swu.edu.cn
Abstract
In order to stabilize planar inverted pendulum, after analyzing the physical characteristics of the
planar inverted pendulum system, a pendulum nine-point controller and a car nine-point controller for X-
axis and Y-axis were designed respectively. Then a fuzzy coordinator was designed using the fuzzy
control theory based on the priority of those two controllers, and the priority level of the pendulum is higher
than the car. Thus, the control tasks of each controller in each axis were harmonized successfully. The
designed control strategy did not depend on mathematical model of the system; it depended on the control
experience of people or the control experts. The compared experiments showed that the control strategy
was easy and effective, what was’s more; it had a very good robust feature.
Keywords: planar inverted pendulum; nine-point controller; fuzzy coordinator
Copyright © 2014 Institute of Advanced Engineering and Science. All rights reserved.
1. Introduction
Inverted pendulum is an absolute instable, high-level, multi-variable, less-driven and
strong coupling nonlinear system. These characteristics make it an ideal device to examine if a
control method is available. Basing on the base motion forms, inverted pendulum is divided into
linear inverted pendulum, circular inverted pendulum and planar inverted pendulum, among
these forms of inverted pendulum, planar inverted pendulum has a stronger features of high-
level, multi-variable and strong coupling. So, there are more challenges to research the planar
inverted pendulum, and the control technologies basing on the planar inverted pendulum have
been widely used in rocket launching, robot control and other field in industry control. In the
literature [1-4], the research basing on planar inverted pendulum system, specifically, in [1-2],
sliding mode control is applied to stabilize the planar inverted pendulum; in [3], sliding mode
control theory is used to control the circular movement and the stabilization; in [4], the LQR
control method is used to control the stabilization of planar inverted pendulum basing on the
mathematical model of the system; in [1-4], all the control behavior is based on the mathematic
model of the system in different degrees. In [5-11], the control behavior is based on linear
inverted pendulum; in [5], the variable universe adaptive fuzzy control is used to stabilize the
quadruple inverted pendulum, and the mathematical model parameters of high degree accuracy
is applied in deducing the deviation fusion function; in [6], the cloud control method is used to
stabilize the triple inverted pendulum system; in [7-8], the human simulated intelligent control
theory is used to stabilize the linear multi-pendulum system, and the LQR theory is used to
steady the pendulum, which is also based on mathematical model; in [9], the fuzzy control
theory is used in swinging up and the LQR theory is used to steady the pendulum. Among the
present intelligent control theory in inverted pendulum control, in [10], it’s adaptive fuzzy control
method; in [11], it’s the single rule of fuzzy control method; in [10-11], there’s no mathematical
model, but they are all based on linear inverted pendulum and there are more challenges for
stabilizing the planar inverted pendulum.
Nine-point controller [12] is a new intelligent control theory and it’s based on pan-
Boolean algebra theory. In which, a system is divided into plus-minus nine control effect with
strong and weak differ. Basing on the change of the error and its derivative in the system, the
control effect is changing over time. In [13], a fuzzy nine-point controller for linear inverted
pendulum is designed for the first time.
 ISSN: 2302-4046 TELKOMNIKA
TELKOMNIKA Vol. 12, No. 1, January 2014: 422 – 432
423
In this paper, the fuzzy nine-point controller is designed for planar inverted pendulum
system, compared to the control strategy in [1-9], there is no mathematical model and it has a
good robust feature. It is a good control strategy for a single input multi-output (SIMO)
complicated system with strong nonlinear feature.
2. System Model Description
The planar single inverted pendulum comprises two rails in X-axis and Y-axis, a cart,
and a pendulum; as is shown in Figure1. The cart can move along the rail of Y-axis, while the
whole rail of Y-axis can move along the rail of X-axis, in this way, the cart can move within the
planar plane. The pendulum, which is set on the cart by a Hooke’s joint, can rotate around X-
axis and Y-axis. At any instant, the pendulum divarate from OZ direction x within XOZ plane,
as well as y within YOZ plane; as is shown in Figure1.
 
y
M
o
X
Y
Z
+
+
+
x
+ +
t he X-axi s rai l
t he pendul um
t he Y-axi s rai l
the cart
Figure 1. The setup of planar inverted
pendulum system
o X
Z
+

+
M
-
- x
Figure 2. The setup of planar inverted
pendulum in XOZ plane
Take the motion behavior in XOZ plane as an example, the pendulum, which is on the
base cart, slide along the X-axis guide rail; as is shown in Figure 2.
In Figure 2, x is the the cart's displacement in X-axis with meter unit (To the left is the
positive direction and to the right is the negative direction).  represents the angle of the rod
deviating from the upright position in XOZ plane (Clockwise direction is positive). According to
the control experience, if the pendulum is deviating from the upright position clockwise, the
pendulum controller should control the cart move to the right direction, in this way, the pendulum
will go back to its equilibrium position by rotating anticlockwise. On the contrary, if the pendulum
is deviating from the upright position anticlockwise, the pendulum controller should control the
cart move to the left direction, and the pendulum will go back to its equilibrium position by
rotating clockwise.
The cart controller will control the cart indirectly. If the cart is leaving the original point to
its right direction, the cart controller should keep its move to the right direction, and this behavior
will lead the pendulum deviate from the upright position clockwise, and at this moment the
pendulum controller will have the cart move to the left direction, so the pendulum will rotate
clockwise and go back to its equilibrium position, of course, the cart will go back to its original
position automatically. If the cart is leaving the original point to its left direction, the movement
behavior will be on the contary as is described above.
Accoding to the analysis above, in order to stabilize the planar inverted pendulum
system, a strong coordinator is needed to harmonize the behavior between the pendulum
controller and the cart controller. Basing on the physical understanding described above, the
control stratege for the planar inverted pendulum system is designed, as is shown in Figure 3.
ISSN: 2302-4046 
Stabilizing Planar Inverted Pendulum System Based on Fuzzy Nine-point Controller (Liu Feng)
424
the cart ni ne-poi nt
control l er
the pendul um
ni ne-poi nt control l er
fuzzy
coordi
-nator
X-axi s
1F
2F
u
re
re&
-
t he angl e and
i t s di ri vat i ve
t he cart
di spl acement
-
ce
the cart ni ne-poi nt
control l er
the pendul um
ni ne-poi nt control l er
fuzzy
coordi
-nator
Y-axi s
1F
2F
u
re
re&
-
-
ce t he cart
di spl acement
t he angl e and
i t s di ri vat i ve
Pl anar
I nverted
Pendul um
Figure 3. The scheme of the control system
0e&
0e0-e
0-e&
e&
e0f
1f 
1f 
3f 
2f 
3f 
2f 4f 
4f 
Figure 4. The theory of nine-point controller
The motion behavior in YOZ plane is similar with XOZ plane. Here no longer repeat
them.
3. Design the Controller
The contrller design includes designing the pendulum nine-point controller and the cart
nine-point controller of the planar inverted pendulum shown in Figure 3, as well as the fuzzy
coordinator in Figure 3.
3.1. The Nine-point Controller
The nine-point contrller[12]
theory, as is shown in Figure 4, it divide the phase plane into
nine control zones, basing on the zero zone of deviation 0| |e e and the deviation derivative
0| |e e& &. Then the control effect of the whole system is divided into nine part, with plus-minus
differ, as well as strong and weak differ.
For example, if the sysetm state is 0e e and 0e e& &, it means the error is very big in
plus direction, so the system need the strongest control effect 4f  with plus direction, in this way
to enlarge the output and reduce the deviation; the other eight zones can be done in the same
manner, if the system state is 0e e and 0| |e e& &, apply the strong control effect 3f  with plus
direction to the system;if the system state is 0e e and 0e e & &, apply the weak control effect
2f  with plus direction to the system; if the system state is 0| |e e and 0e e& &, apply the
weakest control effect 1f  with plus direction to the system; if the system state is 0e e  and
0e e & &, appply the strongest control effect 4f  with minus direction to the system; if the system
state is 0e e  and 0| |e e& &, apply the strong control effect 3f  with minus direction to the
system; if the system state is 0e e  and 0e e& &, apply the weak control effect 2f  with minus
direction to the system; if the system state is 0| |e e and 0e e & &, apply the weakest control
effect 1f  with minus direction to the system; if the system state is 0| |e e and 0| |e e& &, appy
the maintaining control effect 0f .
Basing on the pendulum physical knowledges within the whole system and the nine-
point controller theory mentioned above, if the pendulum is deviating from the upright
equilibrium position with clockwise with a high angular rate, then the system state should be
 ISSN: 2302-4046 TELKOMNIKA
TELKOMNIKA Vol. 12, No. 1, January 2014: 422 – 432
425
0e e and 0e e& &, at this time the cart should move fastly to the right direction to help the
pendulum back to its equilibrium position, so it should be the strongest control effect with plus
direction. If the pendulum’s behavior is within other control effect zone of the nine-point
controller theory, the control effect is given in table 1, and table 1 is the pendulum nine-point
controller (the control effect in the parentheses is for the Y-axis, which is different from the X-
axis). Here re and re&is the pendulum error and its changing rate, and their zero boundary is
0 =0.0087e rad and 0 0.01 /e rad s& respectively.
Table 1. The Rod Nine-point Controller
re& 0e& | |re&  0e& re&- 0e&
re  0e -19(21) -10 -7
| |re  0e -2.5 0 2.7(2.4)
re  - 0e 7.3(6.5) 10.5(9.5) 21(20)
Table 2. The Cart Nine-point Controller
ce& '
0e& | |ce&  '
0e& ce&-
'
0e&
ce  '
0e -2.5 -1 -0.7
ce  '
0e -0.5 0 0.7
ce -
'
0e 0.9 1.8 3(2.5)
Basing on the analysis about the cart motion behavior and the nine-point controller
theory, if the cart is leaving the original point to its left direction and keep enlarging the
displacement, the system state is 0ce e and 0ce e& &, the cart controller should help keep the
cart moving to its left direction, in this way, the pendulum controller will be activated, so the
control effect should be the strongest with minus dirction. Here table 2 shows the cart nine-point
controller (the control effect in the parentheses is for the Y-axis, which is different from the X-
axis). Here ce and ce& represents the cart’s displacement error and its speed, and their zero
boundary is
'
0 0.02e cm and
'
0 =0.04 /e m s& respectively.
3.2. The Fuzzy Coordinator
While applying the pendulum nine-point controller and the cart nine-point controller to
the planar invereted pendulum system synchronously, a coordinator is needed. Take 1c and 2c
as the coordinator of the pendulum nine-point controller output 1F and the cart nine-point
controller output 2F respectively. The final control effect for each axis is 1 2 21u = c F c F . In
order to coordinate the control effect on-line, the 1c and 2c is adjusted on-line with fuzzy control
methods.
The priority task is steady the pendulum, then it is the cart’s going back to original
position; so the pendulum has a higher priority than the cart. Here choosing the absolute value
of the pendulum deviation | |re and its changing rate | |re& as the leading variable of the fuzzy
coordinator, and the universe for the | |re and | |re& is [0, 15o
] and [0, 1] respectively; the fuzzy
set for | |re and | |re& is designed in Figure 5 and Figure 6 respectively. The outcome variables
1c and 2c , their universe are the same and it is [0,1], and the fuzzy set for the coordinators is
shown in Figure 7.
As the pendulum has a higher priority than the cart, so if the pendulum error and its
changing rate is big, the pendulume controller should be the main control effect to help the
pendulum go back to its upright equilibrium position as soon as possible. On the contrary,if the
pendulum error and its changing rate is very small, the cart nine-point controller will be the main
controller to help the cart go back to its original position. Basing on these knowledges, 25 fuzzy
rules are designed in table 3. For example, if | |re is 1A and | |re& is 1A , so 1c should be 1B and
ISSN: 2302-4046 
Stabilizing Planar Inverted Pendulum System Based on Fuzzy Nine-point Controller (Liu Feng)
426
2c shall be 9B ; and the rest can be done in the same manner. Table 3 shows all the fuzzy rules
of 1c and 2c .
| |re
0 3. 75 7. 5 11. 25 15
Membership
1
1A 2A 3A 4A 5A
0. 5
Figure 5. The fuzzy set of pendulum error
| |re&
0 0. 25 0. 50 0. 75 1. 00
Membership
1
1A 2A 3A 4A 5A
0. 05
Figure 6. The fuzzy set of changing rate of
pendulum error
1 2,c c
Membership
1
1B 2B 3B 4B 5B 6B 7B 8B 9B
1
8
1
4
3
8
1
2
5
8
3
4
7
8
1.01
20
0
Figure 7. The fuzzy set of coordinator
Table 3. The Fuzzy Rules of Coordinator
1| | Are & 2| | Are & 3| | Are & 4| | Are & 5| | Are &
1c 2c 1c 2c 1c 2c 1c 2c 1c 2c
1| | Are  1B 9B 2B 8B 3B 7B 4B 6B 5B 5B
2| | Are  2B 8B 3B 7B 4B 6B 5B 5B 6B 4B
3| | Are  3B 7B 4B 6B 5B 5B 6B 4B 7B 3B
4| | Are  4B 6B 5B 5B 6B 4B 7B 3B 8B 2B
5| | Are  5B 5B 6B 4B 7B 3B 8B 2B 9B 1B
Basing on product inference engine, singleton fuzzifier and center average defuzzifier in
fuzzy control theory[14]
, the function of 1c and 2c are shown as function(1).
5, 5
( 1)
1, 1
1
(| |) (| |)
(| |) (| |)
i j
i j
i j
i j A r A r
i j
1
A r A r
b u e u e
c k
u e u e
 
 
 

 &
&
,
5, 5
(10 )
1, 1
2 2
(| |) (| |)
(| |) (| |)
i j
i j
i j
i j A r A r
i j
A r A r
b u e u e
c k
u e u e
 
 
 

 &
&
(1)
 ISSN: 2302-4046 TELKOMNIKA
TELKOMNIKA Vol. 12, No. 1, January 2014: 422 – 432
427
In function (1), 1k and 2k are scaling factors to adjust the weight of 1c and 2c
respectively, ( 1)i jb   represents the central point of fuzzy set ( 1)i jB   ( , 1,2,...,5i j  ), (| |)iA ru e
and (| |)jA ru e& are the membership function of the fuzzy set iA and jA respectively.
4. Robust Control Experiment
Set up the simulation control system of planar inverted pendulum in MATLAB software
basing on the designed control strategy in Figure 3. Choose 5 milisecond as the control cycle to
stabilize the planar inverted pendulum. Set the deviation from the upright with +5o
to start the
experiment, and choose the scaling factor in X-axis with 1k =3.4 and 2k =3.4, and in Y-axis they
are 1k =3.4 and 2k =3.5.
For the first experiment, the pendulum is a long rod with the length is 50 centimeters
and the weight is 110 gram (Here, the “long” rod is differ from the “short” one with the length is
40 centimeters, which will be used in the second experiment). The outcome of this experiment
are shown from Figure 8 to Figure 14.
Figure 8 shows that the pendulum will overcome the initial deviation in X-axis and Y-
axis and keep a fine adjustment at last. In Figure 9, the biggest displacement in X-axis is 16
centimeter, while in Y-axis is 12 centimeter; the displacement in X-axis is a little bigger than in
Y-axis, because the whole Y-rail is moving along the X-rail. Figure 10 and Figure 11 show that
the pendulum/cart controller act as the pendulum/cart nine-point controller designed in table 1
and table 2; as time goes on, the error is smaller and smaller, so the changing over the nine
zones more frequently and the curves are more dense.
(a) In X-axis (b) In Y-axis
Figure 8. The pendulum error of long rod
(a) In X-axis (b) In Y-axis
Figure 9. The cart displacement of long rod
ISSN: 2302-4046 
Stabilizing Planar Inverted Pendulum System Based on Fuzzy Nine-point Controller (Liu Feng)
428
Figure 12 and Figure 13 show the changes of 1c and 2c , in the beginning, the pendulum
error is much bigger than the cart error, so 1c has a bigger value than 2c , later the pendulum
error becomes smaller, and at this time 2c has a bigger value than 1c ; the curves show very
well of the changing process, it also confirm that the priority of the pendulum controller is higher
than that of the cart. Figure 14 gives the change tendency of final control effect, the output
ranges from -60 to 70 in X-axis, and in Y-axis it is from -70 to 68, and they always keep
changing slightly.
(a) In X-axis (b) In Y-axis
Figure 10. The pendulum nine-point controller output of long rod
(a) In X-axis (b) In Y-axis
Figure 11. The cart nine-point controller output of long rod
(a) In X-axis (b) In Y-axis
Figure 12. The change tendency of 1c with long rod
 ISSN: 2302-4046 TELKOMNIKA
TELKOMNIKA Vol. 12, No. 1, January 2014: 422 – 432
429
(a) In X-axis (b) In Y-axis
Figure 13. The change tendency of 2c with long rod
(a) In X-axis (b) In Y-axis
Figure 14. The control force u of long rod
In order to confirm the effectiveness of the designed control strategy, also to show its
robust feature, a controlled trial is designed. This time the pendulum is replaced by a short rod
with a length of 40 centimeter and the weight is 90 gram. Besides, all the other parameters of
the controller is the same with the first experiment with a long rod. This time, the outcome of the
experiment are shown as Figure 15 to Figure 21.
The outcome in Figure 15 is quite similar with Figure 8. In Figure 16 (a) and (b), the
largest displacement in X-axis and Y-axis is 12.5 centimeter and 12 centimeter respectively.
Both the pendulum and the cart can go back toits equilibrium position (For the displacement, it’s
very close to its original point) and keep fine adjustment.
(a) In X-axis (b) In Y-axis
Figure 15. The rod error of short rod
ISSN: 2302-4046 
Stabilizing Planar Inverted Pendulum System Based on Fuzzy Nine-point Controller (Liu Feng)
430
Figure 17 and Figure 18 are similar to Figure 10 and Figure 11 respectively, the
pendulum/cart controller act as the pendulum/cart nine-point controller designed in table 1 and
table 2. Figure 19 and Figure 20 are similar to Figure 12 and Figure 13 respectively; the curves
confirm that the priority of the pendulum controller is higher than that of the cart. In Figure 21 (a)
and (b), the range of the control force in X-axis is [-60, 70], and in Y-axis, it is [-70, 65].
(a) In X-axis (b) In Y-axis
Figure 16. The cart displacement of short rod
(a) In X-axis (b) In Y-axis
Figure 17. The pendulum nine-point controller output of short rod
(a) In X-axis (b) In Y-axis
Figure 18. The cart nine-point controller output of short rod
 ISSN: 2302-4046 TELKOMNIKA
TELKOMNIKA Vol. 12, No. 1, January 2014: 422 – 432
431
(a) In X-axis (b) In Y-axis
Figure 19. The change tendency of 1c with short rod
(a) In X-axis (b) In Y-axis
Figure 20. The change tendency of 2c with short rod
(a) In X-axis (b) In Y-axis
Figure 21. The control force u of short rod
The robust control experiments show the effectiveness of the designed control strategy.
5. Conclusion
This paper analyze the physical features of planar inverted pendulum and its control
logic, then design a pendulum nine-point controller and a cart nine-point controller for X-axis
and Y-axis based on the nine-point controller theory. What’s more, this paper designed a
coordinator to harmonize these two nine-point controllers in each axis based on the priority of
each controller. Robust control experiments show that the control strategy is effective, as well
as has a good robust feature. It is a new control strategy for expressing human control
experiments, and human beings or control specialists are always the master in control system.
ISSN: 2302-4046 
Stabilizing Planar Inverted Pendulum System Based on Fuzzy Nine-point Controller (Liu Feng)
432
Acknowledgement
This work was supported by the National High Technology Research and Development
Program of China (Grant No. 2012AA041101), and China Fundamental Research Funds for the
Central Universities Special Fund (Grant No. XDJK2013C119).
References
[1] Rong-Jong Wai, Li-Jung Chang. Adaptive stabilizing and tracking control for a nonlinear inverted
pendulum system via sliding mode technique. IEEE trans. on industrial electronics. 2006; 53(2): 674-
692.
[2] DUAN Xue-chao, QIU Yuan-ying, DUAN Bao-yan. Adaptive sliding mode fuzzy control of planar
inverted pendulum. Control and Decision. 2007; 22(7): 775-777,782.
[3] DUAN Xue-chao, QIU Yuan-ying, SHENG Ying. Circular Motion and Balance Control of the Planar
Double Inverted Pendulum. Acta Automatica Sinica. 2007; 33(12): 1337-1340.
[4] Liu Feng, Tang Yongchuan, Qi Qian. Stabilize the Planar Single Inverted Pendulum Based on LQR.
Proceedings of the 5th IEEE International Conference on Automation and Logistics (ICAL).
Chongqing. 2011; 238-242.
[5] LI H X, MIAO ZH H, WANG JY. Variable universe adaptive fuzzy control on the quadruple inverted
pendulum. Science in China (Series E). 2002; 45(2): 213-224.
[6] Li Deyi. The Cloud Control Method and Balancing Patterns of Triple Link Inverted Pendulum Systems.
Engineering Science in China. 1999; 1(2): 41-46.
[7] Li Zushu, Dan Yuanhong, Wen Yongling, etc. Swing-up and handstand control of cart-triple-pendulum
system based on human simulated intelligent control theory. Journal of Huazhong University of
Science and Technology, Nature Science. 2004; 32(S1): 38-41.
[8] Tu Xuyan. Artificial Intelligence: Review & Prospect. Beijing: Science Press. 2006: 174-207.
[9] Muskinja N, Tovornik B. swing up and stabilization of a real inverted pendulum. IEEE Trans. on
Industrial Electronics. 2006; 53(2): 631-639.
[10] Wang LX. Stable adaptive fuzzy controllers with application to inverted pendulum tracking. IEEE
Trans. on System, Man, and Cybernetics-Part B. 1996; 26(5): 677-691.
[11] YI JQ, Yubazaki N, Hirota K. Upswing and stabilization control of inverted pendulum system based on
the SIRMs dynamically connected fuzzy inference model. Fuzzy sets and systems. 2001; 122: 139-
152.
[12] Zhang Nanlun. The new control principle.Beijing: National Defense Industry Press. 2005: 60-71.
[13] Qi Qian, Li Zushu, Tan zhi, etc. Fuzzy nine-point controller and its application in the inverted
pendulum. Chinese Journal of Scientific Instrument. 2010; 31(6); 1249-1254.
[14] WANG LX. Fuzzy system and fuzzy control. Beijing: Tsinghua University Press. 2003: 90-93.

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Stabilizing Planar Inverted Pendulum System Based on Fuzzy Nine-point Controller

  • 1. TELKOMNIKA Indonesian Journal of Electrical Engineering Vol.12, No.1, January 2014, pp. 422 ~ 432 DOI: http://dx.doi.org/10.11591/telkomnika.v12i1.4146  422 Received June 27, 2013; Revised August 28, 2013; Accepted September 20, 2013 Stabilizing Planar Inverted Pendulum System Based on Fuzzy Nine-point Controller Tang Yong-chuan, Liu Feng*, Qi Qian, Yang Yang College of Computer and Information Science, Southwest University; Chongqing Engineering Research Center for Instrument and Control Equipment No.2, Tiansheng Road, Beibei District, Chongqing 400715, P.R.China; +86 23 68252940 *Corresponding author, e-mail: liuf@swu.edu.cn Abstract In order to stabilize planar inverted pendulum, after analyzing the physical characteristics of the planar inverted pendulum system, a pendulum nine-point controller and a car nine-point controller for X- axis and Y-axis were designed respectively. Then a fuzzy coordinator was designed using the fuzzy control theory based on the priority of those two controllers, and the priority level of the pendulum is higher than the car. Thus, the control tasks of each controller in each axis were harmonized successfully. The designed control strategy did not depend on mathematical model of the system; it depended on the control experience of people or the control experts. The compared experiments showed that the control strategy was easy and effective, what was’s more; it had a very good robust feature. Keywords: planar inverted pendulum; nine-point controller; fuzzy coordinator Copyright © 2014 Institute of Advanced Engineering and Science. All rights reserved. 1. Introduction Inverted pendulum is an absolute instable, high-level, multi-variable, less-driven and strong coupling nonlinear system. These characteristics make it an ideal device to examine if a control method is available. Basing on the base motion forms, inverted pendulum is divided into linear inverted pendulum, circular inverted pendulum and planar inverted pendulum, among these forms of inverted pendulum, planar inverted pendulum has a stronger features of high- level, multi-variable and strong coupling. So, there are more challenges to research the planar inverted pendulum, and the control technologies basing on the planar inverted pendulum have been widely used in rocket launching, robot control and other field in industry control. In the literature [1-4], the research basing on planar inverted pendulum system, specifically, in [1-2], sliding mode control is applied to stabilize the planar inverted pendulum; in [3], sliding mode control theory is used to control the circular movement and the stabilization; in [4], the LQR control method is used to control the stabilization of planar inverted pendulum basing on the mathematical model of the system; in [1-4], all the control behavior is based on the mathematic model of the system in different degrees. In [5-11], the control behavior is based on linear inverted pendulum; in [5], the variable universe adaptive fuzzy control is used to stabilize the quadruple inverted pendulum, and the mathematical model parameters of high degree accuracy is applied in deducing the deviation fusion function; in [6], the cloud control method is used to stabilize the triple inverted pendulum system; in [7-8], the human simulated intelligent control theory is used to stabilize the linear multi-pendulum system, and the LQR theory is used to steady the pendulum, which is also based on mathematical model; in [9], the fuzzy control theory is used in swinging up and the LQR theory is used to steady the pendulum. Among the present intelligent control theory in inverted pendulum control, in [10], it’s adaptive fuzzy control method; in [11], it’s the single rule of fuzzy control method; in [10-11], there’s no mathematical model, but they are all based on linear inverted pendulum and there are more challenges for stabilizing the planar inverted pendulum. Nine-point controller [12] is a new intelligent control theory and it’s based on pan- Boolean algebra theory. In which, a system is divided into plus-minus nine control effect with strong and weak differ. Basing on the change of the error and its derivative in the system, the control effect is changing over time. In [13], a fuzzy nine-point controller for linear inverted pendulum is designed for the first time.
  • 2.  ISSN: 2302-4046 TELKOMNIKA TELKOMNIKA Vol. 12, No. 1, January 2014: 422 – 432 423 In this paper, the fuzzy nine-point controller is designed for planar inverted pendulum system, compared to the control strategy in [1-9], there is no mathematical model and it has a good robust feature. It is a good control strategy for a single input multi-output (SIMO) complicated system with strong nonlinear feature. 2. System Model Description The planar single inverted pendulum comprises two rails in X-axis and Y-axis, a cart, and a pendulum; as is shown in Figure1. The cart can move along the rail of Y-axis, while the whole rail of Y-axis can move along the rail of X-axis, in this way, the cart can move within the planar plane. The pendulum, which is set on the cart by a Hooke’s joint, can rotate around X- axis and Y-axis. At any instant, the pendulum divarate from OZ direction x within XOZ plane, as well as y within YOZ plane; as is shown in Figure1.   y M o X Y Z + + + x + + t he X-axi s rai l t he pendul um t he Y-axi s rai l the cart Figure 1. The setup of planar inverted pendulum system o X Z +  + M - - x Figure 2. The setup of planar inverted pendulum in XOZ plane Take the motion behavior in XOZ plane as an example, the pendulum, which is on the base cart, slide along the X-axis guide rail; as is shown in Figure 2. In Figure 2, x is the the cart's displacement in X-axis with meter unit (To the left is the positive direction and to the right is the negative direction).  represents the angle of the rod deviating from the upright position in XOZ plane (Clockwise direction is positive). According to the control experience, if the pendulum is deviating from the upright position clockwise, the pendulum controller should control the cart move to the right direction, in this way, the pendulum will go back to its equilibrium position by rotating anticlockwise. On the contrary, if the pendulum is deviating from the upright position anticlockwise, the pendulum controller should control the cart move to the left direction, and the pendulum will go back to its equilibrium position by rotating clockwise. The cart controller will control the cart indirectly. If the cart is leaving the original point to its right direction, the cart controller should keep its move to the right direction, and this behavior will lead the pendulum deviate from the upright position clockwise, and at this moment the pendulum controller will have the cart move to the left direction, so the pendulum will rotate clockwise and go back to its equilibrium position, of course, the cart will go back to its original position automatically. If the cart is leaving the original point to its left direction, the movement behavior will be on the contary as is described above. Accoding to the analysis above, in order to stabilize the planar inverted pendulum system, a strong coordinator is needed to harmonize the behavior between the pendulum controller and the cart controller. Basing on the physical understanding described above, the control stratege for the planar inverted pendulum system is designed, as is shown in Figure 3.
  • 3. ISSN: 2302-4046  Stabilizing Planar Inverted Pendulum System Based on Fuzzy Nine-point Controller (Liu Feng) 424 the cart ni ne-poi nt control l er the pendul um ni ne-poi nt control l er fuzzy coordi -nator X-axi s 1F 2F u re re& - t he angl e and i t s di ri vat i ve t he cart di spl acement - ce the cart ni ne-poi nt control l er the pendul um ni ne-poi nt control l er fuzzy coordi -nator Y-axi s 1F 2F u re re& - - ce t he cart di spl acement t he angl e and i t s di ri vat i ve Pl anar I nverted Pendul um Figure 3. The scheme of the control system 0e& 0e0-e 0-e& e& e0f 1f  1f  3f  2f  3f  2f 4f  4f  Figure 4. The theory of nine-point controller The motion behavior in YOZ plane is similar with XOZ plane. Here no longer repeat them. 3. Design the Controller The contrller design includes designing the pendulum nine-point controller and the cart nine-point controller of the planar inverted pendulum shown in Figure 3, as well as the fuzzy coordinator in Figure 3. 3.1. The Nine-point Controller The nine-point contrller[12] theory, as is shown in Figure 4, it divide the phase plane into nine control zones, basing on the zero zone of deviation 0| |e e and the deviation derivative 0| |e e& &. Then the control effect of the whole system is divided into nine part, with plus-minus differ, as well as strong and weak differ. For example, if the sysetm state is 0e e and 0e e& &, it means the error is very big in plus direction, so the system need the strongest control effect 4f  with plus direction, in this way to enlarge the output and reduce the deviation; the other eight zones can be done in the same manner, if the system state is 0e e and 0| |e e& &, apply the strong control effect 3f  with plus direction to the system;if the system state is 0e e and 0e e & &, apply the weak control effect 2f  with plus direction to the system; if the system state is 0| |e e and 0e e& &, apply the weakest control effect 1f  with plus direction to the system; if the system state is 0e e  and 0e e & &, appply the strongest control effect 4f  with minus direction to the system; if the system state is 0e e  and 0| |e e& &, apply the strong control effect 3f  with minus direction to the system; if the system state is 0e e  and 0e e& &, apply the weak control effect 2f  with minus direction to the system; if the system state is 0| |e e and 0e e & &, apply the weakest control effect 1f  with minus direction to the system; if the system state is 0| |e e and 0| |e e& &, appy the maintaining control effect 0f . Basing on the pendulum physical knowledges within the whole system and the nine- point controller theory mentioned above, if the pendulum is deviating from the upright equilibrium position with clockwise with a high angular rate, then the system state should be
  • 4.  ISSN: 2302-4046 TELKOMNIKA TELKOMNIKA Vol. 12, No. 1, January 2014: 422 – 432 425 0e e and 0e e& &, at this time the cart should move fastly to the right direction to help the pendulum back to its equilibrium position, so it should be the strongest control effect with plus direction. If the pendulum’s behavior is within other control effect zone of the nine-point controller theory, the control effect is given in table 1, and table 1 is the pendulum nine-point controller (the control effect in the parentheses is for the Y-axis, which is different from the X- axis). Here re and re&is the pendulum error and its changing rate, and their zero boundary is 0 =0.0087e rad and 0 0.01 /e rad s& respectively. Table 1. The Rod Nine-point Controller re& 0e& | |re&  0e& re&- 0e& re  0e -19(21) -10 -7 | |re  0e -2.5 0 2.7(2.4) re  - 0e 7.3(6.5) 10.5(9.5) 21(20) Table 2. The Cart Nine-point Controller ce& ' 0e& | |ce&  ' 0e& ce&- ' 0e& ce  ' 0e -2.5 -1 -0.7 ce  ' 0e -0.5 0 0.7 ce - ' 0e 0.9 1.8 3(2.5) Basing on the analysis about the cart motion behavior and the nine-point controller theory, if the cart is leaving the original point to its left direction and keep enlarging the displacement, the system state is 0ce e and 0ce e& &, the cart controller should help keep the cart moving to its left direction, in this way, the pendulum controller will be activated, so the control effect should be the strongest with minus dirction. Here table 2 shows the cart nine-point controller (the control effect in the parentheses is for the Y-axis, which is different from the X- axis). Here ce and ce& represents the cart’s displacement error and its speed, and their zero boundary is ' 0 0.02e cm and ' 0 =0.04 /e m s& respectively. 3.2. The Fuzzy Coordinator While applying the pendulum nine-point controller and the cart nine-point controller to the planar invereted pendulum system synchronously, a coordinator is needed. Take 1c and 2c as the coordinator of the pendulum nine-point controller output 1F and the cart nine-point controller output 2F respectively. The final control effect for each axis is 1 2 21u = c F c F . In order to coordinate the control effect on-line, the 1c and 2c is adjusted on-line with fuzzy control methods. The priority task is steady the pendulum, then it is the cart’s going back to original position; so the pendulum has a higher priority than the cart. Here choosing the absolute value of the pendulum deviation | |re and its changing rate | |re& as the leading variable of the fuzzy coordinator, and the universe for the | |re and | |re& is [0, 15o ] and [0, 1] respectively; the fuzzy set for | |re and | |re& is designed in Figure 5 and Figure 6 respectively. The outcome variables 1c and 2c , their universe are the same and it is [0,1], and the fuzzy set for the coordinators is shown in Figure 7. As the pendulum has a higher priority than the cart, so if the pendulum error and its changing rate is big, the pendulume controller should be the main control effect to help the pendulum go back to its upright equilibrium position as soon as possible. On the contrary,if the pendulum error and its changing rate is very small, the cart nine-point controller will be the main controller to help the cart go back to its original position. Basing on these knowledges, 25 fuzzy rules are designed in table 3. For example, if | |re is 1A and | |re& is 1A , so 1c should be 1B and
  • 5. ISSN: 2302-4046  Stabilizing Planar Inverted Pendulum System Based on Fuzzy Nine-point Controller (Liu Feng) 426 2c shall be 9B ; and the rest can be done in the same manner. Table 3 shows all the fuzzy rules of 1c and 2c . | |re 0 3. 75 7. 5 11. 25 15 Membership 1 1A 2A 3A 4A 5A 0. 5 Figure 5. The fuzzy set of pendulum error | |re& 0 0. 25 0. 50 0. 75 1. 00 Membership 1 1A 2A 3A 4A 5A 0. 05 Figure 6. The fuzzy set of changing rate of pendulum error 1 2,c c Membership 1 1B 2B 3B 4B 5B 6B 7B 8B 9B 1 8 1 4 3 8 1 2 5 8 3 4 7 8 1.01 20 0 Figure 7. The fuzzy set of coordinator Table 3. The Fuzzy Rules of Coordinator 1| | Are & 2| | Are & 3| | Are & 4| | Are & 5| | Are & 1c 2c 1c 2c 1c 2c 1c 2c 1c 2c 1| | Are  1B 9B 2B 8B 3B 7B 4B 6B 5B 5B 2| | Are  2B 8B 3B 7B 4B 6B 5B 5B 6B 4B 3| | Are  3B 7B 4B 6B 5B 5B 6B 4B 7B 3B 4| | Are  4B 6B 5B 5B 6B 4B 7B 3B 8B 2B 5| | Are  5B 5B 6B 4B 7B 3B 8B 2B 9B 1B Basing on product inference engine, singleton fuzzifier and center average defuzzifier in fuzzy control theory[14] , the function of 1c and 2c are shown as function(1). 5, 5 ( 1) 1, 1 1 (| |) (| |) (| |) (| |) i j i j i j i j A r A r i j 1 A r A r b u e u e c k u e u e         & & , 5, 5 (10 ) 1, 1 2 2 (| |) (| |) (| |) (| |) i j i j i j i j A r A r i j A r A r b u e u e c k u e u e         & & (1)
  • 6.  ISSN: 2302-4046 TELKOMNIKA TELKOMNIKA Vol. 12, No. 1, January 2014: 422 – 432 427 In function (1), 1k and 2k are scaling factors to adjust the weight of 1c and 2c respectively, ( 1)i jb   represents the central point of fuzzy set ( 1)i jB   ( , 1,2,...,5i j  ), (| |)iA ru e and (| |)jA ru e& are the membership function of the fuzzy set iA and jA respectively. 4. Robust Control Experiment Set up the simulation control system of planar inverted pendulum in MATLAB software basing on the designed control strategy in Figure 3. Choose 5 milisecond as the control cycle to stabilize the planar inverted pendulum. Set the deviation from the upright with +5o to start the experiment, and choose the scaling factor in X-axis with 1k =3.4 and 2k =3.4, and in Y-axis they are 1k =3.4 and 2k =3.5. For the first experiment, the pendulum is a long rod with the length is 50 centimeters and the weight is 110 gram (Here, the “long” rod is differ from the “short” one with the length is 40 centimeters, which will be used in the second experiment). The outcome of this experiment are shown from Figure 8 to Figure 14. Figure 8 shows that the pendulum will overcome the initial deviation in X-axis and Y- axis and keep a fine adjustment at last. In Figure 9, the biggest displacement in X-axis is 16 centimeter, while in Y-axis is 12 centimeter; the displacement in X-axis is a little bigger than in Y-axis, because the whole Y-rail is moving along the X-rail. Figure 10 and Figure 11 show that the pendulum/cart controller act as the pendulum/cart nine-point controller designed in table 1 and table 2; as time goes on, the error is smaller and smaller, so the changing over the nine zones more frequently and the curves are more dense. (a) In X-axis (b) In Y-axis Figure 8. The pendulum error of long rod (a) In X-axis (b) In Y-axis Figure 9. The cart displacement of long rod
  • 7. ISSN: 2302-4046  Stabilizing Planar Inverted Pendulum System Based on Fuzzy Nine-point Controller (Liu Feng) 428 Figure 12 and Figure 13 show the changes of 1c and 2c , in the beginning, the pendulum error is much bigger than the cart error, so 1c has a bigger value than 2c , later the pendulum error becomes smaller, and at this time 2c has a bigger value than 1c ; the curves show very well of the changing process, it also confirm that the priority of the pendulum controller is higher than that of the cart. Figure 14 gives the change tendency of final control effect, the output ranges from -60 to 70 in X-axis, and in Y-axis it is from -70 to 68, and they always keep changing slightly. (a) In X-axis (b) In Y-axis Figure 10. The pendulum nine-point controller output of long rod (a) In X-axis (b) In Y-axis Figure 11. The cart nine-point controller output of long rod (a) In X-axis (b) In Y-axis Figure 12. The change tendency of 1c with long rod
  • 8.  ISSN: 2302-4046 TELKOMNIKA TELKOMNIKA Vol. 12, No. 1, January 2014: 422 – 432 429 (a) In X-axis (b) In Y-axis Figure 13. The change tendency of 2c with long rod (a) In X-axis (b) In Y-axis Figure 14. The control force u of long rod In order to confirm the effectiveness of the designed control strategy, also to show its robust feature, a controlled trial is designed. This time the pendulum is replaced by a short rod with a length of 40 centimeter and the weight is 90 gram. Besides, all the other parameters of the controller is the same with the first experiment with a long rod. This time, the outcome of the experiment are shown as Figure 15 to Figure 21. The outcome in Figure 15 is quite similar with Figure 8. In Figure 16 (a) and (b), the largest displacement in X-axis and Y-axis is 12.5 centimeter and 12 centimeter respectively. Both the pendulum and the cart can go back toits equilibrium position (For the displacement, it’s very close to its original point) and keep fine adjustment. (a) In X-axis (b) In Y-axis Figure 15. The rod error of short rod
  • 9. ISSN: 2302-4046  Stabilizing Planar Inverted Pendulum System Based on Fuzzy Nine-point Controller (Liu Feng) 430 Figure 17 and Figure 18 are similar to Figure 10 and Figure 11 respectively, the pendulum/cart controller act as the pendulum/cart nine-point controller designed in table 1 and table 2. Figure 19 and Figure 20 are similar to Figure 12 and Figure 13 respectively; the curves confirm that the priority of the pendulum controller is higher than that of the cart. In Figure 21 (a) and (b), the range of the control force in X-axis is [-60, 70], and in Y-axis, it is [-70, 65]. (a) In X-axis (b) In Y-axis Figure 16. The cart displacement of short rod (a) In X-axis (b) In Y-axis Figure 17. The pendulum nine-point controller output of short rod (a) In X-axis (b) In Y-axis Figure 18. The cart nine-point controller output of short rod
  • 10.  ISSN: 2302-4046 TELKOMNIKA TELKOMNIKA Vol. 12, No. 1, January 2014: 422 – 432 431 (a) In X-axis (b) In Y-axis Figure 19. The change tendency of 1c with short rod (a) In X-axis (b) In Y-axis Figure 20. The change tendency of 2c with short rod (a) In X-axis (b) In Y-axis Figure 21. The control force u of short rod The robust control experiments show the effectiveness of the designed control strategy. 5. Conclusion This paper analyze the physical features of planar inverted pendulum and its control logic, then design a pendulum nine-point controller and a cart nine-point controller for X-axis and Y-axis based on the nine-point controller theory. What’s more, this paper designed a coordinator to harmonize these two nine-point controllers in each axis based on the priority of each controller. Robust control experiments show that the control strategy is effective, as well as has a good robust feature. It is a new control strategy for expressing human control experiments, and human beings or control specialists are always the master in control system.
  • 11. ISSN: 2302-4046  Stabilizing Planar Inverted Pendulum System Based on Fuzzy Nine-point Controller (Liu Feng) 432 Acknowledgement This work was supported by the National High Technology Research and Development Program of China (Grant No. 2012AA041101), and China Fundamental Research Funds for the Central Universities Special Fund (Grant No. XDJK2013C119). References [1] Rong-Jong Wai, Li-Jung Chang. Adaptive stabilizing and tracking control for a nonlinear inverted pendulum system via sliding mode technique. IEEE trans. on industrial electronics. 2006; 53(2): 674- 692. [2] DUAN Xue-chao, QIU Yuan-ying, DUAN Bao-yan. Adaptive sliding mode fuzzy control of planar inverted pendulum. Control and Decision. 2007; 22(7): 775-777,782. [3] DUAN Xue-chao, QIU Yuan-ying, SHENG Ying. Circular Motion and Balance Control of the Planar Double Inverted Pendulum. Acta Automatica Sinica. 2007; 33(12): 1337-1340. [4] Liu Feng, Tang Yongchuan, Qi Qian. Stabilize the Planar Single Inverted Pendulum Based on LQR. Proceedings of the 5th IEEE International Conference on Automation and Logistics (ICAL). Chongqing. 2011; 238-242. [5] LI H X, MIAO ZH H, WANG JY. Variable universe adaptive fuzzy control on the quadruple inverted pendulum. Science in China (Series E). 2002; 45(2): 213-224. [6] Li Deyi. The Cloud Control Method and Balancing Patterns of Triple Link Inverted Pendulum Systems. Engineering Science in China. 1999; 1(2): 41-46. [7] Li Zushu, Dan Yuanhong, Wen Yongling, etc. Swing-up and handstand control of cart-triple-pendulum system based on human simulated intelligent control theory. Journal of Huazhong University of Science and Technology, Nature Science. 2004; 32(S1): 38-41. [8] Tu Xuyan. Artificial Intelligence: Review & Prospect. Beijing: Science Press. 2006: 174-207. [9] Muskinja N, Tovornik B. swing up and stabilization of a real inverted pendulum. IEEE Trans. on Industrial Electronics. 2006; 53(2): 631-639. [10] Wang LX. Stable adaptive fuzzy controllers with application to inverted pendulum tracking. IEEE Trans. on System, Man, and Cybernetics-Part B. 1996; 26(5): 677-691. [11] YI JQ, Yubazaki N, Hirota K. Upswing and stabilization control of inverted pendulum system based on the SIRMs dynamically connected fuzzy inference model. Fuzzy sets and systems. 2001; 122: 139- 152. [12] Zhang Nanlun. The new control principle.Beijing: National Defense Industry Press. 2005: 60-71. [13] Qi Qian, Li Zushu, Tan zhi, etc. Fuzzy nine-point controller and its application in the inverted pendulum. Chinese Journal of Scientific Instrument. 2010; 31(6); 1249-1254. [14] WANG LX. Fuzzy system and fuzzy control. Beijing: Tsinghua University Press. 2003: 90-93.