The Effect of Structural Rigidity Uncertainties on
ATMD Controlled Structures
AYLİN ECE KAYABEKİR1, GEBRAİL BEKDAŞ2*, SİNAN MELİH NİGDELİ2
1Civil Engineering Department,
Istanbul Gelişim University
34310 Avcılar, Istanbul, TURKEY
2Civil Engineering Department
Istanbul University - Cerrahpaşa
34310 Avcılar, Istanbul, TURKEY
Abstract: - For efficiency of active control systems for seismically excited structures, and optimization process
in need. This optimum design is defined according to the certain properties of structures, whereas the structural
properties are found via several assumptions done in material strengths calculations and variable loading. These
factors affect the mass and stiffness of the structure, but it is known that the main factor in the optimum design
of control systems is the frequency that is related to mass and stiffness, generally. In this study, the stiffness of
multiple degrees of freedom structure was reduced and increased to investigate the effect of the robustness of
optimum active control systems for uncertainties. The numerical examination is done for a structure with an
active tuned mass damper (ATMD) that is positioned on the top of the structure. For ±20 stiffness change of
structure, the efficiency of ATMD is between 0.99% and 12.63% for the reduction of maximum displacement.
Key-Words: - Robustness, uncertainties in structures, stiffness, active tuned mass damper
Received: May 26, 2021. Revised: December 27, 2021. Accepted: January 24, 2022. Published: February 15, 2022.
1 Introduction
The known history of the world has witnessed a
constant change and adaptation of human beings
due to their struggle with nature. Especially in
recent years, with the number of people approaching
approximately 8 billion, the changing and
diversifying needs of people led to a rapid change in
the face of the world. This change occurs in almost
every aspect of life, such as the increase in the rate
of urbanization, the rise of buildings, the increase in
energy needs, the expansion of high-speed train
networks and highways due to the need for a global
supply chain and urbanization. However, this
change brings with it new problems that need to be
solved. This change and diversity in structural
systems require them to produce new and innovative
solutions, especially for structural engineers who
have an important responsibility in the creation of
the infrastructure of this change.
Structural control systems developed as a part of
these solutions are among the systems that are
frequently used in order to provide structural safety
and comfort against earthquake and wind-like
vibrations, especially in developed countries in the
earthquake zone. Tuned mass dampers have an
important place in terms of structural application
area among control systems with active, passive,
semi-active and hybrid-like varieties. In the field of
practical application, this situation has also led to a
lot of research on tuned mass dampers.
Some of the scientific studies related to active
tuned mass dampers investigated in this study are
mentioned in this section.
In 1996, Ankireddi and Yang investigated the
effectiveness of the ATMD system against structural
responses caused by wind loads in tall buildings [1].
The effectiveness of the isolation systems attached
to TMD and ATMD controlled structures was
examined by Loh and Chao [2]. Yan et al. obtained
analytical expressions to be used in calculating the
control force [3]. The performances of FLC (Fuzzy
Logic Controller) and LQG (linear quadratic
Gaussian) on vibrations control of tall buildings
controlled with ATMD against along wind
excitations was tested by Aldawod et al. [4]. In the
study, a 76-story building in Melbourne, Australia
was considered, and it was concluded that the FLC
algorithm has slightly better performance. A similar
study was also conducted by Samali et al. and it is
demonstrated that the performance of the FLC
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algorithm is better than LQG [5]. Active multi-tuned
mass dampers (AMTMDs) have also been
investigated and suggested to be used to reduce
structural vibration due to ground motion [6-10].
In the other study, Pourzeynali et al. developed
a method combining genetic algorithm (GA) and
FLC to suppress vibration of high rise buildings
under seismic excitations [11]. Guclu ve Yazici
examined the ATMD system using PD
(proportional+ derivative) control and FLC.
Accordingly, it was concluded that FLC has more
effective active control performance [12]. Then, a
combination of PID (proportional+integral and
derivative) control and FLC was proposed [13].
FLC algorithm was also modified with a self-
tunning mechanism to improve control strategy
[14]. Li et al. introduced a design methodology for
AMTMD to attenuate translational and torsional
responses in asymmetric structures [15]. In the other
study, Li also considered soil-structure interaction
(SSI) for AMTMD attached to asymmetric
structures [16]. A hybrid system consisting of
ATMDs was proposed for retrofit of irregular
buildings against translational and torsional
responses due to seismic excitations by Venanzi and
Materazzi [17]. Then, a methodology using a hybrid
system was developed to reduce flexural and
torsional responses in tall buildings [18]. Sugumar
et al. compared stochastic algorithm and LQG
regulator for building frames with ATMD. In the
study, the stochastic algorithm provided more
effective seismic control [19]. Amini et al.
employed particle swarm optimization (PSO) and
linear quadratic regulator (LQR) in the calculation
of active force. The study demonstrated that PSO
provides better solutions for the structures subjected
to near-fault excitations [20]. Fitzgerald et al.
implemented ATMD to a wind turbine to control in-
plane vibrations of blades [21].
In 2014, two identical ATMDs were applied to
the 90th story of The Shanghai World Financial
Center Tower by Lu et al. against wind loads [22].
Shariatmadar and Meshkat Razavi introduced an
active control procedure using both PSO and FLC
[23]. Soleymani and Khodadadi presented a multi-
objective methodology using GA and FLC in order
to mitigate dynamic vibrations due to earthquake
and wind loads. The method was tested on a
benchmark 76-story building in Australia,
Melbourne. However, the optimum design against
earthquake excitations was not adequate for the
reduction of wind-induced vibrations and vice versa
[24]. Considering similar building, the cuckoo
search (CS) algorithm was proposed to be involved
in the calculation process of active forces by Zabihi
Samani and Amini [25]. For the seismically excited
high-rise buildings, PD, PID and LQR controllers
were also examined. Under strong ground motions,
PD and PID had superior performance than LQR.
Additionally, PID was more effective in the
mitigation of structural responses than PD [26]. In
2018, Heidari et al. suggested the use of a hybrid
controller including LQR and PID controller to
attenuate seismic excited vibrations. In the design of
this hybrid controller, CS was employed [27]. Park
et al. developed a control procedure based on a
coupling type ATMD for adjacent buildings [28].
To improve seismic control of super-tall buildings,
Li and Cao proposed an inerter to integrate into the
ATMD system [29]. In the other study, an optimal
design methodology-based sliding mode control was
presented [30]. For the optimum tuning of ATMDs,
metaheuristic algorithms were also investigated [31-
35]. Also, these algorithms have been used in
various control systems [36-40].
As it is known, structural engineers perform
their structural designs under various material and
structural behavior presuppositions. However,
regardless of the complexity of the calculations and
the sophistication of the theory used, in any case,
the existing parameters of the structure may differ
from the values used in the design. Among the
reasons for these are that the structure cannot be
manufactured in accordance with the design
acceptances, or the behavior is not in accordance
with the acceptances, and it contains manufacturing
(workmanship) defects. These can be added to the
differences in the inhomogeneous behavior of
concrete-like materials that are frequently used in
buildings. All these situations may cause a risky
situation in terms of structural security.
In this study, unlike the studies in the literature,
the effect of uncertainties (differences) in the
structural parameters that will occur due to the
mentioned situations on the change of behavior of
an ATMD-controlled structure has been examined.
For this purpose, in an ATMD-controlled structure
designed under certain structural stiffnesses,
analyzes were made under eight different situations
according to the deviations that may occur due to
uncertainty in the floor stiffnesses. The analysis
results of all cases were examined in detail in terms
of the structure's behavior under earthquakes and
structural displacements.
2 Methodology
In this section, the formulations of multiple degrees
of freedom (MDOF) structure with an optimum
ATMD on the top are presented. The formulations
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are given of an ATMD using proportional derivative
integral (PID) type controllers that have optimum
mass (md,opt), stiffness (kd,opt), damping (cd,opt),
proportional gain (Kp,opt), derivative time (Td,opt) and
integral time (Ti,opt). The structure mass, stiffness
and damping coefficients are shown as mi, ki and ci,
respectively. i represent the story number. The
uncertainty percentage is shown as ur.
The equation of motion of structure is shown as
Eq. (1) where M, C and K are mass, damping and
stiffness, respectively. 󰇘󰇛󰇜 is the ground
acceleration. In this study, a set of far-fault ground
motions presented in FEMA P-695 [41] are used
and the results are presented for the most critical
excitation. F(t) represents the control force matrix
given as Eq. (2). x(t) (Eq.3) is the response matrix
including displacements of N story structure (xi to
xN) and ATMD (xd). M, K and C matrices are shown
as Eqs. (4)-(6). The control force (Fu) is calculated
via Eqs. (7)-(9). In these equations, Kf, iATMD, R, Ke,
u(t), td and e(t) are trust constant, armature coil,
resistance value, induced voltage constant of
armature coil, control signal, derivative time and
error signal, respectively.
󰇘󰇛󰇜󰇗󰇛󰇜󰇛󰇜-󰇝󰇞󰇘󰇛󰇜󰇛󰇜 (1)
u
u
0
0
F(t)
F
-F








(2)
d
N
2
1
x
x
x
x
)t(x
(3)
1
2
N
d,opt
m
m
.
.
M
.
m
m











(4)
(5)
1 2 2
2 2 3 3
N N d,opt d,opt
d,opt d,opt
(c c ) c
c (c c ) c
..
. . .
C
. . .
c (c c ) c
cc












(6)
ATMDfu iKF
(7)
ATMD e d N
Ri +K (x -x )=u(t-td)
(8)
p,opt d,opt
i,opt
de(t) 1
u(t) = K e(t)+T + e(t)dt
dt T




(9)
The presented equations of motions are modeled in
Matlab with Simulink [42] and the fourth-order
Runge-Kutta method was used for time-history
analysis by using the constant optimum ATMD
parameters and changing stiffness values of
structure.
3 Numerical Examples
In this section, the effect of story rigidity on the
structural responses is investigated. For that reason,
ten case analyzes are done for different story
rigidity. In the analysis, a ten-story shear building
with ATMD located to the top of the story is
considered.
In the analysis, the optimum ATMD parameters
that were previously founded by Jaya algorithm [35]
are taken. Afterward, to examine the effect of
stiffness uncertainties on the structural responses,
analyzes were repeated for ten different cases in
which the story stiffnesses is changed between -25%
and 25% by increasing 5% and the results were
compared. The cases are shown with ur values and
story stiffnesses are given in Table 1. The value
used in the optimization process was shown as
constant. The structure and ATMD properties that
are taken in the study are given in Table 2.
For each case, critical earthquakes records that
give the largest top story displacement among all
records were found and their structural results were
presented in Table 3.
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Table 1. Cases for different story rigidity
Case No
1
2
3
4
5
constant
6
7
8
9
10
ur (%)
-25
-20
-15
-10
-5
0
5
10
15
20
25
Rigidity coefficient
of each story
(MN/m)
487.5
520.0
552.5
585.0
617.5
650.0
682.5
715.0
747.5
780.0
812.5
Table 2. The story and ATMD properties
Symbol
Definition
Value
Unit
Story
properties
mi
Mass
360
ton
ki
Rigidity coefficient
520-780
MN/m
ci
Damping coefficient
6.2
MNs/m
Optimum
ATMD
parameters
md
Mass
180
ton
Tatmd
Period
0.8923
s
ξd
Damping ratio
28.5447
%
Kp
Proportional gain
-336.3929
Vs/m
Td
Derivative time
2003.7846
s
Ti
Integral time
-6549.9725
s
Constant
ATMD
parameters
stmax
Stroke limit
2
-
R
Resistance value
4.2
Kf
Trust constant
2
N/A
Ke
Induced voltage constant of armature coil
2
V
Table 3. The top story displacements () and accelerations (󰇘) for critical earthquakes
Case
no
Earthquake
record
 (m)
󰇘 (m/s2)
Earthquake
record
 (m)
󰇘 (m/s2)
1
NORTHR/MUL279
0.2773
9.5510
DUZCE/BOL090
0.2462
11.4665
2
NORTHR/MUL279
0.2741
10.4821
DUZCE/BOL090
0.2507
12.4897
3
NORTHR/MUL279
0.2687
11.3113
DUZCE/BOL090
0.2526
13.2650
4
NORTHR/MUL279
0.2614
12.0247
DUZCE/BOL090
0.2523
13.7751
5
NORTHR/MUL279
0.2528
12.8045
DUZCE/BOL090
0.2503
14.4433
opt
NORTHR/MUL279
0.2433
13.4350
DUZCE/BOL090
0.2469
14.8413
6
NORTHR/MUL279
0.2334
13.9121
DUZCE/BOL090
0.2421
15.0906
7
NORTHR/MUL279
0.2237
14.2290
DUZCE/BOL090
0.2365
15.4685
8
NORTHR/MUL279
0.2146
14.3782
DUZCE/BOL090
0.2308
15.6865
9
NORTHR/MUL279
0.2058
14.7806
DUZCE/BOL090
0.2249
16.0083
10
NORTHR/MUL279
0.1971
15.0252
DUZCE/BOL090
0.2187
16.6988
From the analysis results, it is understood that
critical earthquakes vary depending on the change in
stiffness values. The critical earthquakes given in
bold in the Table 3 are NORTHR/MUL279 record
for -25% - -5% stiffness, and DUZCE/BOL090
record for others. Considering the critical
earthquakes, the increase in stiffnesses led to a
decrease in the displacements whereas an increase
in the accelerations.
For the NORTH/MUL279 record, 9.69%
change in displacements, 34.06% in accelerations
(Case 1-5), and for DUZCE/BOL090 record 12.89%
change in displacements and 12.52% in
accelerations (Caseopt-Case10) were observed.
Examining each case for both critical
earthquakes, the difference between maximum
displacements was found to be 0.99% - 12.63%.
This difference was 8.47% - 20.05% for maximum
accelerations.
Also, for all cases accelerations decrease as
stiffness increases, and DUZCE/BOL090
earthquake caused greater story accelerations.
Time history plots of top story displacements
under critical earthquakes were also given in Fig 1
and 2 for 3 cases. From the figures, values and
location of peek points of graphs differ depending
on changing critical earthquakes, as expected.
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Fig. 1: Time history plots of top story displacements under NORTHR/MUL279 record.
Fig. 2: Time history plots of top story displacements under DUZCE/BOL090 record.
4 Conclusion
Uncertainties in stiffness can be caused by many
reasons such as design assumptions, differences in
the behavior of the material (especially using non-
homogeneous materials such as concrete) or
manufacturing errors. Depending on the quality of
the control process during the construction of the
structure, these uncertainties can be minimized, but
it is not possible to completely eliminate.
For that reason, in this study, the performance,
efficiency and robustness of the ATMD design, of
which parameters are obtained under ideal
conditions, in case of such uncertainties in the
structural system are examined. Therefore 11 case
analyzes are performed in which the story stiffness
is changed between -25% and +25% with %5
increment. In the analyses, optimum ATMD
parameters proposed by Kayabekir et al. [35] are
considered and assumed to be constant in all cases.
The analysis results show that uncertainties in
the structural stiffness can be an effect on ATMD
performance. Since the design of ATMD is done
based on structural stiffness, the effect of these
uncertainties on structural behavior is an expected
situation as can be also seen from Fig. 1 and 2. The
critical earthquake may change due to variation of
structural stiffness. Depending on changing critical
earthquakes, the peak values of the structural
responses and timing of the peak values can differ.
These differences for the peak values of the story
displacements are between 0.99% and 12.63%. For
the peak values of story accelerations, 8.47% -
20.05% difference was observed.
In addition, the maximum displacements of the
uncontrolled system are found 0.4101 m (DUZCE/
BOL090) and 0.4363 m (NORTHR/MUL279) for
critical earthquake records. These displacements are
reduced to 0.2469 (DUZCE/BOL090) and 0.2433 m
(NORTHR/ MUL279) by the addition of ATMD to
the structure. In this case, it can be said that the
ATMD design is efficient and reliable even under
stiffness uncertainties.
For future studies, these uncertainties are
investigated on different models.
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Contribution of Individual Authors to the
Creation of a Scientific Article (Ghostwriting
Policy)
Aylin Ece Kayabekir, Gebrail Bekdaş and Sinan
Melih Nigdeli generated the analysis code.
Aylin Ece Kayabekir done the analysis and drew the
figures.
The text of the paper was composed by Aylin Ece
Kayabekir, Gebrail Bekdaş and Sinan Melih
Nigdeli.
Creative Commons Attribution License 4.0
(Attribution 4.0 International, CC BY 4.0)
This article is published under the terms of the
Creative Commons Attribution License 4.0
https://creativecommons.org/licenses/by/4.0/deed.en
_US
WSEAS TRANSACTIONS on SYSTEMS
DOI: 10.37394/23202.2022.21.3
Ayli
n Ece Kayabeki
r,
Gebrai
l Bekdaş, Si
nan Meli
h Ni
gdeli
E-ISSN: 2224-2678
38
Volume 21, 2022