CHAPTER 5 New Trends in Earthquake Engineering. Passive and Active Control Structural control for civil engineering appeared as a necessity imposed by special, longer, or taller constructions spread allover the world. The passive approach was adopted already in many cases. For active control there are experiments showing good results. Hybrid solutions are under investigations by many researchers. However, the field is very large and civil engineer designers do not have a clear image of this scope. This chapter is showing the aim of structural control. It follows a short image of passive control and it is then stressing on active control. Theoretical aspects, devices used, and practical applications of active control are presented. A critical comparison between the two types of structural control is intended to introduce the reader into the complexity of the problems involved by the control implementations. Computational means helping the study of the field are also reviewed.
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CHAPTER 5
New Trends in Earthquake Engineering.
Passive and Active Control
Structural control for civil engineering appeared as a necessity imposed by special,
longer, or taller constructions spread allover the world. The passive approach was
adopted already in many cases. For active control there are experiments showing
good results. Hybrid solutions are under investigations by many researchers.
However, the field is very large and civil engineer designers do not have a
clear image of this scope.
This chapter is showing the aim of structural control. It follows a short image
of passive control and it is then stressing on active control. Theoretical aspects,
devices used, and practical applications of active control are presented.
A critical comparison between the two types of structural control is intended
to introduce the reader into the complexity of the problems involved by the control
implementations. Computational means helping the study of the field are also
reviewed.
5.1 INTRODUCTION
The Civil Engineering field is now undergoing important changes in philosophy and
practice due to dramatic evolution recorded in other branches of human activity like:
electronics, automatics, computer science, robotics, new materials and technologies,
etc. At the same time, it should be mentioned major differences between Civil
Engineering and other engineering fields.
It is specific for constructions to use materials with high costs, on large
surfaces and volumes, and to need huge energy during construction, especially in the
case of long span bridges and very tall buildings.
Life of many people and vital social activities depend on the well functioning
of civil structures during and after important earth shakings. There are also civil
engineering structures with inestimable material and spiritual values, as historical
buildings.
NATURAL ACTIONS STRUCTURES
PROTECTION
Passive Control
Active Control
Typhoons
Earthquakes
Tall
Buildings
Long Span
Bridges0 10 20 30 40 50 60
-800
-600
-400
-200
0
200
400
600KOBE NS 1995
818 gal
acce
lera
tion
(ga
l)
time (s)
Figure 5.1 Relation between actions, structures, and control
Protection of some structures as those reminded above is a very important problem for
human communities. A solution for avoiding the harming effects of strong
earthquakes or strong winds is the structural control. It is using specific means and
procedures that lead to reduction in intensities for actions and change the way they act
on civil engineering structures. It changes also the structural response to the actions
and lowers the induced energy. In Figure 5.1, the existing relation between natural
actions, structural control, and built constructions is shown. This figure highlights the
reduction in the input due to control means.
5.2 SEISMIC RESPONSE CONTROL
In order to determine the ways to control the structures acted by seismic forces, the
equation of energy balance may be written
E E E E Ek s h d (5.1)
where: E is the energy induced by seismic shaking; Ek is the kinetic energy; Es is the
elastic strain energy; Eh is the energy dissipated by the structural system due to
inelastic behavior or other causes; Ed is the energy dissipated by supplemental
damping devices.
From Equation (5.1) it can be deduced that the control means play the role of
taking a part of the energy induced into the structure. However, it should be observed
that there is a dependency between the structural characteristics, e.g. the natural
period of vibration, and the amount of induced seismic energy. Therefore, the seismic
behavior of civil engineering structures is very complex in its nature and its
complexity is amplified through the presence of control means, which are actually
modifying the structural characteristics.
There are many ways to accomplish a seismic response control. According to
Professor Kobori, these ways are:
1. Cut off the energy transmission of the earthquake ground motion to a
structure.
2. Isolate the natural period of the structure from the predominant frequency
domain of the ground motion.
3. Achieve the non-stationary and non-resonant state by providing nonlinear
characteristics.
4. Apply control force such as mass damper/driver or tendon.
5. Utilize the energy absorption mechanism.
If the first method is achievable, then the second and the fifth method are not needed.
However, the first method is difficult to achieve, therefore it is recommended that at
least two of the above methods to be combined.
Table 5.1 Classification of structural protective systems
Seismic
Isolation
Passive Energy
Dissipation
Active
Control
Elastomeric bearings Metallic dampers Active bracing systems
Lead rubber bearings Friction dampers Active mass dampers
Elastomeric bearings with energy
dissipating devices
Viscoelastic dampers Active variable stiffness or
damping systems
Sliding friction pendulum Viscous dampers Pulse systems
Flat sliding bearings with restoring
force devices
Tuned mass dampers Electro-rheological active
dampers
Lubricated sliding bearings with
energy dissipating devices
Tuned liquid dampers Aerodynamic appendages
Table 5.1 shows a classification of protective systems. It provides a part of the many
control devices existing now. Depending on the location of the control devices other
classification can be stated:
a) protective devices located into the structure
b) protective devices located at the base of the structure
c) combination of a) and b).
Each of the above can be either passive or active.
The passive control is based on the nature of the materials they include
(rubber, lead, steel, viscous materials) and especially on supplementary adding in
damping and ductility. Some of passive devices rely on the use of friction forces.
The active control is using external energy for reducing, even minimizing the
seismic response. The controlled structure becomes active, with different
characteristics and different behavior compared to the initial non-controlled one, even
in case of strong actions.
5.3 PASSIVE CONTROL. DEVICES AND PRACTICAL APPLICATIONS
Passive controlled structures are widely spread all over the world. Table 4.3, at the
end of this chapter presents a list of isolated structures and isolation devices used in
different countries.
Also at the end of the chapter there is the Table 4.4 showing some passive
devices used in Japan for seismic isolation of bridges. These devices are the objects of
specifications in a design guide named “Menshin”. Other developed countries try to
setup similar specifications.
Top steel plate
Steel plates
Rubber
Holes for bolts
Bottom steel plate
Figure 5.2 Elastomeric bearing
A rubber bearing with top and bottom steel plates is presented in Figure 5.2. Other
type is that from Figure 5.3. It contains steel plates integrated in rubber. These plates
have the role to limit lateral displacements. The system includes a lead kernel, which
can assure an increased ductility, but it can determine permanent displacements after
strong earthquakes. However, the lead core can be replaced when needed.
Dowel holes
Lead plug
Rubber
Steel plates
End steel plates
Figure 5.3 Lead-rubber bearing
The passive means devices range is considerable large. One important type, named
Tuned Mass Damper (TMD) is based on moving masses. Figure 5.8 shows an Active
Mass Damper. If the active part (the actuator which generates the force ua) is
removed, a TMD is obtained. Such systems determine changes in structural dynamic
characteristics. Especially the frequency response function is lowered if the dynamic
properties of the TMD are close to that of the main structure and if the mass of the
TMD is enough large (between 1% to 4% from the mass of the main system).
In a similar manner is acting a TLD, Tuned Liquid Damper. One TLD is
shown at the fourth level of the structure from Figure 5.9. The mass value, the natural
period of vibration, and the liquid viscosity are the main elements that make the
system to be efficient.
Articulated slider
Supporting
column
Bearing material
Spherical surface
Cylinder
Seal
Figure 5.4 Friction Pendulum System Bearing
Figure 5.4 presents other passive control system based on a sliding bearing moving on
a spherical surface. An important advantage of this device type is that it can assure a
return to the initial position under the structure’s weight.
5.4 ACTIVE CONTROL. THEORETICAL ASPECTS
Every construction suffers changes during its life. At the same time, the environment
where the structure is placed is changing, too. Therefore one could compare existing
constructions to living beings. However, the most common way a civil engineering
structure overcomes external loads is to resist to them. The living beings not only
resist but also adapt to the environmental aggressiveness, responding in a different
manner to different actions or intensities. Adapting to external loads and to structural
changes is a basic idea in active structural control.
In 1972, Prof. James T.P. Yao, through his paper “Concept of Structural
Control”, is defining the start for this new branch in structural synthesis. Figure 5.5
shows a feedback system as J.P.Yao viewed it. The author describes a structural
controlled structure as an error-activated structural system the behavior which varies
automatically in accordance with unpredictable variations in the loading as well as
environmental conditions and thereby produces desirable responses under all possible
loading conditions.
From the point of view of theoretical studies and application methodologies,
there are two main approaches in structural control:
i. LQG (Linear Quadratic Gain) control, based on time domain
ii. H and -Synthesis control, based on frequency domain.
These two ways are very developed in many sub-methods and versions. Meanwhile,
additional tools are added to the main methods: fuzzy sets analysis and neuronal
networks.
Input, r variable, c
Control
Actuating signal, e
Error or
Forward Path Elements
- error sensing device
- compensating network
- amplifier
- servo-motor-
+
Feedback
Path
Elements
Command or
Reference
Figure 5.5 Closed-Loop Control System
From the first category of control, LQG, very popular are: pole assignment, optimal
control, instantaneous optimal control, modal control, critical modal control, and
sliding modes control method.
Majority of these methods is based on rewriting the structural dynamics
classical and familiar system of equations
M z + C z + K z = fs s s (5.2)
in the form of state equation
x = Ax + Bf
y = Cx + Df (5.3)
In the Equation (5.2), Ms, Cs, and Ks are the mass, damping, and stiffness matrices of
the structure; z is the vector of the generalized displacement vector, and f is the vector
of the external forces.
A
C B+
+ xf x
+
+ y
D
Figure 5.6 System described by Equation (5.3)
In the Equation (5.3), A is the system matrix, B is the load location matrix, C is the
measurement matrix, and D is a matrix showing the influence of the input, f, to the
output, y. Equation (5.3) is described by Figure 5.6.
If all the states, x, are known (measured), a state feedback, u, can be
introduced, and the control problem is reduced to finding a gain matrix, K, so that:
x = Ax + B(f - u)
u = Kx (5.4)
and a graphical representation of the Equation (5.4) is given by Figure 5.7.
A
Bx
u
f x
+
+
-
+
K
Figure 5.7 System described by Equation (5.4)
As an example of control method, the optimal control method is presented next. For
this case, the objective is to determine the gain matrix, K, under the condition that a
quadratic index, J, defined by Equation (5.5) should be minimized.
J dtt f
x Qx u Ru0
(5.5)
In the Equation (5.5), Q and R are weighting matrices representing the importance
given to reducing the structural response and the importance given to use less external
energy for obtaining the control, respectively.
This method leads to a Riccati matrical equation
PA PBR B P A P 2Q 011
2 (5.6)
with the matrix P being unknown. After solving, the gain matrix is obtained from the
next equation:
K R B P11
2 (5.7)
Replacing the control force vector, u, into Equation (5.4) one could observe that the
feedback system is transforming the original uncontrolled system by changing the
system matrix A, such that it will respond to the requirements of Equation (5.5).
m2
k1
c1
ua
k2
c2
m1
x x x 2 2 2
x x x 1 1 1
xg
Figure 5.8 Active Tuned Mass Damper
5.5 ACTIVE CONTROL. DEVICES
In structural active control various devices are used. Between them, Active Tuned
Mass Dampers (ATMDs) are widely used and studied. A system with one degree of
freedom equipped with an ATMD is shown in Figure 5.8. It can be seen from this
figure that an ATMD is formed from an additional mobile mass attached to the system
through an actuator, generating the force ua. The active forces values are generated
from the on-line measurements and employing control algorithms.
In Figure 5.8 additional springs and dampers, tuned to dynamic characteristics
of the structure, link the main system and the secondary one. This control system is
also called Hybrid Mass Damper (HMD) because it can be seen as a combination
from a pure active system Active Mass Damper (AMD), and the elements of a passive
Tuned Mass Damper (TMD).
m Active Tuned Mass
Damper, ATMD
Tuned Liquid
Damper, TLD
Active Braces
System, ABS
Active Variable
Stiffness, AVS
Active Tendon
System, ATS
Active/passive base
isolation systems
Figure 5.9 Use of some structural control systems
In order to have a better look about passive and active control systems, Figure 5.9
shows some of them located on a building. The figure is only a representation, not a
true solution, because employing many device types in the same building is not
common. Usually, real applications involve only one type of control system.
However, for hybrid applications, the base isolation is utilized together with some
active devices.
At the top of the building from Figure 5.9 one can observe an ATMD device
and one floor lower, a Tuned Liquid Damper (TLD). At the third floor, there is an
Active Brace System (ABS) which is principally made from a piston and a servo-
valve acting on the diagonal of that floor.
The system from the second floor of the building from Figure 5.9 is named
Active Variable Stiffness (AVS) and was introduced by Professor Takuji Kobori and
Kajima Corporation of Japan. It is made from two very stiff inclined beams moved to
the left or to the right by the upper active piston and therefore minimizing the relative
floor displacement and changing the floor stiffness.
The first floor from the building in Figure 5.9 is equipped with an Active
Tendon System (ATS). This system is based on active diagonals consisting in tendons
having the role to provide the limitation of relative floor displacements.
At the base of the building from Figure 5.9 passive isolators are installed. In
order to prevent too long displacements of the building’s base, an actuator and,
eventually, a spring and a damper are employed. For the base actuators, the problem
of generating huge forces could be prohibitive.
Table 5.2 Buildings with structural active control in Japan
Active Control System's
Name
Developer Building's Name Year
AMD (Active Mass Driver) Kajima Kyobashi Seiwa Bldg. 1989