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   Application of fiber-reinforced polymer (FRP) composites as a confining material for concrete, for retrofitting of critical structures as well as for the construction of concrete filled FRP-tubes as earthquake-resistant columns in new construction already have 
been popular because of the beauty of FRP for providing greater capacity. The reliable design of these structural members for retrofitting and against earthquake-induced forces necessitates a clear understanding of the stress-strain behavior of FRP-confined concrete 
under load cycles., especially under cyclic axial compression for the seismic retrofit. Although the monotonic axial stress-strain behavior of FRP-confined concrete has been studied extensively over the past two decades, only a few studies have so far investigated the 
behavior of FRP-confined concrete under cyclic axial compression. Besides there have been only few studies done on FRP confined HSC based on limited experimental data which led to some research gaps and questions. This study is primarily aiming at filling 
existing research gaps and proposing ideas for further research. The thorough study of existing stress-strain model of FRP confined concrete has led to number of  significant conclusions including proposals for the further study in that field. 
     Not unlike that of FRP, the popularity of high-strength concrete 
(HSC) in  the construction  industry  has  steadily  increased  during  the 
last two decades.  HSC structural members are known to exhibit brittle 
behavior, which jeopardizes their use in seismically active regions. So 
far  there  are  only  few  articles  for  answering  the  stress-strain 
relationship  of  HSC.  The  behavior  of  FRP-confined  HSC  and  FRP-
confined NSC under monotonic and cyclic axial compression will be 
reviewed  and  compared  based  on  other  researcher’s  articles  for  the 
proposal of further study and filling out of the existing research gaps
     The experimental program done by Togay Ozbakkaloglu and Emre 
Akin was taken as primary source for this study and the results have 
been  analyzed  and  compared  with  the  other  existing  stress-strain 
model.
     The experimental program was consisting of a total of 24 FRP-
confined concrete cylinders with a concrete core diameter of 152.5 mm 
and a height of 305 mm which were manufactured and tested under 
axial  compression.    The  test  parameters  included  the  concrete 
compressive  strength  (NSC  and  HSC),  type  of  FRP  material  (CFRP 
and AFRP), FRP thickness (2 to 6 layers), and loading pattern (axial 
monotonic and axial cyclic). AFRP was used as confinement for both 
NSC and HSC where as CFRP are used for HSC. 
Stress-Strain Behavior of FRP-Confined Normal- and High-Strength Concrete
 under Monotonic and Cyclic Axial Compression
SHARIFUL ISLAM
MS in Civil Engineering, Department of Civil Engineering
University of Toledo
INTRODUCTION
EXPERIMENTAL RESULTS
(OZBAKKALOGLU ET. AL)
ABSTRACT
ACKNOWLEDGEMENT
      I would like to express my deepest gratitude to my instructor 
Dr. Azadeh Parvin for her unwavering support and mentorship 
throughout this project.
CONCLUSION
• The axial cyclic stress-strain model proposed by Lam and 
Teng  (2009)  is  highly  accurate  in  predicting  both  the 
unloading and reloading paths of FRP-confined NSC. The 
model  closely  predicts  the  shapes  of  the  unloading  and 
reloading curves and accurately estimates the plastic strains 
for NSC. 
• When  the  model  is  applied  to  HSC  specimens  of  the 
experimental  program,  on  the  other  hand,  the  model 
predictions  deviate  significantly  from  the  experimental 
results;  this  is  caused  largely  by  the  inaccuracies  in  the 
calculation  of  the  plastic  strains  of  FRP-confined  HSC. 
Plastic strain equation  for HSC was calibrated based on the 
extremely limited experimental data reported by Rousakis 
(2001)  on  CFRP-confined  HSC  and  this  might  be  the 
reasons behind this inaccuracies. 
• The predictions of the cyclic stress-strain model proposed 
by Shao et al. (2006) indicated that this model predicts the 
reloading  paths  reasonably  accurately,  but  consistently 
overestimates  the  residual  plastic  strains  and  does  not 
accurately capture the shape of the unloading paths.
Envelop Curve
          Experimental  program  by  Togay  Ozbakkaloglu  and  Emre 
Akin  shows  that  the  envelope  stress-strain  curves  of  cyclically 
loaded  specimens  closely  follow  the  stress-strain  curves  of  the 
corresponding  monotonically  loaded  specimens  which  was  also 
reported by Lam et al. (2006) and Abbasnia and Ziaadiny (2010).
Unloading and Reloading Paths and the Plastic Strain
     Lam et al. (2006) demonstrated that the relationship between 
unloading strains εun;env and plastic strains εpl was linear for CFRP-
confined  NSC  cylinders  for  0.001≤εun;env≤0.0035  and    εun;env 
≥0.0035.  This  observation  was  then  supported  by  that  of 
Abbasnia  and  Ziaadiny  (2010),  which  was  based  on  an 
experimental  investigation  of  CFRP-confined  NSC  square 
prisms.  The  experimental  results  also  in  agreement  with  the 
previousproposal by other researchers.
     Eq. (1) and (2) were calibrated by Lam and Teng for the 
prediction of plastic strain for NSC and HSC. 
Axial Stress-Strain Behavior
• For the monotonic loading, there is an ascending first branch 
in the stress-strain diagram followed by another ascending or, 
almost flat second branch for NSC whereas, for HSC, there is 
a sudden drop (Strength Softening) at the transition point due 
to the brittle nature of HSC. 
• Higher  compressive  strength  and  ultimate  axial  strain  was 
observed for higher number of load cycles for NSC in case of 
cyclic  loading  which  is  in  harmony  with  other  researchers 
(Rousakis  2001;  Lam  et  al.  2006).  On  the  other  side,  HSC 
didn’t  exhibit  this  behavior  which  is  not  in  agreement  with 
other researchers.
• NSC • HSC
Fig 1. Sample Stress-Strain curve with envelop curve for
monotonic and cyclic loading.
→ (1)
→ (2)
     The plastic strain of NSC calculated from the experimental 
results,  closely  resemblance  with  the  analytical  results  from 
Lam  and  Teng  model  but  plastic  strain  of  HSC  was  greatly 
underestimated by Lam and Teng model. This is because of Eq. 
(2) by Lam and Teng model that predicts a reduction of plastic 
strain  with  increasing  unconfined  compressive  strength.  The 
trend line for  HSC,  based  on  the experimental  data, does not 
change significantly with the unconfined compressive strength.
Fig 2. Comparison of experimentally recorded plastic strains with
predictions of Lam and Teng’s model: (a) AFRP-confined NSC;
(b) AFRP-confined HSC
          In  addition  to  the  studies  cited  previously,  the  model 
proposed by Shao et al. (2006) provides a set of equations for 
the calculation of the plastic strains (Eq. 3  & Eq. 4).
     The plastic strains also overestimated by Shao’s model and 
this shortcoming is caused by the overestimation of Esecu which 
is based on the σun;env∕fo.co ratio.
Fig 3. Comparison of experimentally recorded plastic strains
with predictions of Shao’s model: (a)AFRP-confined NSC;
(b) AFRP-confined HSC.
Effect of Unconfined Compressive Strength
     By comparing samples of same f’lu/f’co, indicate that the 
ultimate  strength  is  lower  for  HSC  than  NSC  under  cyclic 
loading. kε values of HSC are consistently lower than that of 
NSC which suggests that it is strength dependent which was 
also reported by other researchers (Wang,2009;Li,2011).
Effect of FRP Type
     The comparison of the average kε values given in Table 1 
for  the  AFRP-  and  CFRP-confined  HSC  specimens  suggests 
that the type of FRP does not have significant influence on kε. 
This  observation,  however,  is  not  in  agreement  with  the 
findings of on going research by Li (2011) in Ozbakkaloglu’s 
research  group  at  the  University  of  Adelaide.  Li  (2011) 
observed  higher  kε  values  have  for  AFRP-confined  concrete 
compared to CFRP-confined concrete. 
Effect of Loading Pattern
 Strain-reduction factor, kε value does not depend on the load 
cycles according to Ozbakkaloglu et al. so is the hoops strain 
єh,rupt    but Lam et al. 2006 and Demir et al. 2010 proposed an 
observed  increase  in  єh,rupt  with  increase  in  loading/unloading 
PROPOSAL FOR FURTHER STUDY
     Among over 15 design-oriented stress-strain models studied in 
this  project,  none  is  able  to  correctly  predict  the  stress-strain 
behavior of FRP-confined HSC. There is a need for a stress-strain 
model that can accurately predict the behavior of FRP-confined 
HSC, and more work is required to better understand and model 
the  behavior  of  FRP-confined  HSC.  If  this  gaps  can  be  filled, 
FRP-confined  HSC  would  be  promising  in  the  prolific  field  of 
retrofitting.
→ (3)
→ (4)
COMPARISON AND
FINDING EXISTING RESEARCH GAPS
PROJECT-
SPRING_2016
CIVE 6460
Table 1. Test Results of FRP-Confined Concrete Cylinders
(Ozbakkaloglu et al.2012)

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IRJET- Behaviour of CFST Column Element with & without Shear Studs under ...
 

Stress-Strain Behavior of FRP-Confined Concrete under Monotonic and Cyclic Loading

  • 1.    Application of fiber-reinforced polymer (FRP) composites as a confining material for concrete, for retrofitting of critical structures as well as for the construction of concrete filled FRP-tubes as earthquake-resistant columns in new construction already have  been popular because of the beauty of FRP for providing greater capacity. The reliable design of these structural members for retrofitting and against earthquake-induced forces necessitates a clear understanding of the stress-strain behavior of FRP-confined concrete  under load cycles., especially under cyclic axial compression for the seismic retrofit. Although the monotonic axial stress-strain behavior of FRP-confined concrete has been studied extensively over the past two decades, only a few studies have so far investigated the  behavior of FRP-confined concrete under cyclic axial compression. Besides there have been only few studies done on FRP confined HSC based on limited experimental data which led to some research gaps and questions. This study is primarily aiming at filling  existing research gaps and proposing ideas for further research. The thorough study of existing stress-strain model of FRP confined concrete has led to number of  significant conclusions including proposals for the further study in that field.       Not unlike that of FRP, the popularity of high-strength concrete  (HSC) in  the construction  industry  has  steadily  increased  during  the  last two decades.  HSC structural members are known to exhibit brittle  behavior, which jeopardizes their use in seismically active regions. So  far  there  are  only  few  articles  for  answering  the  stress-strain  relationship  of  HSC.  The  behavior  of  FRP-confined  HSC  and  FRP- confined NSC under monotonic and cyclic axial compression will be  reviewed  and  compared  based  on  other  researcher’s  articles  for  the  proposal of further study and filling out of the existing research gaps      The experimental program done by Togay Ozbakkaloglu and Emre  Akin was taken as primary source for this study and the results have  been  analyzed  and  compared  with  the  other  existing  stress-strain  model.      The experimental program was consisting of a total of 24 FRP- confined concrete cylinders with a concrete core diameter of 152.5 mm  and a height of 305 mm which were manufactured and tested under  axial  compression.    The  test  parameters  included  the  concrete  compressive  strength  (NSC  and  HSC),  type  of  FRP  material  (CFRP  and AFRP), FRP thickness (2 to 6 layers), and loading pattern (axial  monotonic and axial cyclic). AFRP was used as confinement for both  NSC and HSC where as CFRP are used for HSC.  Stress-Strain Behavior of FRP-Confined Normal- and High-Strength Concrete  under Monotonic and Cyclic Axial Compression SHARIFUL ISLAM MS in Civil Engineering, Department of Civil Engineering University of Toledo INTRODUCTION EXPERIMENTAL RESULTS (OZBAKKALOGLU ET. AL) ABSTRACT ACKNOWLEDGEMENT       I would like to express my deepest gratitude to my instructor  Dr. Azadeh Parvin for her unwavering support and mentorship  throughout this project. CONCLUSION • The axial cyclic stress-strain model proposed by Lam and  Teng  (2009)  is  highly  accurate  in  predicting  both  the  unloading and reloading paths of FRP-confined NSC. The  model  closely  predicts  the  shapes  of  the  unloading  and  reloading curves and accurately estimates the plastic strains  for NSC.  • When  the  model  is  applied  to  HSC  specimens  of  the  experimental  program,  on  the  other  hand,  the  model  predictions  deviate  significantly  from  the  experimental  results;  this  is  caused  largely  by  the  inaccuracies  in  the  calculation  of  the  plastic  strains  of  FRP-confined  HSC.  Plastic strain equation  for HSC was calibrated based on the  extremely limited experimental data reported by Rousakis  (2001)  on  CFRP-confined  HSC  and  this  might  be  the  reasons behind this inaccuracies.  • The predictions of the cyclic stress-strain model proposed  by Shao et al. (2006) indicated that this model predicts the  reloading  paths  reasonably  accurately,  but  consistently  overestimates  the  residual  plastic  strains  and  does  not  accurately capture the shape of the unloading paths. Envelop Curve           Experimental  program  by  Togay  Ozbakkaloglu  and  Emre  Akin  shows  that  the  envelope  stress-strain  curves  of  cyclically  loaded  specimens  closely  follow  the  stress-strain  curves  of  the  corresponding  monotonically  loaded  specimens  which  was  also  reported by Lam et al. (2006) and Abbasnia and Ziaadiny (2010). Unloading and Reloading Paths and the Plastic Strain      Lam et al. (2006) demonstrated that the relationship between  unloading strains εun;env and plastic strains εpl was linear for CFRP- confined  NSC  cylinders  for  0.001≤εun;env≤0.0035  and    εun;env  ≥0.0035.  This  observation  was  then  supported  by  that  of  Abbasnia  and  Ziaadiny  (2010),  which  was  based  on  an  experimental  investigation  of  CFRP-confined  NSC  square  prisms.  The  experimental  results  also  in  agreement  with  the  previousproposal by other researchers.      Eq. (1) and (2) were calibrated by Lam and Teng for the  prediction of plastic strain for NSC and HSC.  Axial Stress-Strain Behavior • For the monotonic loading, there is an ascending first branch  in the stress-strain diagram followed by another ascending or,  almost flat second branch for NSC whereas, for HSC, there is  a sudden drop (Strength Softening) at the transition point due  to the brittle nature of HSC.  • Higher  compressive  strength  and  ultimate  axial  strain  was  observed for higher number of load cycles for NSC in case of  cyclic  loading  which  is  in  harmony  with  other  researchers  (Rousakis  2001;  Lam  et  al.  2006).  On  the  other  side,  HSC  didn’t  exhibit  this  behavior  which  is  not  in  agreement  with  other researchers. • NSC • HSC Fig 1. Sample Stress-Strain curve with envelop curve for monotonic and cyclic loading. → (1) → (2)      The plastic strain of NSC calculated from the experimental  results,  closely  resemblance  with  the  analytical  results  from  Lam  and  Teng  model  but  plastic  strain  of  HSC  was  greatly  underestimated by Lam and Teng model. This is because of Eq.  (2) by Lam and Teng model that predicts a reduction of plastic  strain  with  increasing  unconfined  compressive  strength.  The  trend line for  HSC,  based  on  the experimental  data, does not  change significantly with the unconfined compressive strength. Fig 2. Comparison of experimentally recorded plastic strains with predictions of Lam and Teng’s model: (a) AFRP-confined NSC; (b) AFRP-confined HSC           In  addition  to  the  studies  cited  previously,  the  model  proposed by Shao et al. (2006) provides a set of equations for  the calculation of the plastic strains (Eq. 3  & Eq. 4).      The plastic strains also overestimated by Shao’s model and  this shortcoming is caused by the overestimation of Esecu which  is based on the σun;env∕fo.co ratio. Fig 3. Comparison of experimentally recorded plastic strains with predictions of Shao’s model: (a)AFRP-confined NSC; (b) AFRP-confined HSC. Effect of Unconfined Compressive Strength      By comparing samples of same f’lu/f’co, indicate that the  ultimate  strength  is  lower  for  HSC  than  NSC  under  cyclic  loading. kε values of HSC are consistently lower than that of  NSC which suggests that it is strength dependent which was  also reported by other researchers (Wang,2009;Li,2011). Effect of FRP Type      The comparison of the average kε values given in Table 1  for  the  AFRP-  and  CFRP-confined  HSC  specimens  suggests  that the type of FRP does not have significant influence on kε.  This  observation,  however,  is  not  in  agreement  with  the  findings of on going research by Li (2011) in Ozbakkaloglu’s  research  group  at  the  University  of  Adelaide.  Li  (2011)  observed  higher  kε  values  have  for  AFRP-confined  concrete  compared to CFRP-confined concrete.  Effect of Loading Pattern  Strain-reduction factor, kε value does not depend on the load  cycles according to Ozbakkaloglu et al. so is the hoops strain  єh,rupt    but Lam et al. 2006 and Demir et al. 2010 proposed an  observed  increase  in  єh,rupt  with  increase  in  loading/unloading  PROPOSAL FOR FURTHER STUDY      Among over 15 design-oriented stress-strain models studied in  this  project,  none  is  able  to  correctly  predict  the  stress-strain  behavior of FRP-confined HSC. There is a need for a stress-strain  model that can accurately predict the behavior of FRP-confined  HSC, and more work is required to better understand and model  the  behavior  of  FRP-confined  HSC.  If  this  gaps  can  be  filled,  FRP-confined  HSC  would  be  promising  in  the  prolific  field  of  retrofitting. → (3) → (4) COMPARISON AND FINDING EXISTING RESEARCH GAPS PROJECT- SPRING_2016 CIVE 6460 Table 1. Test Results of FRP-Confined Concrete Cylinders (Ozbakkaloglu et al.2012)