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ACEEE Int. J. on Transportation and Urban Development, Vol. 01, No. 01, Apr 2011

Retrofitting of Masonry Buildings by Base Isolation
Radhikesh P. Nanda1, Pankaj Agarwal2, and Manish Shrikhande2
1

NIT Durgapur, Department of Civil Engineering, Durgapur, India,
Email: rpnanda2002@yahoo.co.in
2
IIT Roorkee, Department of Earthquake Engineering,Roorkee, India
E-mail: {panagfeq/mshrifeq}@iitr.ernet.in
Abstract- Seismic response of masonry buildings retrofitted
using base isolation technique is investigated. The concept of
seismic isolation is applied here by separating the super
structure from the foundation at plinth level by a sliding
earthquake energy reducing friction layer in the form of green
marble/geosynthetic. The dynamic interface property of the
sliding couple has been investigated. In order to investigate
the effectiveness of base isolation the response of the sliding
system is obtained numerically by solving the governing
equations of motion under under synthetically generated IS:
1893, 2002, spectrum compatible accelerogram corresponding
to most severe seismic zone of India (PGA=0.36g) and compared
with the corresponding fixed base structure. It is observed that
50% reduction in maximum roof acceleration for the base
isolated structure in comparison to the maximum roof
acceleration of conventional structures limiting the
earthquake energy transmission to super structure during
strong earthquake, leading lesser damage of masonry
buildings in earthquake prone area and can be used as a low
cost base isolation for earthquake hazard mitigation

Figure 1. Construction detail for P-F isolation system in brick
wall of a brick masonry building

The main concept of base isolation consists of
decoupling the super structure at its base i.e. plinth level
from the damaging effect of horizontal component of induced
ground motion. To achieve this, a smooth layer is introduced
at plinth level, on which the super structure simply rests and
is free to slide except for friction resistance. Thus, leading to
mechanisms such as:
 Friction allowing some parts to slide relative to other.
 There is a limitation of transfer of seismic input
energy to structure.
 Energy dissipation takes place due to coulomb
friction
Arya[1] Qamaruddin et al. [4], proposed a sliding joint
concept which consists of decoupling the building at the
plinth level, by providing a smooth finished layer of cement
sand mortar above which mobil oil was applied. Feasibility
study of this concept had been tested sliding brick building
models with different sliding layer materials, namely, graphite
powder, dry sand, and wet sand.The cracking observed in
sliding specimens had been much less than in conventionally
strengthened specimens. A similar P-F isolation system had
been proposed by Chinese group (Li [3]) with specially
screened sand layer in between terrazzo plate. The
effectiveness of isolation system was tested by shake table
test. It was confirmed that the sliding begins when input
acceleration exceeds a certain level, depending upon the
coefficient of friction value of the sliding layer. Lou et al. [7]
have experimented with low friction materials as sliding joints
to ensure building safety during strong earthquakes. Several
brick with and without sliding joint were tested under lateral
loads with simulated dead load. The walls with sliding joints

Index Terms- Earthquake hazard mitigation, masonry
buildings, Geosynthetic, Pure friction base isolation

I. INTRODUCTION
Masonry construction is the most popular and
suitable for low cost housing purposes in almost all
developing countries. These buildings are seldom designed
against earthquake forces and are prone to collapse during
earthquake. Retrofitting is one of the emerging technologies
to overcome these deficit buildings to make them strong
enough to mitigate the impact of earthquake hazards. Base
isolation is one of the retrofitting techniques used widely
over last 4-5 decades. Out of several base isolation devices
the pure friction (P-F) base isolation system is the simplest
and is ideally suited for use in low-cost masonry buildings.
Attempt has made to apply a sliding earthquake energy
reducing friction layer in the form of green marble/
geosynthetic sliding couples which are easily available in
the Indian market cheaply and can be easily bonded to
building materials has been placed at the plinth level as shown
in Fig.1.

© 2011 ACEEE

DOI: 01.IJTUD.01.01.37

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ACEEE Int. J. on Transportation and Urban Development, Vol. 01, No. 01, Apr 2011
were observed to slide at a lateral force amplitude 50% of the
lateral force at which cracking begins in wall without sliding
joint.The effectiveness of non-woven geotextile-smooth
marble sliding interface as a frictional base isolation system
for masonry building was studied by nanda et al. [5] with the
help of experimental and analytical studies. During simulated
earthquake tests on shake table, a 65% reduction in the
maximum acceleration response at the roof level of building
on sliding base was observed in comparison with the response
of a similar fixed base building.
It had been observed that response of structure by
P-F system strongly dependent upon friction coefficient of
the sliding couple. The lower the friction coefficient lower is
response acceleration and the base shear force. There is no
restoring force provided by any type of external horizontal
spring or damping elements. Lack of additional damping
element causes sliding displacement at isolation levels.
Special attention has to be considered to keep these
displacements within manageable limits However lower
frictional coefficient leads to larger sliding displacement. So
a usable coefficient value has been empirically stated from
0.05 to 0.15 (Nikolic-Brzev [6]). The sliding materials should
be, durable, economically available and can be constructed
without any complication. Previous investigations reveals
that Teflon (PTFE) sliding against stainless steel gives very
low friction value in the most desirable range ie.0.05 to 0.15.
For this reason Teflon has been utilized widely for more than
30 years in seismic isolator for bridges.
However, bonding steel sheets continuously over
concrete course is very much expensive and leads to
construction complication. Graphite, grease, screened sand,
dry and weight sand (see, e.g., Arya [1], Li [3], Lou et al. [7]),
are good alternate but they cannot be used for a long term as
grease can be contaminated by debris, dirt etc., graphite can
be affected by chemical and sand gets crushed after the shock
which will increase the frictional characteristics. Thus there
is a need for search for alternate interface materials which
may be easily available, economically viable and can be used
with lesser complications. The dynamic interface properties
of these materials are being investigated and used in
mathematical model for obtaining the seismic response of
single story masonry buildings.

The building material is assumed to be elastic. Its
stiffness is computed by considering bending as well as shear
deformation in the wall elements. It is assumed that the sliding
displacement between the contact surfaces can occur without
overturning or tilting.
A. Non sliding:


M t ( g  t )  Cxt  Kxt  0
x x
B. Sliding:
Top mass-


M t ( g  b  t )  Cxt  Kxt  0
x x x
Bottom mass-

II. ANALYTICAL MODELLING
The non sliding conditioned is determined when
the horizontal inertia force does not exceed the opposing
friction force, i.e.

The building is idealized as two degree of freedom discrete
lumped mass model. The spring (K) and damping action (C)
in the system is assumed to be provided by the wall elements.
The mass of the roof and one half height of the wall is lumped
at the top (Mt) while the remaining half of the wall and the
bond beam mass is lumped at base (Mb). The lower mass is
assumed to rest on a plane with dry frictional damping to
permit sliding of the system. Let the ground acceleration be


Cxt  Kxt  M b ( g  b )   ( M t  M b ) g
x x
As long as the force, that causes sliding exceeds the
frictional resistance the bottom mass moves with the base
and the system acts as a single degree of freedom system. As
soon as the force acting at the base exceeds the maximum
static friction bottom mass begins to slide and after sliding
begins it can cease at any instant of time when non slip
condition reached. Hence at any instant response of the
building can be obtained by solving the two simultaneous

x
denoted by g ; xt and xb represent t he relative
displacement of top mass with respect to bottom mass and
relative displacement of the bottom mass with respect to
ground respectively.
© 2011 ACEEE

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45
ACEEE Int. J. on Transportation and Urban Development, Vol. 01, No. 01, Apr 2011
observed in the coefficient of static friction for the range of
normal loads considered. From these tests, the average value
of coefficient of static friction was obtained as 0.11.

equations for sliding case with the non slip condition. These
equations are solved by MATLAB 7.0.1 SIMULINK
environment with ODE4 Rungekutta solver

IV. RESULTS AND DISCUSSION

III. FRICTION TEST

From the friction test the coefficient of friction
between the proposed interfaces lies in the desirable range
i.e. 0.05 to 0.15.The above friction coefficients has been used
in the analytical model. The effect of the ground motion on
the behaviour of geosynthetic/marble isolation system is
investigated analytically by using a synthetic accelerogram
that is compatible with the design spectrum of IS 1893 (Part
1): 2002 corresponding to the level of maximum considered
earthquake in the most severe seismic zone (PGA=0.36g).
Fig.5 represents the ground motion and comparative absolute
acceleration and displacement response for fixed and sliding
single story building of mass ratio (MR) =2, time period 2 sec
and damping 5% critical. In case of fixed building there is
acceleration amplification as compare to ground motion. The
peak absolute acceleration at roof level is 0.8g while 0.4g for
base isolated sliding interfaces i.e. 50% reduction in roof
acceleration.

The experimental set up was as shown in Fig. 3. It
consists of the following components. A mild steel foundation
plate was anchored to the ground by foundation bolts. The
foundation plate was provided in order to provide support to
the shear box. The shear box was kept in between two plates,
namely the bottom plate and the top plate (200mm diameter
and 20mm thick). The lower half of the shear box of 50mm
height was kept over the bottom plate. When a horizontal
load was applied, the bottom plate moved and thus created
shear deformations along the predetermined shear surface
i.e. mid height of the sample. The normal load was applied
through this assembly that consists of a hydraulic jack and a
reaction beam. In order to apply a shear load, an actuator was
used and this was fixed to the bottom plate of the shear box.
The upper half of the shear box was restrained horizontally,
using a beam column arrangement, such that it does not move
when the horizontal load was applied. The large shear box is
circular in shape was designed to accommodate samples of
314.15 square centimeter cross sectional size i.e. sample of 20
cm diameter.

Figure 3. Experimental set up for servo controlled actuator and
sliding samples.

The specimens of 20 cm diameter and 5 cm height
concrete (1:1.5:3 ratio) casted with ground polished smooth
green marble on one side. With some specimens, 2 mm thick
Geosynthetic sheet Polyfelt.TS-50 is pasted by Bond Tite
adhesive. Static tests were planned under strain controlled
conditions. The ramp rate was kept constant at 0.5mm/sec and
the normal load was from 10 kN to 50 kN. Ramp limit was fixed as
25mm. Load and displacement data was obtained from the
load cell and displacement transducer embedded in the
actuator system.The load displacement graph is shown in
Fig.4. The coefficient of static friction from the static test was
obtained as the ratio of the maximum shear force just before
sliding to the normal load. No significant variation was
© 2011 ACEEE

DOI: 01.IJTUD.01.01.37

Figure 5. Absolute acceleration response at roof level for sliding
and fixed model

46
ACEEE Int. J. on Transportation and Urban Development, Vol. 01, No. 01, Apr 2011
From relative displacement response for sliding and
fixed single story building of mass ratio (MR) =2, time period
2 sec and damping 5% critical, (Fig.6) it is found that the
maximum relative sliding displacement is 20 mm which is well
within commonly applied plinth projection of 75mm.

[4] M. Qamaruddin, Rasheeduzzafar, A. S Arya. and B. Chandra,
“Seismic response of masonry buildings with sliding substructure”,
Journal of Structural Engineering, ASCE, vol. 112(9), pp. 20012011,1986.
[5] R. P. Nanda, P. Agarwal and M. Shrikhande, “Frictional base
isolation by geotextiles for brick masonry buildings”, Geosynthetic
International, vol. 17 (1), pp 48-55, 2010.
[6] S. Nikolic-Brzev, “Seismic protection of multi-storey brick
buildings by seismic isolation technique”, Ph.D Thesis, Department
of Earthquake Engineering, University of Roorkee, Roorkee, India,
1993.
[7] Y. Lou, M. Wang and J. Su, “A research of sliding shock absorbing
multistory brick buildings”, Proceedings of Tenth World Conference
on Earthquake Engineering, vol. 4, pp. 2499-2503, 1992.

REFERENCES
[1] A. S. Arya, “Sliding concept for mitigation of earthquake disaster
to masonry buildings”, Proceedings of Eight World Conference on
Earthquake Engineering, San Francisco, vol. 5, pp. 951-958, 1984.
[2] Indian standard: 1983 (Part1): 2002, “Criteria for Earthquake
Resistant Design of Structures”
[3] L. Li, “Base isolation measure for aseismic buildings in china”,
Proceedings of Eight World Conference on Earthquake Engineering,
San Francisco, vol. 6, pp. 791-798, 1984.

© 2011 ACEEE

DOI: 01.IJTUD.01.01.37

47

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Retrofitting of Masonry Buildings by Base Isolation

  • 1. ACEEE Int. J. on Transportation and Urban Development, Vol. 01, No. 01, Apr 2011 Retrofitting of Masonry Buildings by Base Isolation Radhikesh P. Nanda1, Pankaj Agarwal2, and Manish Shrikhande2 1 NIT Durgapur, Department of Civil Engineering, Durgapur, India, Email: rpnanda2002@yahoo.co.in 2 IIT Roorkee, Department of Earthquake Engineering,Roorkee, India E-mail: {panagfeq/mshrifeq}@iitr.ernet.in Abstract- Seismic response of masonry buildings retrofitted using base isolation technique is investigated. The concept of seismic isolation is applied here by separating the super structure from the foundation at plinth level by a sliding earthquake energy reducing friction layer in the form of green marble/geosynthetic. The dynamic interface property of the sliding couple has been investigated. In order to investigate the effectiveness of base isolation the response of the sliding system is obtained numerically by solving the governing equations of motion under under synthetically generated IS: 1893, 2002, spectrum compatible accelerogram corresponding to most severe seismic zone of India (PGA=0.36g) and compared with the corresponding fixed base structure. It is observed that 50% reduction in maximum roof acceleration for the base isolated structure in comparison to the maximum roof acceleration of conventional structures limiting the earthquake energy transmission to super structure during strong earthquake, leading lesser damage of masonry buildings in earthquake prone area and can be used as a low cost base isolation for earthquake hazard mitigation Figure 1. Construction detail for P-F isolation system in brick wall of a brick masonry building The main concept of base isolation consists of decoupling the super structure at its base i.e. plinth level from the damaging effect of horizontal component of induced ground motion. To achieve this, a smooth layer is introduced at plinth level, on which the super structure simply rests and is free to slide except for friction resistance. Thus, leading to mechanisms such as:  Friction allowing some parts to slide relative to other.  There is a limitation of transfer of seismic input energy to structure.  Energy dissipation takes place due to coulomb friction Arya[1] Qamaruddin et al. [4], proposed a sliding joint concept which consists of decoupling the building at the plinth level, by providing a smooth finished layer of cement sand mortar above which mobil oil was applied. Feasibility study of this concept had been tested sliding brick building models with different sliding layer materials, namely, graphite powder, dry sand, and wet sand.The cracking observed in sliding specimens had been much less than in conventionally strengthened specimens. A similar P-F isolation system had been proposed by Chinese group (Li [3]) with specially screened sand layer in between terrazzo plate. The effectiveness of isolation system was tested by shake table test. It was confirmed that the sliding begins when input acceleration exceeds a certain level, depending upon the coefficient of friction value of the sliding layer. Lou et al. [7] have experimented with low friction materials as sliding joints to ensure building safety during strong earthquakes. Several brick with and without sliding joint were tested under lateral loads with simulated dead load. The walls with sliding joints Index Terms- Earthquake hazard mitigation, masonry buildings, Geosynthetic, Pure friction base isolation I. INTRODUCTION Masonry construction is the most popular and suitable for low cost housing purposes in almost all developing countries. These buildings are seldom designed against earthquake forces and are prone to collapse during earthquake. Retrofitting is one of the emerging technologies to overcome these deficit buildings to make them strong enough to mitigate the impact of earthquake hazards. Base isolation is one of the retrofitting techniques used widely over last 4-5 decades. Out of several base isolation devices the pure friction (P-F) base isolation system is the simplest and is ideally suited for use in low-cost masonry buildings. Attempt has made to apply a sliding earthquake energy reducing friction layer in the form of green marble/ geosynthetic sliding couples which are easily available in the Indian market cheaply and can be easily bonded to building materials has been placed at the plinth level as shown in Fig.1. © 2011 ACEEE DOI: 01.IJTUD.01.01.37 44
  • 2. ACEEE Int. J. on Transportation and Urban Development, Vol. 01, No. 01, Apr 2011 were observed to slide at a lateral force amplitude 50% of the lateral force at which cracking begins in wall without sliding joint.The effectiveness of non-woven geotextile-smooth marble sliding interface as a frictional base isolation system for masonry building was studied by nanda et al. [5] with the help of experimental and analytical studies. During simulated earthquake tests on shake table, a 65% reduction in the maximum acceleration response at the roof level of building on sliding base was observed in comparison with the response of a similar fixed base building. It had been observed that response of structure by P-F system strongly dependent upon friction coefficient of the sliding couple. The lower the friction coefficient lower is response acceleration and the base shear force. There is no restoring force provided by any type of external horizontal spring or damping elements. Lack of additional damping element causes sliding displacement at isolation levels. Special attention has to be considered to keep these displacements within manageable limits However lower frictional coefficient leads to larger sliding displacement. So a usable coefficient value has been empirically stated from 0.05 to 0.15 (Nikolic-Brzev [6]). The sliding materials should be, durable, economically available and can be constructed without any complication. Previous investigations reveals that Teflon (PTFE) sliding against stainless steel gives very low friction value in the most desirable range ie.0.05 to 0.15. For this reason Teflon has been utilized widely for more than 30 years in seismic isolator for bridges. However, bonding steel sheets continuously over concrete course is very much expensive and leads to construction complication. Graphite, grease, screened sand, dry and weight sand (see, e.g., Arya [1], Li [3], Lou et al. [7]), are good alternate but they cannot be used for a long term as grease can be contaminated by debris, dirt etc., graphite can be affected by chemical and sand gets crushed after the shock which will increase the frictional characteristics. Thus there is a need for search for alternate interface materials which may be easily available, economically viable and can be used with lesser complications. The dynamic interface properties of these materials are being investigated and used in mathematical model for obtaining the seismic response of single story masonry buildings. The building material is assumed to be elastic. Its stiffness is computed by considering bending as well as shear deformation in the wall elements. It is assumed that the sliding displacement between the contact surfaces can occur without overturning or tilting. A. Non sliding:  M t ( g  t )  Cxt  Kxt  0 x x B. Sliding: Top mass-  M t ( g  b  t )  Cxt  Kxt  0 x x x Bottom mass- II. ANALYTICAL MODELLING The non sliding conditioned is determined when the horizontal inertia force does not exceed the opposing friction force, i.e. The building is idealized as two degree of freedom discrete lumped mass model. The spring (K) and damping action (C) in the system is assumed to be provided by the wall elements. The mass of the roof and one half height of the wall is lumped at the top (Mt) while the remaining half of the wall and the bond beam mass is lumped at base (Mb). The lower mass is assumed to rest on a plane with dry frictional damping to permit sliding of the system. Let the ground acceleration be  Cxt  Kxt  M b ( g  b )   ( M t  M b ) g x x As long as the force, that causes sliding exceeds the frictional resistance the bottom mass moves with the base and the system acts as a single degree of freedom system. As soon as the force acting at the base exceeds the maximum static friction bottom mass begins to slide and after sliding begins it can cease at any instant of time when non slip condition reached. Hence at any instant response of the building can be obtained by solving the two simultaneous x denoted by g ; xt and xb represent t he relative displacement of top mass with respect to bottom mass and relative displacement of the bottom mass with respect to ground respectively. © 2011 ACEEE DOI: 01.IJTUD.01.01.37 45
  • 3. ACEEE Int. J. on Transportation and Urban Development, Vol. 01, No. 01, Apr 2011 observed in the coefficient of static friction for the range of normal loads considered. From these tests, the average value of coefficient of static friction was obtained as 0.11. equations for sliding case with the non slip condition. These equations are solved by MATLAB 7.0.1 SIMULINK environment with ODE4 Rungekutta solver IV. RESULTS AND DISCUSSION III. FRICTION TEST From the friction test the coefficient of friction between the proposed interfaces lies in the desirable range i.e. 0.05 to 0.15.The above friction coefficients has been used in the analytical model. The effect of the ground motion on the behaviour of geosynthetic/marble isolation system is investigated analytically by using a synthetic accelerogram that is compatible with the design spectrum of IS 1893 (Part 1): 2002 corresponding to the level of maximum considered earthquake in the most severe seismic zone (PGA=0.36g). Fig.5 represents the ground motion and comparative absolute acceleration and displacement response for fixed and sliding single story building of mass ratio (MR) =2, time period 2 sec and damping 5% critical. In case of fixed building there is acceleration amplification as compare to ground motion. The peak absolute acceleration at roof level is 0.8g while 0.4g for base isolated sliding interfaces i.e. 50% reduction in roof acceleration. The experimental set up was as shown in Fig. 3. It consists of the following components. A mild steel foundation plate was anchored to the ground by foundation bolts. The foundation plate was provided in order to provide support to the shear box. The shear box was kept in between two plates, namely the bottom plate and the top plate (200mm diameter and 20mm thick). The lower half of the shear box of 50mm height was kept over the bottom plate. When a horizontal load was applied, the bottom plate moved and thus created shear deformations along the predetermined shear surface i.e. mid height of the sample. The normal load was applied through this assembly that consists of a hydraulic jack and a reaction beam. In order to apply a shear load, an actuator was used and this was fixed to the bottom plate of the shear box. The upper half of the shear box was restrained horizontally, using a beam column arrangement, such that it does not move when the horizontal load was applied. The large shear box is circular in shape was designed to accommodate samples of 314.15 square centimeter cross sectional size i.e. sample of 20 cm diameter. Figure 3. Experimental set up for servo controlled actuator and sliding samples. The specimens of 20 cm diameter and 5 cm height concrete (1:1.5:3 ratio) casted with ground polished smooth green marble on one side. With some specimens, 2 mm thick Geosynthetic sheet Polyfelt.TS-50 is pasted by Bond Tite adhesive. Static tests were planned under strain controlled conditions. The ramp rate was kept constant at 0.5mm/sec and the normal load was from 10 kN to 50 kN. Ramp limit was fixed as 25mm. Load and displacement data was obtained from the load cell and displacement transducer embedded in the actuator system.The load displacement graph is shown in Fig.4. The coefficient of static friction from the static test was obtained as the ratio of the maximum shear force just before sliding to the normal load. No significant variation was © 2011 ACEEE DOI: 01.IJTUD.01.01.37 Figure 5. Absolute acceleration response at roof level for sliding and fixed model 46
  • 4. ACEEE Int. J. on Transportation and Urban Development, Vol. 01, No. 01, Apr 2011 From relative displacement response for sliding and fixed single story building of mass ratio (MR) =2, time period 2 sec and damping 5% critical, (Fig.6) it is found that the maximum relative sliding displacement is 20 mm which is well within commonly applied plinth projection of 75mm. [4] M. Qamaruddin, Rasheeduzzafar, A. S Arya. and B. Chandra, “Seismic response of masonry buildings with sliding substructure”, Journal of Structural Engineering, ASCE, vol. 112(9), pp. 20012011,1986. [5] R. P. Nanda, P. Agarwal and M. Shrikhande, “Frictional base isolation by geotextiles for brick masonry buildings”, Geosynthetic International, vol. 17 (1), pp 48-55, 2010. [6] S. Nikolic-Brzev, “Seismic protection of multi-storey brick buildings by seismic isolation technique”, Ph.D Thesis, Department of Earthquake Engineering, University of Roorkee, Roorkee, India, 1993. [7] Y. Lou, M. Wang and J. Su, “A research of sliding shock absorbing multistory brick buildings”, Proceedings of Tenth World Conference on Earthquake Engineering, vol. 4, pp. 2499-2503, 1992. REFERENCES [1] A. S. Arya, “Sliding concept for mitigation of earthquake disaster to masonry buildings”, Proceedings of Eight World Conference on Earthquake Engineering, San Francisco, vol. 5, pp. 951-958, 1984. [2] Indian standard: 1983 (Part1): 2002, “Criteria for Earthquake Resistant Design of Structures” [3] L. Li, “Base isolation measure for aseismic buildings in china”, Proceedings of Eight World Conference on Earthquake Engineering, San Francisco, vol. 6, pp. 791-798, 1984. © 2011 ACEEE DOI: 01.IJTUD.01.01.37 47