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1 (2012)
                                 PAGES 97-112
                                      M.R. Tabeshpour*
          Faculty of Engineering, Sabzevar Tarbiat Moallem University, Sabzevar, Iran
                      Received: 5 September 2010, Accepted: 5 July 2011
ABSTRACT
1. INTRODUCTION
Some special structures such as high-rise towers and power plant chimneys and their
equipments and/or in-charge facilities are often considered to be fully functional after even
very strong ground motions. Consequently, seismic assessment for actual performance of
structures during earthquakes, the nonlinear dynamic analysis is required. Then the damage
*
    E-mail address of the corresponding author: tabesh_mreza@yahoo.com (M.R. Tabeshpour)
98                                      M.R. Tabeshpour
indices of structure have to be calculated, using appropriate damage models since these
indices could be numerical representation of damage states of the structures. However,
numerical modeling of such mega-structures with numerous elements may not be allowed to
include all details of mechanical characteristics of consisting materials, particularly
nonlinear performance of elements during large deformations. Therefore, a simplified model
corresponding to dynamic characteristics of whole structure is substantially needed to
investigate seismic performance and failure modes of these essential structures subjected to
strong ground motions.
   In this paper a practical method to assessment chimney like towers such as smoke stacks,
minarates and TV towers is presented based on nonlinear dynamic analysis considering
appropriate hysteretic behavior of section and material properties. Damage analysis is
presented as well. Such an analysis is required for fragility curve of the structure. Many
nonlinear dynamic analyses are required for fragility cures. Only using simple reliable
macro (beam-column element) model can achieve such a goal. Some examples of damaged
towers in previous earthquakes show the necessity of the nonlinear dynamic analysis of
these types of structures.
    The investigation is focused on the dynamic response of the stack due to an earthquake
motion recorded at a nearby site. Gould et al. [3] and Huang and Gould [4] presented
interesting results of analysis of the Tüpras stack. They presented nonlinear static analysis
of the collapsed stack using a demand-collapse comparison. The demand was represented by
an acceleration-displacement response spectrum based on the recorded motion as well as
some smoothed adaptations typical of design spectra, while the capacities were calculated
from pushover curves using a nonlinear reinforced concrete finite element analysis. The
results confirm that the stack could readily fail under the considered earthquake and were
also consistent with the debris pattern. Pushover results shown in Figure 4 are cracking
patterns for the model with and without opening in a step. Of course, a full nonlinear
100                                    M.R. Tabeshpour
Figure 4. Cracking pattern for the model with and without opening [3]
interaction is considered negligible. When this effect is taken into account, the use is
commonly made of a sway rocking model for the structures with spread or short-pile
foundation. The SSI effect on the structure as well as piles, however, is considered
significant in case of long piles in soft ground. In such a case, some coupled system should
be adopted for the seismic design model. A finite element model would be powerful in
evaluating the SSI effect if it were linear. Also as a simple model a lumped mass-spring-
beam model can be considered appropriate for taking into account the major SSI effect as
well as the material non-linearity in the structure and the ground [6]. Figure 6 shows the
models mentioned above. Halabian and Kabiri have investigated the effect of soil structure
interaction on the response of stack like structures [7].
    In this paper, an exclusive review of relevant modeling and methodology for estimation
of damage indices in special RC structures has been carried out. A procedure for developing
a 2-D simplified nonlinear model based on moment-curvature in some plane-sections of a 3-
D sophisticated model but linear system having almost identical dynamic properties is
developed.
    The significance of this study, if any, is mainly concentrated on model simplification that
provides sufficient accuracy based on a nonlinear discrete model. Damage indices under
different hazard levels of excitations provide the database for vulnerability and seismic risk
analyses for the both elements and whole of structures. For instance, from relative
displacement responses of nonlinear model, one may estimate the most probable modes of
failure under MCE level of input excitation.
    As noted above, the damage indices of structure have to be calculated, using appropriate
damage models. It is because of the fact that damage indices are quantitative values for damage
states of the structures. These models are usually based on the maximum deformations,
hysteretic energies and structural deteriorations. Damage indices are appropriate tools for
quantifying numerically the damage in structures sustained under earthquake loading. Many
researchers have defined various damage indices. Damage indices may be defined locally for
102                                      M.R. Tabeshpour
elements or globally for whole the structure. An extensive review of defined damage indices
for various types of structures has been carried out [9-10]. Vulnerability of an existing
structure based on seismic hazard analysis has been assessed [11].
    Park-Ang damage index [12], considered in IDARC [13], is the most usual damage index
for damage analysis of reinforced concrete structures. It can be calculated in the element,
storey and overall scales. An important point is that the damage indices of stories are
calculated based on hysteretic energy weighting factors and therefore the structural
importance of beams and columns are the same. Also overall damage index of structure is
calculated by summation of the storey damage indices on the basis of hysteretic energy of
each storey.
    Seismic vulnerability and damage analysis of special structures have been carried out
successfully using IDARC program [14-15]. The key idea of structural modeling of the
special structures is to develop a simplified 2-D model using beam-column elements based
on moment-curvature in some plane sections. Appropriate results have been achieved by
nonlinear dynamic analysis of these simplified models.
    Some special structures such as high rise towers are often analyzed elastically using shell
or solid elements, ignoring the effect of nonlinear properties. But it is clear that in order to
understand the actual behavior of the structure, nonlinear dynamic analysis must be carried
out. To investigate the structural behavior of towers under future earthquakes, the structure
should be modeled as a way to perform the seismic behavior properly. The structural
modeling can be carried out using various types of elements. Among these elements beam-
column element is an appropriate type considering both the complexity of the structural
performance and the time consuming of the analyses.
    In this paper the seismic performance of Tous power-plant chimney, which is located in a
seismically active zone, has been evaluated.
2. STRUCTURAL MODELING
As mentioned earlier, it is possible to model the structure using various types of elements.
But it is clear that nonlinear dynamic analysis of structure is required for seismic
vulnerability. It is possible to use various types off elements to model high rise cantilever
type towers. The beam-column element is the most appropriate method for structural
modeling, because of limitations in the computation time. Figure 7 shows the discrete model
of the structure using lumped mass and beam-column elements. Beam-column elements are
modeled considering flexural, shear and axial deformations. Flexural and shear components
of the deformation are modeled using three parameter Park model described later. The axial
deformation component is modeled using a linear-elastic spring.
             NONLINEAR DYNAMIC ANALYSIS OF CHIMNEY-LIKE TOWERS                             103
Softening of the concrete under deformation near its limit state of resistance is an important
property that must be considered in nonlinear dynamic analysis. The moment–curvature
relation method is one of the specialty approaches used to express the real behavior of
concrete structures when deformed. This method could widely serve all general cross-
sectional shapes that may be used as different geometric cross-sections in towers. The
longitudinal concrete stresses can be found from the longitudinal concrete strains by using
the appropriate concrete stress–strain relationship in compression. Figure 8 shows the
relation between stress and strain for steel and concrete materials.
                       (a)                                              (b)
               Figure 8. Stress – strain relationship for steel (a) and concrete (b)
   Assuming that there is appropriate reinforcement such that the collapse of the tower will
be due to crushing of concrete in primary stress arising from axial load and flexure, it can be
used from the moment - curvature diagram in order to damage analysis.
104                                         M.R. Tabeshpour
4. PUSHOVER ANALYSIS
The nonlinear pushover analysis, or collapse mode analysis, is a simple and efficient
technique to predict the seismic response of prior to a full dynamic analysis. A pushover
analysis can establish the sequence of component yielding, the potential ductility capacity,
and the adequacy of the lateral strength of the structures. The pushover analysis option
performs an incremental analysis of the structure subjected to a distribution of lateral forces.
   The pushover analysis may be carried out using force control or displacement control. In
the former option, the structure is subjected to an incremental distribution of lateral forces
and the incremental displacements are then calculated. In the latter option, the structure is
subjected to a displacement profile, and the lateral forces that needed to generate the
deformation are calculated. Typically, since the deformed profile is not known, and an
estimate of the lateral distribution of forces can be made, force control is commonly used.
For displacement control, the user must specify the target maximum deformation profile of
the structure. This profile is internally divided by the number of steps specified by the user,
and then incrementally applied to the structure. In the force control option the user must
specify the maximum force distribution, or select one of the force distributions available in
the program: Uniform Distribution, Inverted Triangular Distribution, Generalized Power
Distribution Modal Adaptive Distribution.
   The generalized power distribution was introduced to consider different variation of the
storey accelerations with the storey elevation. This distribution was introduced to capture
different modes of deformation, and the influence of higher modes in the response. The
force increment at floor “i” is calculated according to:
                                                   Wi hik
                                        Fi      N
                                                                    Vb                     (1)
                                                  
                                                  j 1
                                                         W j h kj
where Wi and hi are the storey weight and the storey elevation, respectively, and Vb is the
increment of the building base shear and k is the parameter that controls the shape of the
force distribution. The recommended value for k may be calculated as a function of the
fundamental period of the structure (T):
                              k  1.0                           for        T  0.5        (2a)
                                        T  0.5
                            k  1.0                                      otherwise       (2c)
                                           2
The nonlinear dynamic analysis is carried out using a combination of the Newmark-Beta
                NONLINEAR DYNAMIC ANALYSIS OF CHIMNEY-LIKE TOWERS                         105
integration method, and the pseudo-force method. The viscous damping matrix is calculated
in the program using one of the following options: Mass or Stiffness proportional damping
and Rayleigh damping. In the program IDARC the circular frequency corresponding to the
first mode of vibration is used for the mass and stiffness proportional damping, while the
circular frequencies corresponding to the first and second modes are used for the Rayleigh
damping type. Under these conditions, mass proportional damping will yield a smaller
damping ratio for the higher modes, while stiffness proportional and Rayleigh damping may
result in a higher critical damping ratio for the higher modes.
    Modeling the hysteretic behavior of structural elements is one of the core aspects of a
nonlinear structural analysis program. The three parameter Park hysteretic model is as part
of the original release of IDARC. The hysteretic model incorporates stiffness degradation,
strength deterioration, non-symmetric response, slip-lock, and a trilinear monotonic
envelope. The model traces the hysteretic behavior of an element as it changes from one
linear stage to another, depending on the historey of deformations. The model is therefore
piece-wise linear. Each linear stage is referred to as a branch. Figures 9 shows the effect of
various parameters on the shape of the hysteretic loops.
6. DAMAGE ANALYSIS
In order to damage analysis, it is necessary to quantify the structural damage and therefore
damage index must be defined. Many damage indices have been defined. The most usual
damage index is the Park-Ang model. It is defined as combination of maximum deformation
and hysteretic energy [12]:
                                               
                                          u  u Py 
                                    DI  m           dE h                              (3)
 dE   h   is the hysteretic energy absorbed by the element during the earthquake, Py is the
yield strength of the element. Park-Ang damage model can be extended to the storey and
overall scales. Park-Ang damage indices for various damage states are shown in Table 1.
7. CASE STUDY
The chimney has cylindrical shape with 100m height, and external diameter of 10 meter.
The cylindrical shell thickness is 80cm from base to the elevation of 17.5m and then it is
reduced to 30cm in upper part. The schematic view of the chimney has been presented in
Figure 10.
    Seismic hazard analysis has been performed to determine the peak ground acceleration
(PGA) in both case studies. For instance for return periods of 75, 500, 1000 and 2500 years
at the site of chimney, PGA values resulted in 0.13, 0.26, 0.33, and 0.43g, respectively.
    In order to determine the periods and the effects of different modes of the structure,
eigenvalue analysis must be performed. For the studied chimney the periods of the first three
modes associated to 1.67, 0.30 and 0.11 sec, respectively. It is important to note that the
mode shapes and frequencies of the structure were measured using Ambient Vibration
Survey (AVS) [16]. The first and second frequencies resulted in 1.48 and 0.29 sec
             NONLINEAR DYNAMIC ANALYSIS OF CHIMNEY-LIKE TOWERS                             107
respectively. The third mode of AVS test has been associated to the torsional mode, and
therefore it is not comparable with numerical results. Figure 11 shows the flexural mode
shapes. It is clear from the first mode that the considered power distribution of lateral force
is appropriate for pushover analysis.
   The results of the pushover analyses for various types of lateral force have been
presented in Figure 12. As shown in this Figure, the uniform distribution of lateral load
gives the maximum base shear. Also the base shear of the triangle distribution is more than
that of the power distribution for the power factors equal to 1.5, 1.625 and 2 that are
corresponding to the periods of 1.5, 1.75 and 2.5 sec, respectively. Note that the
fundamental period of the structure is 1.67 sec. It is seen that the ultimate strength of the
structure is approximately 19% of weight.
   For all kinds of distribution proposed for lateral loads, the mechanism is similar to Figure
13, in which the plastic hinge occurs in the elevation 17.5m, the section that thickness
changes sharply.
Nonlinear dynamic analysis has been performed under the input motions shown in Figure 14.
   Nonlinear dynamic analysis has been performed under the input motions shown in Figure
14. Time history responses at top of the structure for input motion scaled to PGA level of 75
years return period are given in Figure 15.
             NONLINEAR DYNAMIC ANALYSIS OF CHIMNEY-LIKE TOWERS                               109
Figure 15. Time history responses at top of the structure for input motion scaled to PGA level of
                                     75 years return period
   The effect of input motion is observed clearly. Overall drift of the structure for PGA
values of 0.1g-0.6g has been shown in Figure 16. It is seen that for PGAs less than 0.3g,
there is no considerable difference among the responses of various input motions, but for
PGAs greater than 0.3g, the input motion characteristic has a strong influence on the
response of the structure.
110                                    M.R. Tabeshpour
   Global damage index of the structure for PGA values of 0.1-0.6g has been shown in
Figure 17. It is observed that for PGAs greater than 0.2g, the input motion has an obvious
influence on the damage of the structure. Also for PGAs greater than 0.6g structural collapse
may occur under some records consisting of low frequency content.
8. CONCLUSIONS
The nonlinear dynamic analysis is essentially needed for seismic assessment in evaluation of
actual performance of complicated structures during earthquakes. Then the damage indices
of structure had to be calculated, using appropriate damage models, since these indices
would be numerical representation of damage states of the structures. However, numerical
modeling of such mega-structures with numerous elements would not be allowed to include
all details of mechanical characteristics of consisting materials, particularly in large
deformations. Therefore, a simplified model corresponding to dynamic characteristics of
whole structure was developed to investigate seismic performance and failure modes of
these essential structures subjected to strong ground motions. The simplified model provided
sufficient accuracy based on a nonlinear discrete model. To verify the proposed modeling
procedure, two case studies were investigated numerically. Acceleration time histories
scaled to different hazard levels were used as input excitations. Among the results,
distribution of damage indexes could verify the most probable mode of failure under the
severe excitation.
REFERENCES