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Transcript of FINITE ELEMENT MODELLING OF SELF COMPACTING CONCRETE BEAMS WITH DIFFERENT COVERS SUBJECTED TO...
International J.of Multidispl.Research & Advcs. in Engg.(IJMRAE), ISSN 0975-7074, Vol. 4, No. I (January 2012), pp. 207-224
FINITE ELEMENT MODELLING OF SELF COMPACTING CONCRETE BEAMS WITH DIFFERENT COVERS SUBJECTED
TO THERMAL LOADS
ANAND. N, PRINCE ARULRAJ. G AND XAVIER OLI ELAVAN. P
Abstract
Fire resistance of structures is an important safety aspect which is to be considered in the design of
buildings. The resistance of materials to fire has been studied by few researchers in the past. The
behavior of concrete subjected to higher temperature is not yet completely understood. The Indian
standard for plain and reinforced cement concrete IS 456:2000 has a clause for fire resistance. As per
this clause, fire resistance is a function of cover to the reinforcement. The fire resistance depends on
many other parameters such as grade of concrete, grade of steel, density of concrete etc. Self
compacting concrete has been recently accepted as a promising material that can be used in structural
elements with congested reinforcement. An attempt has been made in this study to understand the
thermal behaviour of self compacting concrete beams with different covers for various heating
conditions. During the present study, the concrete beams were analysed under temperature loads for
deflection, stresses and strain using the software ANSYS 11. Since, the behaviour of concrete is non-
linear; the non-linear behaviour properties are incorporated in the model and the model is solved using
a coupled thermal structural analysis method. Meshing has been done using an optimized modeling
procedure where every element is created and placed in position so that consistent support conditions
and loading points can be maintained. Reduction of strength and increase in deflection values were
observed when temperature loads were introduced in the model geometry. Increasing the cover
resulted in excessive deflection which can be interpreted as spalling in real cases.
---------------------------------------- Keywords : Furnace, Cover, SCC, Room temperature, Deflection, Peak load
© http: //www.ascent-journals.com
ANAND. N, PRINCE ARULRAJ. G AND XAVIER OLI ELAVAN. P 208
1. INTRODUCTION
The fire safety of any building depends to a great extent on its fire resistance, which in turn
depends on the combustibility and fire resistance of its main structural elements. The
strength of the concrete and steel will decrease as the temperature increases. When the
strength of the steel at an elevated temperature reduces to that of the ultimate stress in the
steel, flexural collapse will occur. The study of the behavior of concrete at elevated
temperature assumes great importance in recent times because the accumulated annual loss
of life and property due to fire is comparable to the loss caused by earthquakes and cyclones.
This necessitates development of new codes for fire-resistant design which can be achieved
only through extensive studies on the structural behavior of concrete under high temperature
conditions. Concrete protects the steel inside against the harmful effects of the external
environment. One of the most important of these effects is high temperature. Concrete cover
plays a major role in protecting the reinforcement against high temperature. The choice of
finite element modeling for the purpose of this study is mainly based on the limitations of the
experimental investigations such as cost of the experimental setup, limitations in casting
large specimens, risks involved in handling heated specimens and the prolonged time
necessary to carry out investigations. These limitations and risks are eradicated by use of the
software ANSYS which has been accepted and widely used for such research investigations.
Ansys modeling enables to carry out a detailed study of various cases in a short period of
time, provided, the model is validated with the help of few experimental investigations.
2. REVIEW OF LITERATURE
El-Hawary et al (1997) investigated the effect of fire exposure time and the concrete cover
thickness on the behaviour of R.C. beams subjected to fire in shear zone and cooled by
water. Eight reinforced concrete beams of size 180 x 20 x 12 cm were investigated. The
beams were divided into two groups. Group (1) consisted of four beams with a cover
thickness of 2 cm and group (2) consisted of four beams with a cover thickness of 4 cm.
FINITE ELEMENT MODELLING OF SELF COMPACTING… 209
Each group was subjected to a temperature of 650°C for different periods of time, i.e. 0, 30,
60. 120 min. The compressive strengths of concrete beams were determined nondestructively
using a Schmidt hammer the next day after exposure to fire. Then the beams were tested by
applying two transverse loads incrementally. Strains and deformations were measured at
each load increment. Cracking loads, crack propagation and ultimate loads were recorded for
each beam. The behaviour of the beams exposed to fire in the shear zone were found to be
highly affected by the fire exposure time and the change of the cover thickness.
Xudong Shi et al (2004) carried out an experimental investigation on flexural members
exposed to fire with different concrete cover (CC) thickness (10–30 mm). Investigation was
carried out to determine the influence of the CC on the fire resistance of reinforced concrete
flexural members. Fire load was applied through the bottom and the side faces. From the test
results, it was found that the bottom CC had significant influence on the fire resistance
however the extent of this influence decreased with an increase in the CC thickness. Thus, it
is improper to excessively increase the bottom CC thickness to improve fire resistance. The
lateral CC was found to have insignificant effect on the fire resistance compared to the
bottom CC. A concept of the equivalent CC thickness is proposed in this paper to predict the
effect of the CC on the flexural capacity of reinforced concrete members exposed to fire.
Esref Unluoglu et al (2007) investigated the mechanical properties of structural
reinforcement steel after the exposure to high temperatures. Plain steel, reinforcing steel bars
embedded in mortar and plain mortar specimens were prepared and exposed to 20, 100, 200,
300, 500, 800 and 950 °C temperature for 3 h individually. Deformed steel bars with
diameters of 10, 16 and 20mm were used during the study. Tensile strength of the
reinforcements taken from cooled specimens, variations in the yield strength, ultimate
strength were determined. A cover of 25 mm was found to give protection against
temperature up to 500°C. However, when this temperature exceeded, the reinforcing steel
was found to loss its strength. It was observed that 25 mm cover thickness was not sufficient
to protect the mechanical properties of reinforcing steel when exposed to temperatures over
ANAND. N, PRINCE ARULRAJ. G AND XAVIER OLI ELAVAN. P 210
500°C. Considering the reports that, temperatures during fire accidents could reach a value
as high as 1093°C, adequate concrete cover thickness has to be provided to protect the
reinforcements.
Ilker Bekir Topcu et al (2011) studied the changes in the mechanical properties of the
reinforcement steels having covers in the range 3cm to 5cm inside the mortar specimens
after exposure to high temperatures. In order to ensure covers in the range 3cm to 5cm, 76 ×
76 × 310 and 116 × 116 × 350 mm sized reinforced mortar specimen were prepared. These
reinforced mortar specimens were exposed to 20, 100, 200, 300, 500 and 800°C
temperatures. After the exposure, the steel rods were taken out of these mortar specimen and
the mechanical properties were determined. Stress–strain curves of the steel bars exposed to
several temperatures were drawn. The yield and ultimate strengths of the steel bars were also
determined. The results of the study have shown that the larger the covers resulted in better
protection of steel bars against high temperatures.
3. ESTIMATION OF THE INPUT PARAMETERS
In order to model the reinforced self compacting concrete specimens subjected to elevated
temperature, stress strain relationship for self compacting concrete and time temperature
graphs are to be given as input in the Ansys model. Self compacting concrete mix of grade
M25 concrete was designed. Cubes and cylinders were cast. Compressive strength and
density of the cubes were found. The cylinders were used to derive the stress-strain
behaviour of SCC using uniaxial compression test. Time-temperature curves were obtained
for the specimens heated inside the electrical furnace using an IR-thermometer for the
following cases.
a. Specimens were kept inside the furnace and heated from room temperature to 9000C
b. Specimens were placed in the furnace after achieving a furnace temperature of 9000C
and the specimens were kept inside the furnace for durations of 30 minutes, 60 minutes
and 90 minutes
FINITE ELEMENT MODELLING OF SELF COMPACTING… 211
Time-temperature relationship for the specimens that are heated from room temperature
to 9000C is shown in Fig 1 and Fig 2 gives the Time-temperature relationship for the
specimens that are kept for 90 minutes at 900°C.
Figure 1: Time-temperature Curve for Specimens Heated from
Room-temperature to 9000C (1173 K)
Figure 2: Time-temperature Curve for Specimens that are kept for
90minutes at 9000C (1173 K)
ANAND. N, PRINCE ARULRAJ. G AND XAVIER OLI ELAVAN. P 212
Similar curves have been drawn for other heating conditions. These time-temperature curves
have been fitted with suitable curves and equations have been derived which were used as
input in the Ansys model. Table 1 gives the details of the relationship between time and
temperature for the various heating conditions.
Table 1: Time-Temperature Equations Adopted for ANSYS Modeling
CONDITION EQUATION
270C to 9000C Temp = 265.6*Time0.2483
90 minutes at 9000C Temp = (66.3*Time) + 940
60 minutes at 9000C Temp = (55.672*Time) + 965
30 minutes at 9000C Temp = (57.193*Time) + 960
4. METHODOLOGY
4.1 Solid65
SOLID65 is used for the 3-D modeling of concrete. This element is capable of cracking in
tension and crushing in compression. The element is defined by eight nodes having three
degrees of freedom at each node such as translations in the nodal x, y, and z directions. The
geometry details of SOLID 65 element is shown in Fig.3
4.2. Solid70
SOLID70 is used for modeling concrete with thermal load. This element has a 3-D thermal
conduction capability. The element has eight nodes with a single degree of freedom,
temperature, at each node. The element is applicable to a 3-D, steady-state or transient
thermal analysis. The element also can compensate for mass transport heat flow from a
constant velocity field. The geometry details of SOLID 70 element are shown in Fig 4.
FINITE ELEMENT MODELLING OF SELF COMPACTING… 213
Figure 3: Geometry of Solid 65 Element
Figure 4: Geometry of Solid 70 Element
ANAND. N, PRINCE ARULRAJ. G AND XAVIER OLI ELAVAN. P 214
4.3. Link 8
LINK8 is used for modeling the rebars. Link 8 is a spar which may be used in a variety of
engineering applications. The 3-D spar element is a uniaxial tension-compression element
with three degrees of freedom at each node: translations in the nodal x, y, and z directions.
The geometry details of LINK 8 element are shown in Fig 5.
Figure 5 : Geometry of Link 8 Element
5. VALIDATION OF ANSYS MODEL
As software packages require to be validated for checking accuracy of results, ANSYS
results need to be validated with experimental results before carrying out detailed analysis.
Validation was done using the results of the experimental investigation carried out by Kumar
A and Kumar V (2003) and Moetaz M. El-Hawary et al (1996)
Table 2 shows the details of the specimen used by Kumar A and Kumar V
Table 2: Salient Features of Test Carried out by Kumar A and Kumar V
Size of the
specimen (m)
Temperature
range Time duration
Time-
temperature
curve
Rate of
heating
Rate of
cooling/
coolant
Beam(3.96x0.2
x0.3)
Furnace
temperature
1hr,1.5hr,2hr,
2.5hr
IS 3809-
1979 -
Natural
air
FINITE ELEMENT MODELLING OF SELF COMPACTING… 215
Table 3 shows the details of the specimen used by Moetaz M. El-Hawary et al et al
Table 3: Salient Features of Test Carried out by Moetaz M. El-Hawary et al
Size of the
specimen
(m)
Temperature
range
Time
duration
Time-
temperature
curve
Rate of
heating
Rate of
cooling/
coolant
Beam
(1.8x0.12
x0.2)
650°C (furnace
temperature)
0, 30min,
60min,
120min
Furnace
temperature
curve
-
Sprayed with
water
immediately
The beams used by Kumar A and Kumar V and the beam used by Moetaz were modeled in
Ansys and the comparison between the results of the experimental investigation and the
Ansys results are given in Table 4 and Table 5.
Table 4: Comparison of Results of the Experimental Investigation of Kumar A & Kumar V with
Ansys Results
Condition Deflection Ultimate Load % of Error
Experi
ment Ansys
Experi
ment Ansys Deflection Load
Units mm mm Tonne Tonne
Reference
specimen 27 28.84 16 17.45 6.82 9.06
Specimen heated
for 60 min as per
IS 3809 & cooled
by air
29 30.54 13 13.97 5.31 7.46
ANAND. N, PRINCE ARULRAJ. G AND XAVIER OLI ELAVAN. P 216
Table 5: Comparison of Results of the Experimental Investigation of El-Hawary et al with
Ansys Results
Condition Deflection Ultimate Load % of Error
Experi
ment Ansys
Experi
ment Ansys
Deflect
ion Load
Units mm mm Tonne Tonne
Reference specimen 6.75 7.11 5.95 6.54 5.33 9.91
Specimen kept in
the furnace at 650°C
for 30 minutes and
cooled by water 9.60 10.54 5.25 5.88 9.79
12.0
From Table 4 and Table 5 it can be seen that the percentage of error between the Ansys
model and the experimental investigation is within the acceptable limits.
6. ANSYS MODELING
Seventeen SCC beams were modeled during the present investigation. The sizes of all beams
were 500x100x100 mm. All beams were reinforced with two number of 6mm diameter
Fe415 rods at top and three number of 6mm diameter Fe415 rods at bottom. The first beam
is a reference specimen. The second and third beams were heated from room temperature to
900°C. The second beam had a cover of 20mm and the third beam had a cover of 25mm.
Both these beams were cooled by air. The fourth and fifth beams were kept at a temperature
of 900°C for 30 minutes. The fourth beam had a cover of 20mm and the fifth beam had a
cover of 25mm. Both these beams were cooled by air. The sixth and seventh beams were
FINITE ELEMENT MODELLING OF SELF COMPACTING… 217
kept at a temperature of 900°C for 60 minutes. The sixth beam had a cover of 20mm and the
seventh beam had a cover of 25mm. Both these beams were cooled by air. The eighth and
ninth beams were kept at a temperature of 900°C for 90 minutes. The eighth beam had a
cover of 20mm and the ninth beam had a cover of 25mm. Both these beams were cooled by
air. The tenth and eleventh beams were heated from room temperature to 900°C. The tenth
beam had a cover of 20mm and the eleventh beam had a cover of 25mm. Both these beams
were cooled by spraying water. The twelfth and thirteenth beams were kept at a temperature
of 900°C for 30 minutes. The twelfth beam had a cover of 20mm and the thirteenth beam
had a cover of 25mm. Both these beams were cooled by spraying water. The fourteenth and
fifteenth beams were kept at a temperature of 900°C for 60 minutes. The fourteenth beam
had a cover of 20mm and the fifteenth beam had a cover of 25mm. Both these beams were
cooled by spraying water. The sixteenth and seventeenth beams were kept at a temperature
of 900°C for 90 minutes. The sixteenth beam had a cover of 20mm and the seventeenth beam
had a cover of 25mm. Both these beams were cooled by spraying water. The load deflection
curves for the SCC beams that are heated from room temperature to 900°C and for the beams
that are kept at a temperature of 900°C for 30, 60 and 90 minutes are shown in Fig. 6, Fig.7,
Fig.8 and Fig.9 respectively. These specimens were cooled by air.
ANAND. N, PRINCE ARULRAJ. G AND XAVIER OLI ELAVAN. P 218
Figure 6: Load-Deflection Curves for Beams Heated from Room Temperature to 9000C and
Cooled by Air
Figure 7: Load-Deflection Curves for Beams Heated for 30 Minutes Under 9000C and Cooled by
Air
FINITE ELEMENT MODELLING OF SELF COMPACTING… 219
Figure 8: Load-Deflection Curves for Beams Heated for 60 Minutes Under 900°C and Cooled by
Air
Figure 9: Load-Deflection Curves for Beams Heated for 90 Minutes Under 9000C and Cooled by
Air
ANAND. N, PRINCE ARULRAJ. G AND XAVIER OLI ELAVAN. P 220
The load deflection curves for the SCC beams that are heated from room temperature to
900°C and for the beams that are kept at a temperature of 900°C for 30, 60 and 90 minutes
are shown in Fig. 10, Fig.11, Fig.12 and Fig.13 respectively. These specimens were cooled
by spraying water.
Figure 10: Load-Deflection Curves for Beams Heated from Room Temperature to 9000C and
Cooled by Spraying Water
Fig. 11: Load-Deflection Curves for Beams Heated for 30 Minutes Under 9000C and Cooled by
Spraying Water
FINITE ELEMENT MODELLING OF SELF COMPACTING… 221
Figure 12: Load-Deflection Curves for Beams Heated for 60 Minutes Under 9000C Cooled by
Spraying Water
Figure 13: Load-Deflection Curves for Beams Heated for 90 Minutes Under 9000C Cooled by
Spraying Water
ANAND. N, PRINCE ARULRAJ. G AND XAVIER OLI ELAVAN. P 222
The comparison of the deflections of the SCC beams that are subjected to elevated
temperatures is given in Table 6.
Table 6: Comparison of Deflection Values of SCC Beams
Type of
specimen
Type of
cooling
Deflection at
peak load for
beams with
20mm cover
Deflection at
peak load for
beams with
25mm cover
% increase
in deflection
Reference 2.769 3.105 12.13
Room temperature to
900°C
Air 2.805 4.153 48.06
30 minutes at 900°C Air 2.861 4.273 49.35
60 minutes at 900°C Air 2.892 4.295 48.51
90 minutes at 900°C Air 2.935 4.331 47.56
Room temperature to
900°C
Water 4.556 4.939 8.41
30 minutes at 900°C Water 2.908 4.428 52.27
60 minutes at 900°C Water 3.116 4.555 46.18
90 minutes at 900°C Water 3.933 4.745 20.64
It is seen from Table 6 that the deflections for the beam with a cover of 25mm are larger than
that for the beam having a cover of 20mm. The larger deflection for the reference specimen
is due to the reduction in the effective depth of beam as a result of larger cover. The reason
for larger deflection for the specimen subjected to elevated temperature may be due to
spalling of concrete and reduction in effective depth. Deflections of water cooled specimens
FINITE ELEMENT MODELLING OF SELF COMPACTING… 223
are more than that of the air cooled specimens. The specimen heated from room temperature
to 900°C has the largest deflection when compared with the reference specimen. The
increase in the deflection for the specimen having a cover of 20mm and heated from room
temperature to 900°C is 64.5% higher than the reference specimen when cooled by water.
The increase in the deflection for the specimen having a cover of 25mm and heated from
room temperature to 900°C is 59.07% higher than the reference specimen when cooled by
water. The specimens which are heated from room temperature to 900°C have largest
deflections. Since it takes nearly 400 minutes for the specimen to reach 900°C from room
temperature, the specimens are exposed to severe conditions for a larger period than the
other specimens. Hence the deflections are more in specimens that are heated from room
temperature to 900°C.
CONCLUSIONS
Initial deflections were observed for the SCC beams subjected to elevated temperatures even
before the introduction of structural loads. The SCC beams with a cover of 25mm heated
from room temperature to 900°C had 49.35% more deflection than that of the SCC beams
with a cover of 20mm when cooled by air. The SCC beams with a cover of 25mm heated
from room temperature to 900°C has 52.27% more deflection than that of the SCC beams
with a cover of 20mm when cooled by spraying water. Higher cover resulted in higher
deflections in all the cases of heating. The increase in deflection may be due to spalling of
concrete cover thus exposing the reinforcement to higher temperature. Improving the cover
will improve the performance of R.C.C elements only up to a certain limit. Beyond this limit,
spalling of concrete will takes place resulting in exposure of reinforcements to higher
temperatures. Since the ratio d’/d (d’-Effective cover, d-Effective depth) will be an important
factor in deciding the effectiveness of cover, the detailed Ansys analysis is further required
to obtain the optimal cover for maximum protection of reinforcement against high
temperature.
ANAND. N, PRINCE ARULRAJ. G AND XAVIER OLI ELAVAN. P 224
REFERENCES
[1] Kumar. A and Kumar. V, “Behaviour of RCC beams after exposure to elevated temperatures”, IE(I) Journal – CV, Vol. 84, November 2003, pp 165-170
[2] El-Hawary. M.M., Ragab. A.M., Abd El-Azim. A and Elibiari. S., “Effect of fire on flexural behaviour of RC beams”, Construction and Building Materials, Vol. 10, No. 2, 1996, pp 147-150
[3] El-Hawary. M.M., Ragab. A.M., Abd El-Azim. A and Elibiari. S., “Effect of fire on shear behaviour of RC beams”, Computers and structures, Vol. 65, No. 2, 1997, pp 281-287
[4] Xudong Shi, Teng-Hooi Tan, Kang-Hai Tan and Zhenhai Guo., “Influence of Concrete Cover on Fire Resistance of Reinforced Concrete Flexural Members”, Journal of Structural Engineering, Vol. 130, No. 8, August 2004, pp 1225-1232
[5] Esref Unluoglu, Ilker Bekir Topcua and Burcak Yalaman, “Concrete cover effect on reinforced concrete bars exposed to high temperatures”, Construction and Building Materials, 21 (2007), pp. 1155–1160
[6] Ilker Bekir Topcu, Ahmet Raif Boga and Abdullah Demir, “Influence of cover thickness on the mechanical properties of steel bar in mortar exposed to high temperatures”, Fire and Materials, Volume 35, Issue 2, March 2011, pp. 93–103
Anand. N
Asst. Professor, School of Civil Engineering, Karunya University, Coimbatore, India Email : [email protected]
Prince Arulraj. G
Prof and Dean of Civil Engineering, SNS College of Technology, Coimbatore, India Email : [email protected]
Xavier Oli Elavan.P
Asst. Professor, Dept of Civil Engineering, Hindustan College of Engineering and Technology, Coimbatore, India Email : [email protected]