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Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications
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ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42
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Seismic Response of Non-Structural Element Placed on Single
Story Two-Way Asymmetric Building under Bi-Directional
Excitations
Pinkesh M. Dalal 1
, Snehal V. Mevada2
, Sumant B. Patel3
1
P.G. Student,2
Assistant Professor,3
Associate Professor,
1-2-3
Structural Engineering Department, Birla Vishvakarma Mahavidyalaya [Engineering College], Vallabh
Vidyanagar, Gujarat, India.
Abstract:
The seismic response of non-structural element placed on single-storey, two-way asymmetric building under
bi-directional excitations is investigated. The response is obtained by numerically solving the governing
equations of motion. The seismic response of the system and non-structural element is obtained by numerically
solving the equations of motion using state-space method under different system parameters. The comparative
performance is investigated of non-structural element placed at different places on single story asymmetric
building and finding a best place for survival during earthquake. It is found that non-structural element at
flexible edge along Y- direction gives less response of displacement and acceleration. So, non-structural
element placed at flexible edge along Y- direction on asymmetric SDOF system performs better in earthquake
than at other places.
Keywords: Seismic, Bi-Direction Excitation, Non-Structural Elements, Displacement, Acceleration.
I. INTRODUCTION
Non-structural elements (NSEs) of a building
are not a part of the main load-resisting system.
Murty and Goswami (2005) found that the damage
costs of Non-Structural Elements (NSEs) may
account for 65% to 85% of the total construction cost
of commercial buildings. Vijayanarayanan et al.
(2012) found that in critical facilities, building has
losses due to damaging equipment and inventory can
be two to three times greater than the cost of
replacing collapsed buildings or structures.
Classification of Non-Structural Elements
1) Architectural Components: This category
includes the elevator penthouses, stairways,
partitions, parapets, and heliports, cladding
systems, signboards, lighting systems and
suspended ceilings.
2) Mechanical and Electrical Equipment: This
category includes the storage tanks, pressure
vessels, piping systems, ducts, escalators,
smokestacks, antennas, cranes, radars and object
tracking devices, computer and data acquisition
systems, control panels, transformers,
switchgears, emergency power systems, fire
protection systems, boilers, heat exchangers,
chillers, cooling towers and machinery such as
pumps, turbines, generators, engines and motors.
3) Building Contents and Inventory: This category
includes the masonry wall, door, window, stair,
Bookshelves, file cabinets, storage racks,
decorative items and any other piece of furniture
commonly found in office buildings and
warehouses (Mondal and Jain, 2005)
In the past, many researchers investigated
and studied about the behaviour of NSEs. Adam and
fotiu (1997) investigated numerically the effect of
ductile material behaviour on the response of
coupled primary-secondary systems by using linear
and nonlinear floor response spectra.
Villaverde(1997)determined simple way equivalent
static lateral forces for the seismic design of NSE
attached to primary structure. Mondal and Jain
(2005) provide design philosophy and design
provision of international seismic code, and
recommended design lateral forces. Singh et
al.(2006)calculated and compared the seismic
design force for flexible non-structural component
by using floor response spectra. Chaudhuri and
Villaverde(2008) investigated the seismic response
of NSE which are attached to steel moment resisting
frames and series of linear and nonlinear SDOF by
using ensemble of 25 recorded earthquake ground
motion and influence of the NSE location,
nonlinearity and damping ratio. Dhanani et al.(2013)
investigated the seismic response of NSE by using
time history analysis, NSE placed on various floor at
RESEARCH ARTICLE OPEN ACCESS
Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications
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ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42
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various place of three story asymmetric building and
analysis has been perform to obtain the displacement
and acceleration of NSE. Although, some of the
work has been done to investigate the seismic
response of NSE. However, no work has been
reported to obtain the optimum location of NSE
when NSEs placed on asymmetric building under bi-
direction excitation. The objectives of the study are
summarized as: (i) to perform the time history
analysis to find the acceleration and displacement
for NSEs placed at various locations on single story
two-way asymmetric building, (ii) to determine the
best suitable location for non-structural elements on
single story two-way asymmetric buildings.
II. STRUCTURAL MODEL AND
SOLUTION OF EQUATIONS OF
MOTION
The system considered is an idealized single-
storey building which consists of a rigid deck
supported on columns as shown in Fig. 1. Following
assumptions are made for the structural system
under consideration: (i) floor of the superstructure is
assumed as rigid, (ii) force–deformation behaviour
of the superstructure is considered as linear and
within elastic range (iii) the structure is excited by
bi-directional horizontal component of earthquake
ground motion and the vertical component of
earthquake motion is neglected, and (iv) mass of the
columns is ignored and the columns are considered
to only provide lateral stiffness. The mass of deck is
assumed to be uniformly distributed and hence
centre of mass (CM) coincides with the geometrical
centre of the deck. The stiffness asymmetry with
respect to the CM in two direction and hence, the
centre of rigidity (CR) is located at an eccentric
distance, ex from CM in x-direction and ey from CM
in y-direction. The system is asymmetric and
therefore, three degrees of freedom are considered
for model namely the lateral displacement in x-
direction, ux lateral displacement in y-direction, uy
and torsional displacement, uθ as represented in Fig.
1. The governing equations of motion of the building
with lateral and torsional degrees of freedom of the
system are obtained in the matrix form are expressed
as:
𝑀𝑢̈ + 𝐶𝑢̇ + 𝐾𝑢 = −𝑀𝑢 𝑔̈ …(1)
where, M, C and K are the mass, damping and
stiffness matrices of the system, respectively; 𝑢 =
{ 𝑢 𝑥 𝑢 𝑦 𝑢 𝜃}T
is the displacement vector; 𝑢̈ 𝑔 =
{ 𝑢̈ 𝑔𝑥 𝑢̈ 𝑔𝑦 0}T
is the ground acceleration vector;
and𝑢̈ 𝑔𝑥 and 𝑢̈ 𝑔𝑦is the ground acceleration in x and
y-direction respectively.
The mass matrix can be expressed as:
𝑀 = [
𝑚 0 0
0 𝑚 0
0 0 𝑚𝑟2
] …(2)
where, m represents the lumped mass of the deck;
and r is the mass radius of gyration about the vertical
axis through CM which is given by,
𝑟 = √(𝑏2 + 𝑑2)/12; where b and d are the plan
dimensions of the building.
The stiffness matrix of the system is obtained
as follows:
𝐾 = [
𝑘 𝑥𝑥 𝑘 𝑥𝑦 𝑘 𝑥𝜃
𝑘 𝑦𝑥 𝑘 𝑦𝑦 𝑘 𝑦𝜃
𝑘 𝜃𝑥 𝑘 𝜃𝑦 𝑘 𝜃𝜃
] …(3)
Where
𝑘 𝑥𝑥= 𝐾1 + 𝐾2 + 𝐾3+ 𝐾4,
𝑘 𝑦𝑦= 𝐾1 + 𝐾2 + 𝐾3+ 𝐾4,
𝑘 𝑥𝑦=𝑘 𝑦𝑥= 0,
𝑘 𝑥𝜃 = 𝑘 𝜃𝑥 = 𝑑
2⁄ (𝐾1 − 𝐾2 − 𝐾3+ 𝐾4),
𝑘 𝑦𝜃 = 𝑘 𝜃𝑦 = 𝑏
2⁄ (−𝐾1 + 𝐾2 + 𝐾3 − 𝐾4),
𝑘 𝜃𝜃 = ( 𝑑2
4⁄ + 𝑏2
4⁄ ) (𝐾1 + 𝐾2 + 𝐾3+ 𝐾4),
where,𝐾idenotes total lateral stiffness of the building
of𝑖 𝑡ℎ
column ; 𝑘 𝑥𝑥 denotes total lateral stiffness of
the building along x-direction due to force along x-
direction; 𝑘 𝑦𝑦 denotes total lateral stiffness of the
building along y-direction due to force along y-
direction; 𝑘 𝑥𝑦 denotes total lateral stiffness of the
building along x-direction due to force along y-
direction; 𝑘 𝑦𝑥 denotes total lateral stiffness of the
building along y-direction due to force along x-
direction; 𝑘 𝑥𝜃 denotes total lateral stiffness of the
building along x-direction due to torsion in building;
𝑘 𝑦𝜃 denotes total lateral stiffness of the building
along y-direction due to torsion in building; 𝑘 𝜃𝜃
denotes total torsional stiffness of the building due
to torsion in building.
The damping matrix of the system is not
known explicitly and it is constructed from the
Rayleigh’s damping considering mass and stiffness
proportional as,
C = α M + β K …(4)
Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications
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Where, α and β are the coefficients depending on
damping ratio of two vibration modes. For the
present study, 5 % damping is considered for both
modes of vibration of system.
The governing equations of motion are
solved using the state-space method (Hart and Wong
2000; Lu 2004) and rewritten as:
𝑧 𝑘+1 = 𝑒 𝐴∆𝑡
𝑧 𝑘 + 𝐴−1(𝑒 𝐴∆𝑡
− 𝐼)𝑢 𝑔̈ …(5)
where, 𝑧 = { 𝑢 𝑢̇} 𝑇
is a state vector; 𝐴 is the system
matrix; 𝐼 is the identity matrix; and 𝑒 𝐴∆𝑡
is the state
transition matrix. These matrices are expressed as,
𝐴 = [
0 1
−𝑀−1
𝐾 −𝑀−1
𝐶
] …(6)
𝑧̈ 𝑘+1 = 𝐴 𝑧 𝑘 + 𝐻 𝑢 𝒈̈ …(7)
𝐻 =
[
0 0
0
0
0
0
−1
−1
−1
−1
−1
−1]
…(8)
where, 𝑧̇ = { 𝑢̇ 𝑢̈} 𝑇
is a state vector, k denotes the
time step; and H is the distribution matrix of
excitations.
(a) Plan of two-way asymmetric building
(b) Isometric view of system showing bi-direction
excitation and floor response
Fig. 1 : Plan and isometric view of two-way
asymmetric building showing bi-direction
excitation and floor response
III. MODEL OF NON-STRUCTURAL
ELEMENT AND SOLUTION OF
EQUATION OF MOTION
The NSE of steel material (2% damping)
placed at various places of two-way asymmetric
single story building (5% damping) is shown in Fig.
2. The NSE is placed at stiff and flexible edge (along
X direction) and stiff and flexible edge (along Y
direction) of the system. The building is analysed
under bi-direction earthquake ground motions.
Following assumptions are made for NSE under
consideration: (i) the NSE is excited by
unidirectional horizontal component of floor
response due to earthquake ground motion and the
vertical component of floor response due to
earthquake motion is neglected, (ii) the NSE is
assumed to be rigidly connected with floor of
building. The governing equations of motion of the
NSE with lateral and torsional degrees of freedom of
the system are expressed as:
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𝑚𝑢 𝑁̈ + 𝑐𝑢 𝑁̇ + 𝑘𝑢 𝑁 = −𝑚(𝑢 𝑔̈ + 𝑢̈) …(9)
where m is mass of NSE; c= 2ξ𝜔 𝑛m, is damping of
NSE; and k=m𝜔 𝑛
2
is stiffness of the NSE; 𝑢 𝑁 is the
displacement of NSE; 𝑢̈ 𝑔is the ground acceleration;
𝑢̈ is acceleration of floor, 𝑢 𝑥𝑠̈ 𝑎𝑛𝑑 𝑢 𝑥𝑓̈ = 𝑢 𝑥̈ ±
𝑢 𝜃̈ ( 𝑏
2⁄ ), is acceleration of floor at Stiff and flexible
edge (along X- direction) ,𝑢 𝑦𝑠̈ 𝑎𝑛𝑑 𝑢 𝑦𝑓̈ = 𝑢 𝑦̈ ±
𝑢 𝜃̈ ( 𝑑
2⁄ ), is acceleration of floor at Stiff and flexible
edge (along Y-direction).
The governing equations of motion are
solved using the state-space method (Hart and Wong
2000; Lu 2004) and rewritten as:
𝑧 𝑛 𝑘+1
= 𝑧 𝑛 𝑘
+ 𝐴 𝑛
−1
(𝑒 𝐴 𝑛∆𝑡
− 𝐼 𝑛)(𝑢 𝑔̈ + 𝑢̈) .(10)
where 𝑧 𝑛 = {𝑢 𝑁 𝑢 𝑁̇ } 𝑇
is a state vector; 𝐴 𝑛 is the
system matrix; 𝐼 𝑛 is the identity matrix for NSE; and
𝑒 𝐴 𝑛∆𝑡
is the state transition matrix. These matrices
are expressed as,
𝐴 𝑛 = [
0 1
−𝑚−1
𝑘 −𝑚−1
𝑐
] …(11)
𝑧 ̇ 𝑛 𝑘+1
= 𝐴 𝑛 𝑧 𝑛 𝑘
+ 𝐻 𝑛 (𝑢 𝑔̈ + 𝑢̈) …(12)
𝐻 𝑛 = [
0
−1
] …(13)
Where,𝑧 𝑛̇ = {𝑢̇ 𝑁 𝑢̈ 𝑁} 𝑇
is a state vector, k denotes
the time step; and 𝐻 𝑛 is the distribution matrix of
excitations.
(a) NSE placed at flexible edge along X-direction
(b) NSE placed at Stiff edge along X-direction
(c) NSE placed at flexible edge along Y-direction
(d) NSE placed at stiff edge along Y-direction
Fig. 2 : Isometric view of asymmetric building
showing NSE placed at various places and their
responses.
IV. NUMERICAL STUDY
The seismic response of Non-Structural
Element placed on asymmetric single story building
is investigated by numerical simulation study. The
maximum displacements as well as maximum
Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications
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accelerations of NSE are obtained at stiff and
flexible edge (along X direction), and the stiff and
flexible edge (along Y direction) on asymmetric
single story building. The response quantities of
interest are lateral and torsional displacements of the
floor due to bi-direction earthquake obtained at the
CM (ux ,uy and uθ ), displacements at stiff and
flexible edges (along X-direction) of the system
(𝑢 𝑥𝑠 𝑎𝑛𝑑 𝑢 𝑥𝑓 = 𝑢 𝑥 ± 𝑢 𝜃 ( 𝑏
2⁄ )), and at stiff and
flexible edges (along Y-direction) of the system (
𝑢 𝑦𝑠 𝑎𝑛𝑑 𝑢 𝑦𝑓 = 𝑢 𝑦 ± 𝑢 𝜃 ( 𝑑
2⁄ )), lateral and
torsional accelerations of the floor obtained at the
CM (𝑢 𝑥̈ , 𝑢 𝑦̈ 𝑎𝑛𝑑 𝑢 𝜃̈ ), accelerations at stiff and
flexible edges (along X-direction) of the system
(𝑢 𝑥𝑠̈ 𝑎𝑛𝑑 𝑢 𝑥𝑓̈ = 𝑢 𝑥̈ ± 𝑢 𝜃̈ ( 𝑏
2⁄ )), and at stiff and
flexible edges (along Y-direction) of the system
(𝑢 𝑦𝑠̈ 𝑎𝑛𝑑 𝑢 𝑦𝑓̈ = 𝑢 𝑦̈ ± 𝑢 𝜃̈ ( 𝑑
2⁄ )).The response is
investigated under following parametric variations:
uncoupled lateral time period of system (𝑇𝑥 =
2𝜋
𝜔 𝑥
⁄ 𝑎𝑛𝑑 𝑇𝑦 = 2𝜋
𝜔 𝑦
⁄ ), lateral time period for
stiff NSE (T=0.25sec) and for flexible NSE
(T=1sec). The peak responses are obtained
corresponding to the parameters which are listed
above and variations are plotted for the four real
earthquake ground motions namely, Imperial Valley
(1940), Loma Prieta (1989), Northridge (1994) and
Kobe (1995) as per the details summarized in Table
1. The time histories of the ground motions of the
earthquakes are shown in Fig. 3. The considered
earthquakes are most accurately recorded and are
widely used by the researchers and they cover the
range of all varieties of earthquakes and hence shall
be helpful to lead to the generalized conclusions.
The numerical study has been carried out to
investigate the peak displacements and peak
accelerations of NSE which is placed at various
positions on two-way asymmetric building (building
height consider for Stiff building is 3.5m and for
flexible building it is 25m) under bi-direction
excitations. The time period for stiff NSE is taken as
0.25 second and for flexible NSE it is 1 second.
Table 1: Details of earthquake motions considered for the numerical study
Earthquake Recording station
Duration
(sec)
Component
for X-
direction
PGA (g)
for X-
direction
Component
for Y-
direction
PGA (g)
for Y-
direction
Imperial
Valley, 19 May
1940
El Centro (USGS 117,
Array# 9)
40 ELC 180 0.3129 ELC 270 0.2148
Loma Prieta,
18 October
1989
Los Gatos Presentation
Center (LGPC, UCSC
16)
25 LGP 000 0.9663 LGP 090 0.5872
Northridge, 17
January 1994
Sylmar Converter
Station (DWP 74)
40 SCS 142 0.8972 SCS 52 0.6125
Kobe, 16
January 1995
Japan Meteorological
Agency (JMA, 99999
KJMA)
48 KJM 000 0.8213 KJM 090 0.5985
Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications
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Fig. 3: Earthquake ground motions considered for the study
The time history analysis is carried out for NSE and
building. The time histories of displacements and
accelerations are plotted for NSE and buildings
when NSE is placed at various places (flexible and
stiff edge along X-direction and flexible and stiff
edge along Y-direction) in building for different
conditions (i.e stiff NSE placed on stiff system,
Flexible NSE placed on stiff system, stiff NSE
placed on flexible system and flexible NSE placed
on flexible system) under four earthquakes (i.e
Imperial Valley, Kobe, Loma prieta and
Northridge). From the seismic responses for the
NSE and buildings under the four earthquake
excitations considered, the optimum place is
selected for NSE to perform effectively under
earthquake excitations.
1) Stiff NSE placed on Stiff asymmetric building
The floor acceleration of the building is
applied as a ground motion for the NSE and the
response of NSE (i.e. displacements and
accelerations) are obtained and plotted in Fig. 4. The
time histories of displacements and accelerations for
NSE, when stiff NSE is placed on stiff asymmetric
building at various places (as shown in Fig. 2) under
Imperial Valley earthquake are shows in Fig. 4. In
which, dnXF and dnXS denotes the displacement of
NSE at flexible and stiff edge along X-direction,
dnYF and dnYS denotes the displacement of NSE at
flexible and stiff edge along Y-direction. AnXF and
AnXS denotes the acceleration of NSE at flexible
and stiff edge along X-direction and AnYF and
AnYS denotes the acceleration of NSE at flexible
and stiff edge along Y-direction, respectively.
Similarly, the results are obtained for other
earthquakes such as Kobe, Loma Prieta and
Northridge.
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Fig. 4: Time histories for Displacements and Accelerations of stiff NSE placed (at Stiff and Flexible
Edge along X-direction and along Y-direction) on stiff Building under Imperial Valley Earthquake
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Table 2: Peak Displacement and Peak Acceleration for Stiff NSE placed on Stiff asymmetric building.
Response
Imperial
Valley
Kobe
Loma
Prieta
Northridge Average
dnXS(m) 0.0185 0.0544 0.0247 0.0330 0.0326
dnXF(m) 0.0201 0.0320 0.0281 0.0311 0.0278
dnYS(m) 0.0224 0.0598 0.0274 0.0201 0.0324
dnYF(m) 0.0163 0.0259 0.0230 0.0183 0.0208
AnXS(m/sec2
) 15.0982 31.4101 28.1518 15.1686 22.4571
AnXF(m/sec2
) 12.7881 15.5279 17.8554 12.4447 14.6540
AnYS(m/sec2
) 15.8664 32.9884 27.0113 11.5297 21.8489
AnYF(m/sec2
) 9.9364 13.8569 13.6852 9.5609 11.7598
Table 2 shows the peak displacement and peak
acceleration values for various earthquakes and the
average values for stiff NSE placed on stiff
asymmetric building. From the Table 2, it is
observed that the displacement and acceleration of
NSE is less when NSE is placed on flexible edge of
building as compared to stiff edge.
2) Flexible NSE placed on Stiff asymmetric
building
The time histories of the displacements and
accelerations for NSE, when flexible NSE is placed
on stiff asymmetric building at various places under
Imperial Valley earthquake are shows in Fig. 5.
Similarly the results are obtained for other
earthquakes such as Kobe, Loma Prieta and
Northridge.
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Fig. 5: Time histories for Displacement and Acceleration of flexible NSE placed (at Stiff and Flexible
Edge along X-direction and along Y-direction) on stiff Building under Imperial Valley Earthquake
Table 3: Peak Displacement and Peak Acceleration for flexible NSE placed on Stiff asymmetric building
Response
Imperial
Valley
Kobe Loma Priata Northridge Average
dnXS(m) 0.1567 0.3742 0.2806 0.4082 0.3049
dnXF(m) 0.1593 0.4403 0.2814 0.4009 0.3204
dnYS(m) 0.0639 0.4300 0.1277 0.4060 0.2569
dnYF(m) 0.0744 0.3769 0.1334 0.4203 0.2512
AnXS(m/sec2
) 12.7982 28.2494 30.1454 17.8892 22.2705
AnXF(m/sec2
) 9.4693 21.6578 19.5792 17.8309 17.1343
AnYS(m/sec2
) 9.5646 25.1792 27.5009 16.8230 19.7669
AnYF(m/sec2
) 3.5693 19.6678 12.1277 17.0077 13.0931
The peak displacement and peak acceleration
values for various earthquakes and the average
values for flexible NSE placed on stiff asymmetric
building are as shown in Table 3. From the Table 3,
it is observed that the displacement of NSE is less
when it is placed on building along Y-direction as
compared to along X-direction and acceleration of
NSE less when NSE placed on flexible edge of
building as compared to stiff edge.
3) Stiff NSE placed on flexible asymmetric
building
The time histories of displacements and
accelerations for NSE, when stiff NSE placed on
flexible asymmetric building at various places under
Imperial Valley earthquake are shows in Fig. 6.
Similarly, the results are obtained for other
earthquakes such as Kobe, Loma Prieta and
Northridge.
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Fig. 6: Time histories for Displacement and Acceleration of stiff NSE placed (at Stiff and Flexible
Edge along X-direction and along Y-direction) on flexible Building under Imperial Valley
Earthquake
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Table 4: Peak Displacement and Peak Acceleration for stiff NSE placed on flexible asymmetric building
Response
Imperial
Valley
Kobe Loma Priata Northridge Average
dnXS(m) 0.0216 0.0430 0.0319 0.0430 0.0348
dnXF(m) 0.0195 0.0317 0.0310 0.0351 0.0293
dnYS(m) 0.0208 0.0371 0.0301 0.0266 0.0286
dnYF(m) 0.0150 0.0240 0.0237 0.0190 0.0204
AnXS(m/sec2
) 20.3036 23.0869 49.7014 27.6464 30.1845
AnXF(m/sec2
) 18.1060 16.2312 37.7042 28.4492 25.1226
AnYS(m/sec2
) 14.3309 20.9834 56.3394 20.5907 28.0611
AnYF(m/sec2
) 9.4018 12.2900 37.0867 21.1391 19.9794
The peak displacement and peak acceleration
values for various earthquakes and the average value
for stiff NSE placed on flexible asymmetric building
are as shown in Table 4. From the Table 4, it is
observed that the displacement of NSE is less when
it is placed on building along Y-direction as
compared to along X-direction and acceleration of
NSE is less when NSE is placed on flexible edge of
building as compared to stiff edge.
4) Flexible NSE placed on flexible asymmetric
building
The time histories of displacements and
accelerations for NSE, when flexible NSE placed on
flexible asymmetric building at various places under
Imperial Valley earthquake are shows in Fig. 7.
Similarly, the results are obtained for other
earthquakes such as Kobe, Loma Prieta and
Northridge.
Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications
www.ijera.com
ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42
www.ijera.com 41 | P a g e
Fig. 7: Time histories for Displacement and Acceleration of flexible NSE placed (at Stiff and Flexible
Edge along X-direction and along Y-direction) on flexible Building under Imperial Valley
Earthquake
Table 5: Peak Displacement and Peak Acceleration for flexible NSE placed on flexible asymmetric building
Response
Imperial
Valley
Kobe Loma Priata Northridge Average
dnXS(m) 0.1599 0.3957 0.2857 0.4144 0.3139
dnXF(m) 0.1582 0.4373 0.2828 0.4017 0.3200
dnYS(m) 0.0655 0.3989 0.1313 0.4116 0.2518
dnYF(m) 0.0716 0.3757 0.1338 0.4194 0.2501
AnXS(m/sec2
) 16.1957 23.4060 44.6513 22.9830 26.8090
AnXF(m/sec2
) 13.4392 23.1828 41.1663 28.9612 26.6874
AnYS(m/sec2
) 9.6969 23.2217 54.2783 22.7902 27.4968
AnYF(m/sec2
) 6.8831 19.6746 38.5967 22.1392 21.8234
The peak displacement and peak acceleration
values for various earthquakes and the average
values for flexible NSE placed on flexible
asymmetric building are as shown in Table 5. From
the Table-5, it is observed that the displacement of
NSE is less when it placed on building along Y-
direction as compared to along the X-direction and
acceleration of NSE less when NSE placed on
flexible edge of building as compared to stiff edge.
IV. CONCLUSIONS:
The seismic response of non-structural element
placed on single-storey, two-way asymmetric
building under bi-directional excitations is
investigated. The seismic response of the system and
non-structural element is obtained by numerically
solving the equations under the different system
parameters. From the present numerical study, the
following conclusions can be drawn:
1. The displacement and acceleration of NSE is
less when NSE is placed on flexible edge of
building as compared to stiff edge when stiff
NSE is placed on stiff building. Also, the
displacement of NSE is less when it is placed on
building along Y-direction as compared to
along the X-direction and acceleration of NSE
less when NSE is placed on flexible edge of
building as compared to stiff edge when stiff or
flexible NSE is placed on flexible building as
well as flexible NSE is placed on stiff building.
Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications
www.ijera.com
ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42
www.ijera.com 42 | P a g e
2. The peak displacement and peak acceleration of
NSE is less at the flexible edge along the Y-
direction of one-story two-way asymmetric
building subjected to bi-direction excitations.
3. It is advisable to place the NSE at the flexible
edge along the Y-direction of one-storey two
way asymmetric building because the seismic
responses (i.e., displacement and acceleration)
of NSE is less at that place so that it will
perform better in earthquake.
REFERENCES:
[1] Murty C.V.R.,Goswami Rupen.(2005)
"Earthquake Protection of Non-Structural
Elements in Buildings" Gujarat State
Disaster Management Authority.
[2] Vijayanarayanan A.R.,Goswami Rupen
and Murty C.V.R. (2012),”Determining
Levels of Seismic Shaking Effects in
Buildings for securing Non-Structural
Elements.” Fourth International
Conference on Structural Stability and
Dynamics (ICSSD 2012), 4–6 January,
2012. Malaviya National Institute of
Technology, Jaipur & Texas A&M
University, USA
[3] Mondal Goutam and Jain Sudhir K (2005),
Design of Non-Structural Elements for
buildings: A review of codal provisions by,
The Indian Concrete Journal, August 2005.
[4] Mondal Goutam and Jain Sudhir K,
Proposed draft for IS: 1893 on design of
Non-Structural Elements, The Indian
Concrete Journal, and October 2005.
[5] Christoph Adam and Peter a Fotiu, (1997),
“Dynamic response of earthquake excited
inelastic primary secondary systems",
EarthquakeEng. Struct. Dyn., vol:22,
pp:58–71.
[6] VillaverdeRoberto, (1997), “Method to
improve seismic provisions for non-
structural components in buildings”,
Journal of Structural Engineering, Vol.
123, Paper No. 13719, Pg no: 432-439
[7] Singh, M. P., Suarez, L. E., Matheu, E. E.,
and Maldonado, G. O., (2006), “Seismic
Design Forces.II: Flexible Non-structural
Components”, Journal of structural
engineering © ASCE, October 2006 ,Vol.
132, No. 10.
[8] Chaudhuri Samit Ray and Villaverde
Roberto, (2008), “Effect of Building
Nonlinearity on Seismic Response of Non-
structural Components: A Parametric
Study”, Journal of structural engineering ©
ASCE, April 2008, Vol. 134, No.4.
[9] Dhanani Suresh L., Patel Sumant B.,
Mevada Snehal V, (2013), “Seismic
Response of Non-Structural Elements”,
International Journal of innovations in
Engineering and Technology (IJIET),
Vol.2.
[10] Hart GC and Wong K, “Structural Dynamics
for Structural Engineers”, John Wiley
&Sons, Inc.
[11] Lyan-Ywan Lu (2004). “Predictive control
of seismic structures with semi-active
friction dampers” earthquake engineering
and structural dynamics.
[12] Chopra AK., “Dynamics of Structures”,
Third Edition, Pearson Publication.

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Seismic Response of Non-Structural Element Placed on Single Story Two-Way Asymmetric Building under Bi-Directional Excitations

  • 1. Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42 www.ijera.com 30 | P a g e Seismic Response of Non-Structural Element Placed on Single Story Two-Way Asymmetric Building under Bi-Directional Excitations Pinkesh M. Dalal 1 , Snehal V. Mevada2 , Sumant B. Patel3 1 P.G. Student,2 Assistant Professor,3 Associate Professor, 1-2-3 Structural Engineering Department, Birla Vishvakarma Mahavidyalaya [Engineering College], Vallabh Vidyanagar, Gujarat, India. Abstract: The seismic response of non-structural element placed on single-storey, two-way asymmetric building under bi-directional excitations is investigated. The response is obtained by numerically solving the governing equations of motion. The seismic response of the system and non-structural element is obtained by numerically solving the equations of motion using state-space method under different system parameters. The comparative performance is investigated of non-structural element placed at different places on single story asymmetric building and finding a best place for survival during earthquake. It is found that non-structural element at flexible edge along Y- direction gives less response of displacement and acceleration. So, non-structural element placed at flexible edge along Y- direction on asymmetric SDOF system performs better in earthquake than at other places. Keywords: Seismic, Bi-Direction Excitation, Non-Structural Elements, Displacement, Acceleration. I. INTRODUCTION Non-structural elements (NSEs) of a building are not a part of the main load-resisting system. Murty and Goswami (2005) found that the damage costs of Non-Structural Elements (NSEs) may account for 65% to 85% of the total construction cost of commercial buildings. Vijayanarayanan et al. (2012) found that in critical facilities, building has losses due to damaging equipment and inventory can be two to three times greater than the cost of replacing collapsed buildings or structures. Classification of Non-Structural Elements 1) Architectural Components: This category includes the elevator penthouses, stairways, partitions, parapets, and heliports, cladding systems, signboards, lighting systems and suspended ceilings. 2) Mechanical and Electrical Equipment: This category includes the storage tanks, pressure vessels, piping systems, ducts, escalators, smokestacks, antennas, cranes, radars and object tracking devices, computer and data acquisition systems, control panels, transformers, switchgears, emergency power systems, fire protection systems, boilers, heat exchangers, chillers, cooling towers and machinery such as pumps, turbines, generators, engines and motors. 3) Building Contents and Inventory: This category includes the masonry wall, door, window, stair, Bookshelves, file cabinets, storage racks, decorative items and any other piece of furniture commonly found in office buildings and warehouses (Mondal and Jain, 2005) In the past, many researchers investigated and studied about the behaviour of NSEs. Adam and fotiu (1997) investigated numerically the effect of ductile material behaviour on the response of coupled primary-secondary systems by using linear and nonlinear floor response spectra. Villaverde(1997)determined simple way equivalent static lateral forces for the seismic design of NSE attached to primary structure. Mondal and Jain (2005) provide design philosophy and design provision of international seismic code, and recommended design lateral forces. Singh et al.(2006)calculated and compared the seismic design force for flexible non-structural component by using floor response spectra. Chaudhuri and Villaverde(2008) investigated the seismic response of NSE which are attached to steel moment resisting frames and series of linear and nonlinear SDOF by using ensemble of 25 recorded earthquake ground motion and influence of the NSE location, nonlinearity and damping ratio. Dhanani et al.(2013) investigated the seismic response of NSE by using time history analysis, NSE placed on various floor at RESEARCH ARTICLE OPEN ACCESS
  • 2. Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42 www.ijera.com 31 | P a g e various place of three story asymmetric building and analysis has been perform to obtain the displacement and acceleration of NSE. Although, some of the work has been done to investigate the seismic response of NSE. However, no work has been reported to obtain the optimum location of NSE when NSEs placed on asymmetric building under bi- direction excitation. The objectives of the study are summarized as: (i) to perform the time history analysis to find the acceleration and displacement for NSEs placed at various locations on single story two-way asymmetric building, (ii) to determine the best suitable location for non-structural elements on single story two-way asymmetric buildings. II. STRUCTURAL MODEL AND SOLUTION OF EQUATIONS OF MOTION The system considered is an idealized single- storey building which consists of a rigid deck supported on columns as shown in Fig. 1. Following assumptions are made for the structural system under consideration: (i) floor of the superstructure is assumed as rigid, (ii) force–deformation behaviour of the superstructure is considered as linear and within elastic range (iii) the structure is excited by bi-directional horizontal component of earthquake ground motion and the vertical component of earthquake motion is neglected, and (iv) mass of the columns is ignored and the columns are considered to only provide lateral stiffness. The mass of deck is assumed to be uniformly distributed and hence centre of mass (CM) coincides with the geometrical centre of the deck. The stiffness asymmetry with respect to the CM in two direction and hence, the centre of rigidity (CR) is located at an eccentric distance, ex from CM in x-direction and ey from CM in y-direction. The system is asymmetric and therefore, three degrees of freedom are considered for model namely the lateral displacement in x- direction, ux lateral displacement in y-direction, uy and torsional displacement, uθ as represented in Fig. 1. The governing equations of motion of the building with lateral and torsional degrees of freedom of the system are obtained in the matrix form are expressed as: 𝑀𝑢̈ + 𝐶𝑢̇ + 𝐾𝑢 = −𝑀𝑢 𝑔̈ …(1) where, M, C and K are the mass, damping and stiffness matrices of the system, respectively; 𝑢 = { 𝑢 𝑥 𝑢 𝑦 𝑢 𝜃}T is the displacement vector; 𝑢̈ 𝑔 = { 𝑢̈ 𝑔𝑥 𝑢̈ 𝑔𝑦 0}T is the ground acceleration vector; and𝑢̈ 𝑔𝑥 and 𝑢̈ 𝑔𝑦is the ground acceleration in x and y-direction respectively. The mass matrix can be expressed as: 𝑀 = [ 𝑚 0 0 0 𝑚 0 0 0 𝑚𝑟2 ] …(2) where, m represents the lumped mass of the deck; and r is the mass radius of gyration about the vertical axis through CM which is given by, 𝑟 = √(𝑏2 + 𝑑2)/12; where b and d are the plan dimensions of the building. The stiffness matrix of the system is obtained as follows: 𝐾 = [ 𝑘 𝑥𝑥 𝑘 𝑥𝑦 𝑘 𝑥𝜃 𝑘 𝑦𝑥 𝑘 𝑦𝑦 𝑘 𝑦𝜃 𝑘 𝜃𝑥 𝑘 𝜃𝑦 𝑘 𝜃𝜃 ] …(3) Where 𝑘 𝑥𝑥= 𝐾1 + 𝐾2 + 𝐾3+ 𝐾4, 𝑘 𝑦𝑦= 𝐾1 + 𝐾2 + 𝐾3+ 𝐾4, 𝑘 𝑥𝑦=𝑘 𝑦𝑥= 0, 𝑘 𝑥𝜃 = 𝑘 𝜃𝑥 = 𝑑 2⁄ (𝐾1 − 𝐾2 − 𝐾3+ 𝐾4), 𝑘 𝑦𝜃 = 𝑘 𝜃𝑦 = 𝑏 2⁄ (−𝐾1 + 𝐾2 + 𝐾3 − 𝐾4), 𝑘 𝜃𝜃 = ( 𝑑2 4⁄ + 𝑏2 4⁄ ) (𝐾1 + 𝐾2 + 𝐾3+ 𝐾4), where,𝐾idenotes total lateral stiffness of the building of𝑖 𝑡ℎ column ; 𝑘 𝑥𝑥 denotes total lateral stiffness of the building along x-direction due to force along x- direction; 𝑘 𝑦𝑦 denotes total lateral stiffness of the building along y-direction due to force along y- direction; 𝑘 𝑥𝑦 denotes total lateral stiffness of the building along x-direction due to force along y- direction; 𝑘 𝑦𝑥 denotes total lateral stiffness of the building along y-direction due to force along x- direction; 𝑘 𝑥𝜃 denotes total lateral stiffness of the building along x-direction due to torsion in building; 𝑘 𝑦𝜃 denotes total lateral stiffness of the building along y-direction due to torsion in building; 𝑘 𝜃𝜃 denotes total torsional stiffness of the building due to torsion in building. The damping matrix of the system is not known explicitly and it is constructed from the Rayleigh’s damping considering mass and stiffness proportional as, C = α M + β K …(4)
  • 3. Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42 www.ijera.com 32 | P a g e Where, α and β are the coefficients depending on damping ratio of two vibration modes. For the present study, 5 % damping is considered for both modes of vibration of system. The governing equations of motion are solved using the state-space method (Hart and Wong 2000; Lu 2004) and rewritten as: 𝑧 𝑘+1 = 𝑒 𝐴∆𝑡 𝑧 𝑘 + 𝐴−1(𝑒 𝐴∆𝑡 − 𝐼)𝑢 𝑔̈ …(5) where, 𝑧 = { 𝑢 𝑢̇} 𝑇 is a state vector; 𝐴 is the system matrix; 𝐼 is the identity matrix; and 𝑒 𝐴∆𝑡 is the state transition matrix. These matrices are expressed as, 𝐴 = [ 0 1 −𝑀−1 𝐾 −𝑀−1 𝐶 ] …(6) 𝑧̈ 𝑘+1 = 𝐴 𝑧 𝑘 + 𝐻 𝑢 𝒈̈ …(7) 𝐻 = [ 0 0 0 0 0 0 −1 −1 −1 −1 −1 −1] …(8) where, 𝑧̇ = { 𝑢̇ 𝑢̈} 𝑇 is a state vector, k denotes the time step; and H is the distribution matrix of excitations. (a) Plan of two-way asymmetric building (b) Isometric view of system showing bi-direction excitation and floor response Fig. 1 : Plan and isometric view of two-way asymmetric building showing bi-direction excitation and floor response III. MODEL OF NON-STRUCTURAL ELEMENT AND SOLUTION OF EQUATION OF MOTION The NSE of steel material (2% damping) placed at various places of two-way asymmetric single story building (5% damping) is shown in Fig. 2. The NSE is placed at stiff and flexible edge (along X direction) and stiff and flexible edge (along Y direction) of the system. The building is analysed under bi-direction earthquake ground motions. Following assumptions are made for NSE under consideration: (i) the NSE is excited by unidirectional horizontal component of floor response due to earthquake ground motion and the vertical component of floor response due to earthquake motion is neglected, (ii) the NSE is assumed to be rigidly connected with floor of building. The governing equations of motion of the NSE with lateral and torsional degrees of freedom of the system are expressed as:
  • 4. Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42 www.ijera.com 33 | P a g e 𝑚𝑢 𝑁̈ + 𝑐𝑢 𝑁̇ + 𝑘𝑢 𝑁 = −𝑚(𝑢 𝑔̈ + 𝑢̈) …(9) where m is mass of NSE; c= 2ξ𝜔 𝑛m, is damping of NSE; and k=m𝜔 𝑛 2 is stiffness of the NSE; 𝑢 𝑁 is the displacement of NSE; 𝑢̈ 𝑔is the ground acceleration; 𝑢̈ is acceleration of floor, 𝑢 𝑥𝑠̈ 𝑎𝑛𝑑 𝑢 𝑥𝑓̈ = 𝑢 𝑥̈ ± 𝑢 𝜃̈ ( 𝑏 2⁄ ), is acceleration of floor at Stiff and flexible edge (along X- direction) ,𝑢 𝑦𝑠̈ 𝑎𝑛𝑑 𝑢 𝑦𝑓̈ = 𝑢 𝑦̈ ± 𝑢 𝜃̈ ( 𝑑 2⁄ ), is acceleration of floor at Stiff and flexible edge (along Y-direction). The governing equations of motion are solved using the state-space method (Hart and Wong 2000; Lu 2004) and rewritten as: 𝑧 𝑛 𝑘+1 = 𝑧 𝑛 𝑘 + 𝐴 𝑛 −1 (𝑒 𝐴 𝑛∆𝑡 − 𝐼 𝑛)(𝑢 𝑔̈ + 𝑢̈) .(10) where 𝑧 𝑛 = {𝑢 𝑁 𝑢 𝑁̇ } 𝑇 is a state vector; 𝐴 𝑛 is the system matrix; 𝐼 𝑛 is the identity matrix for NSE; and 𝑒 𝐴 𝑛∆𝑡 is the state transition matrix. These matrices are expressed as, 𝐴 𝑛 = [ 0 1 −𝑚−1 𝑘 −𝑚−1 𝑐 ] …(11) 𝑧 ̇ 𝑛 𝑘+1 = 𝐴 𝑛 𝑧 𝑛 𝑘 + 𝐻 𝑛 (𝑢 𝑔̈ + 𝑢̈) …(12) 𝐻 𝑛 = [ 0 −1 ] …(13) Where,𝑧 𝑛̇ = {𝑢̇ 𝑁 𝑢̈ 𝑁} 𝑇 is a state vector, k denotes the time step; and 𝐻 𝑛 is the distribution matrix of excitations. (a) NSE placed at flexible edge along X-direction (b) NSE placed at Stiff edge along X-direction (c) NSE placed at flexible edge along Y-direction (d) NSE placed at stiff edge along Y-direction Fig. 2 : Isometric view of asymmetric building showing NSE placed at various places and their responses. IV. NUMERICAL STUDY The seismic response of Non-Structural Element placed on asymmetric single story building is investigated by numerical simulation study. The maximum displacements as well as maximum
  • 5. Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42 www.ijera.com 34 | P a g e accelerations of NSE are obtained at stiff and flexible edge (along X direction), and the stiff and flexible edge (along Y direction) on asymmetric single story building. The response quantities of interest are lateral and torsional displacements of the floor due to bi-direction earthquake obtained at the CM (ux ,uy and uθ ), displacements at stiff and flexible edges (along X-direction) of the system (𝑢 𝑥𝑠 𝑎𝑛𝑑 𝑢 𝑥𝑓 = 𝑢 𝑥 ± 𝑢 𝜃 ( 𝑏 2⁄ )), and at stiff and flexible edges (along Y-direction) of the system ( 𝑢 𝑦𝑠 𝑎𝑛𝑑 𝑢 𝑦𝑓 = 𝑢 𝑦 ± 𝑢 𝜃 ( 𝑑 2⁄ )), lateral and torsional accelerations of the floor obtained at the CM (𝑢 𝑥̈ , 𝑢 𝑦̈ 𝑎𝑛𝑑 𝑢 𝜃̈ ), accelerations at stiff and flexible edges (along X-direction) of the system (𝑢 𝑥𝑠̈ 𝑎𝑛𝑑 𝑢 𝑥𝑓̈ = 𝑢 𝑥̈ ± 𝑢 𝜃̈ ( 𝑏 2⁄ )), and at stiff and flexible edges (along Y-direction) of the system (𝑢 𝑦𝑠̈ 𝑎𝑛𝑑 𝑢 𝑦𝑓̈ = 𝑢 𝑦̈ ± 𝑢 𝜃̈ ( 𝑑 2⁄ )).The response is investigated under following parametric variations: uncoupled lateral time period of system (𝑇𝑥 = 2𝜋 𝜔 𝑥 ⁄ 𝑎𝑛𝑑 𝑇𝑦 = 2𝜋 𝜔 𝑦 ⁄ ), lateral time period for stiff NSE (T=0.25sec) and for flexible NSE (T=1sec). The peak responses are obtained corresponding to the parameters which are listed above and variations are plotted for the four real earthquake ground motions namely, Imperial Valley (1940), Loma Prieta (1989), Northridge (1994) and Kobe (1995) as per the details summarized in Table 1. The time histories of the ground motions of the earthquakes are shown in Fig. 3. The considered earthquakes are most accurately recorded and are widely used by the researchers and they cover the range of all varieties of earthquakes and hence shall be helpful to lead to the generalized conclusions. The numerical study has been carried out to investigate the peak displacements and peak accelerations of NSE which is placed at various positions on two-way asymmetric building (building height consider for Stiff building is 3.5m and for flexible building it is 25m) under bi-direction excitations. The time period for stiff NSE is taken as 0.25 second and for flexible NSE it is 1 second. Table 1: Details of earthquake motions considered for the numerical study Earthquake Recording station Duration (sec) Component for X- direction PGA (g) for X- direction Component for Y- direction PGA (g) for Y- direction Imperial Valley, 19 May 1940 El Centro (USGS 117, Array# 9) 40 ELC 180 0.3129 ELC 270 0.2148 Loma Prieta, 18 October 1989 Los Gatos Presentation Center (LGPC, UCSC 16) 25 LGP 000 0.9663 LGP 090 0.5872 Northridge, 17 January 1994 Sylmar Converter Station (DWP 74) 40 SCS 142 0.8972 SCS 52 0.6125 Kobe, 16 January 1995 Japan Meteorological Agency (JMA, 99999 KJMA) 48 KJM 000 0.8213 KJM 090 0.5985
  • 6. Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42 www.ijera.com 35 | P a g e Fig. 3: Earthquake ground motions considered for the study The time history analysis is carried out for NSE and building. The time histories of displacements and accelerations are plotted for NSE and buildings when NSE is placed at various places (flexible and stiff edge along X-direction and flexible and stiff edge along Y-direction) in building for different conditions (i.e stiff NSE placed on stiff system, Flexible NSE placed on stiff system, stiff NSE placed on flexible system and flexible NSE placed on flexible system) under four earthquakes (i.e Imperial Valley, Kobe, Loma prieta and Northridge). From the seismic responses for the NSE and buildings under the four earthquake excitations considered, the optimum place is selected for NSE to perform effectively under earthquake excitations. 1) Stiff NSE placed on Stiff asymmetric building The floor acceleration of the building is applied as a ground motion for the NSE and the response of NSE (i.e. displacements and accelerations) are obtained and plotted in Fig. 4. The time histories of displacements and accelerations for NSE, when stiff NSE is placed on stiff asymmetric building at various places (as shown in Fig. 2) under Imperial Valley earthquake are shows in Fig. 4. In which, dnXF and dnXS denotes the displacement of NSE at flexible and stiff edge along X-direction, dnYF and dnYS denotes the displacement of NSE at flexible and stiff edge along Y-direction. AnXF and AnXS denotes the acceleration of NSE at flexible and stiff edge along X-direction and AnYF and AnYS denotes the acceleration of NSE at flexible and stiff edge along Y-direction, respectively. Similarly, the results are obtained for other earthquakes such as Kobe, Loma Prieta and Northridge.
  • 7. Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42 www.ijera.com 36 | P a g e Fig. 4: Time histories for Displacements and Accelerations of stiff NSE placed (at Stiff and Flexible Edge along X-direction and along Y-direction) on stiff Building under Imperial Valley Earthquake
  • 8. Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42 www.ijera.com 37 | P a g e Table 2: Peak Displacement and Peak Acceleration for Stiff NSE placed on Stiff asymmetric building. Response Imperial Valley Kobe Loma Prieta Northridge Average dnXS(m) 0.0185 0.0544 0.0247 0.0330 0.0326 dnXF(m) 0.0201 0.0320 0.0281 0.0311 0.0278 dnYS(m) 0.0224 0.0598 0.0274 0.0201 0.0324 dnYF(m) 0.0163 0.0259 0.0230 0.0183 0.0208 AnXS(m/sec2 ) 15.0982 31.4101 28.1518 15.1686 22.4571 AnXF(m/sec2 ) 12.7881 15.5279 17.8554 12.4447 14.6540 AnYS(m/sec2 ) 15.8664 32.9884 27.0113 11.5297 21.8489 AnYF(m/sec2 ) 9.9364 13.8569 13.6852 9.5609 11.7598 Table 2 shows the peak displacement and peak acceleration values for various earthquakes and the average values for stiff NSE placed on stiff asymmetric building. From the Table 2, it is observed that the displacement and acceleration of NSE is less when NSE is placed on flexible edge of building as compared to stiff edge. 2) Flexible NSE placed on Stiff asymmetric building The time histories of the displacements and accelerations for NSE, when flexible NSE is placed on stiff asymmetric building at various places under Imperial Valley earthquake are shows in Fig. 5. Similarly the results are obtained for other earthquakes such as Kobe, Loma Prieta and Northridge.
  • 9. Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42 www.ijera.com 38 | P a g e Fig. 5: Time histories for Displacement and Acceleration of flexible NSE placed (at Stiff and Flexible Edge along X-direction and along Y-direction) on stiff Building under Imperial Valley Earthquake Table 3: Peak Displacement and Peak Acceleration for flexible NSE placed on Stiff asymmetric building Response Imperial Valley Kobe Loma Priata Northridge Average dnXS(m) 0.1567 0.3742 0.2806 0.4082 0.3049 dnXF(m) 0.1593 0.4403 0.2814 0.4009 0.3204 dnYS(m) 0.0639 0.4300 0.1277 0.4060 0.2569 dnYF(m) 0.0744 0.3769 0.1334 0.4203 0.2512 AnXS(m/sec2 ) 12.7982 28.2494 30.1454 17.8892 22.2705 AnXF(m/sec2 ) 9.4693 21.6578 19.5792 17.8309 17.1343 AnYS(m/sec2 ) 9.5646 25.1792 27.5009 16.8230 19.7669 AnYF(m/sec2 ) 3.5693 19.6678 12.1277 17.0077 13.0931 The peak displacement and peak acceleration values for various earthquakes and the average values for flexible NSE placed on stiff asymmetric building are as shown in Table 3. From the Table 3, it is observed that the displacement of NSE is less when it is placed on building along Y-direction as compared to along X-direction and acceleration of NSE less when NSE placed on flexible edge of building as compared to stiff edge. 3) Stiff NSE placed on flexible asymmetric building The time histories of displacements and accelerations for NSE, when stiff NSE placed on flexible asymmetric building at various places under Imperial Valley earthquake are shows in Fig. 6. Similarly, the results are obtained for other earthquakes such as Kobe, Loma Prieta and Northridge.
  • 10. Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42 www.ijera.com 39 | P a g e Fig. 6: Time histories for Displacement and Acceleration of stiff NSE placed (at Stiff and Flexible Edge along X-direction and along Y-direction) on flexible Building under Imperial Valley Earthquake
  • 11. Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42 www.ijera.com 40 | P a g e Table 4: Peak Displacement and Peak Acceleration for stiff NSE placed on flexible asymmetric building Response Imperial Valley Kobe Loma Priata Northridge Average dnXS(m) 0.0216 0.0430 0.0319 0.0430 0.0348 dnXF(m) 0.0195 0.0317 0.0310 0.0351 0.0293 dnYS(m) 0.0208 0.0371 0.0301 0.0266 0.0286 dnYF(m) 0.0150 0.0240 0.0237 0.0190 0.0204 AnXS(m/sec2 ) 20.3036 23.0869 49.7014 27.6464 30.1845 AnXF(m/sec2 ) 18.1060 16.2312 37.7042 28.4492 25.1226 AnYS(m/sec2 ) 14.3309 20.9834 56.3394 20.5907 28.0611 AnYF(m/sec2 ) 9.4018 12.2900 37.0867 21.1391 19.9794 The peak displacement and peak acceleration values for various earthquakes and the average value for stiff NSE placed on flexible asymmetric building are as shown in Table 4. From the Table 4, it is observed that the displacement of NSE is less when it is placed on building along Y-direction as compared to along X-direction and acceleration of NSE is less when NSE is placed on flexible edge of building as compared to stiff edge. 4) Flexible NSE placed on flexible asymmetric building The time histories of displacements and accelerations for NSE, when flexible NSE placed on flexible asymmetric building at various places under Imperial Valley earthquake are shows in Fig. 7. Similarly, the results are obtained for other earthquakes such as Kobe, Loma Prieta and Northridge.
  • 12. Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42 www.ijera.com 41 | P a g e Fig. 7: Time histories for Displacement and Acceleration of flexible NSE placed (at Stiff and Flexible Edge along X-direction and along Y-direction) on flexible Building under Imperial Valley Earthquake Table 5: Peak Displacement and Peak Acceleration for flexible NSE placed on flexible asymmetric building Response Imperial Valley Kobe Loma Priata Northridge Average dnXS(m) 0.1599 0.3957 0.2857 0.4144 0.3139 dnXF(m) 0.1582 0.4373 0.2828 0.4017 0.3200 dnYS(m) 0.0655 0.3989 0.1313 0.4116 0.2518 dnYF(m) 0.0716 0.3757 0.1338 0.4194 0.2501 AnXS(m/sec2 ) 16.1957 23.4060 44.6513 22.9830 26.8090 AnXF(m/sec2 ) 13.4392 23.1828 41.1663 28.9612 26.6874 AnYS(m/sec2 ) 9.6969 23.2217 54.2783 22.7902 27.4968 AnYF(m/sec2 ) 6.8831 19.6746 38.5967 22.1392 21.8234 The peak displacement and peak acceleration values for various earthquakes and the average values for flexible NSE placed on flexible asymmetric building are as shown in Table 5. From the Table-5, it is observed that the displacement of NSE is less when it placed on building along Y- direction as compared to along the X-direction and acceleration of NSE less when NSE placed on flexible edge of building as compared to stiff edge. IV. CONCLUSIONS: The seismic response of non-structural element placed on single-storey, two-way asymmetric building under bi-directional excitations is investigated. The seismic response of the system and non-structural element is obtained by numerically solving the equations under the different system parameters. From the present numerical study, the following conclusions can be drawn: 1. The displacement and acceleration of NSE is less when NSE is placed on flexible edge of building as compared to stiff edge when stiff NSE is placed on stiff building. Also, the displacement of NSE is less when it is placed on building along Y-direction as compared to along the X-direction and acceleration of NSE less when NSE is placed on flexible edge of building as compared to stiff edge when stiff or flexible NSE is placed on flexible building as well as flexible NSE is placed on stiff building.
  • 13. Pinkesh M. Dalal.et al. Int. Journal of Engineering Research and Applications www.ijera.com ISSN: 2248-9622, Vol. 6, Issue 5, (Part - 2) May 2016, pp.30-42 www.ijera.com 42 | P a g e 2. The peak displacement and peak acceleration of NSE is less at the flexible edge along the Y- direction of one-story two-way asymmetric building subjected to bi-direction excitations. 3. It is advisable to place the NSE at the flexible edge along the Y-direction of one-storey two way asymmetric building because the seismic responses (i.e., displacement and acceleration) of NSE is less at that place so that it will perform better in earthquake. REFERENCES: [1] Murty C.V.R.,Goswami Rupen.(2005) "Earthquake Protection of Non-Structural Elements in Buildings" Gujarat State Disaster Management Authority. [2] Vijayanarayanan A.R.,Goswami Rupen and Murty C.V.R. (2012),”Determining Levels of Seismic Shaking Effects in Buildings for securing Non-Structural Elements.” Fourth International Conference on Structural Stability and Dynamics (ICSSD 2012), 4–6 January, 2012. Malaviya National Institute of Technology, Jaipur & Texas A&M University, USA [3] Mondal Goutam and Jain Sudhir K (2005), Design of Non-Structural Elements for buildings: A review of codal provisions by, The Indian Concrete Journal, August 2005. [4] Mondal Goutam and Jain Sudhir K, Proposed draft for IS: 1893 on design of Non-Structural Elements, The Indian Concrete Journal, and October 2005. [5] Christoph Adam and Peter a Fotiu, (1997), “Dynamic response of earthquake excited inelastic primary secondary systems", EarthquakeEng. Struct. Dyn., vol:22, pp:58–71. [6] VillaverdeRoberto, (1997), “Method to improve seismic provisions for non- structural components in buildings”, Journal of Structural Engineering, Vol. 123, Paper No. 13719, Pg no: 432-439 [7] Singh, M. P., Suarez, L. E., Matheu, E. E., and Maldonado, G. O., (2006), “Seismic Design Forces.II: Flexible Non-structural Components”, Journal of structural engineering © ASCE, October 2006 ,Vol. 132, No. 10. [8] Chaudhuri Samit Ray and Villaverde Roberto, (2008), “Effect of Building Nonlinearity on Seismic Response of Non- structural Components: A Parametric Study”, Journal of structural engineering © ASCE, April 2008, Vol. 134, No.4. [9] Dhanani Suresh L., Patel Sumant B., Mevada Snehal V, (2013), “Seismic Response of Non-Structural Elements”, International Journal of innovations in Engineering and Technology (IJIET), Vol.2. [10] Hart GC and Wong K, “Structural Dynamics for Structural Engineers”, John Wiley &Sons, Inc. [11] Lyan-Ywan Lu (2004). “Predictive control of seismic structures with semi-active friction dampers” earthquake engineering and structural dynamics. [12] Chopra AK., “Dynamics of Structures”, Third Edition, Pearson Publication.