Research Article  Open Access
Jung J. Kim, Mahmoud Reda Taha, "Experimental and Numerical Evaluation of Direct Tension Test for Cylindrical Concrete Specimens", Advances in Civil Engineering, vol. 2014, Article ID 156926, 8 pages, 2014. https://doi.org/10.1155/2014/156926
Experimental and Numerical Evaluation of Direct Tension Test for Cylindrical Concrete Specimens
Abstract
Concrete cracking strength can be defined as the tensile strength of concrete subjected to pure tension stress. However, as it is difficult to apply direct tension load to concrete specimens, concrete cracking is usually quantified by the modulus of rupture for flexural members. In this study, a new direct tension test setup for cylindrical specimens (101.6 mm in diameter and 203.2 mm in height) similar to those used in compression test is developed. Double steel plates are used to obtain uniform stress distributions. Finite element analysis for the proposed test setup is conducted. The uniformity of the stress distribution along the cylindrical specimen is examined and compared with rectangular cross section. Fuzzy image pattern recognition method is used to assess stress uniformity along the specimen. Moreover, the probability of cracking at different locations along the specimen is evaluated using probabilistic finite element analysis. The experimental and numerical results of the cracking location showed that gravity effect on fresh concrete during setting time might affect the distribution of concrete cracking strength along the height of the structural elements.
1. Introduction
Concrete cracking strength is difficult to be quantified and therefore is a source of considerable uncertainty in serviceability prediction. The existence of cracks under service load in reinforced concrete (RC) structures makes it difficult to predict deflections. While cracked concrete is usually assumed to be incapable of carrying tensile stresses, the concrete between adjacent cracks can resist tensile force due to the bond between concrete and steel reinforcement. This is known as tension stiffening effect. Therefore, for the consideration of the deflections of RC structures, concrete cracking strength affects the structural stiffness of the members. Moreover, cracking plays an important role in the durability of RC structures. When concrete cracks, its permeability increases and the processes of concrete deterioration and rebar corrosion get accelerated [1, 2].
For flexural elements, concrete cracking is usually represented by the modulus of rupture [3]. However, in research experiments, the modulus of rupture showed a wide variation [4, 5]. While the modulus of rupture provides a good estimate for cracking strength, researchers showed that accurate serviceability predictions require obtaining the real tensile strength of concrete [6]. Moreover, researchers have argued that, because of the significance of shrinkage on serviceability of RC structures, other cracking criteria, such as the direct or indirect tensile strength of concrete, should be used as evidence of concrete cracking [7]. Three methods are commonly used to measure concrete cracking strength: flexural, splitting, and direct tension test. While the flexural strength test and splitting tensile strength test can be conducted in accordance with the American standard test method (ASTM), ASTM C 78 [8] and ASTM C 496/C 496M [9], respectively, ASTM has no recommendations for direct tension test for concrete, as it is challenging to ensure that uniaxial stress along the specimen is evenly applied.
Several methods have been proposed for direct tension test, such as using friction grip, anchor, and epoxy, to attach the loading machine and concrete specimen. However, all these methods induce secondary stresses that result in an uneven stress application to concrete specimens [10]. To make the applied point load a more evenly distributed load, US Bureau of Reclamation [11] proposes the use of a double plate system for two sizes of diameters of 152.4 mm and 254 mm cylinder specimens. The outer plate is connected to a loading machine, while the inner plate is bonded with the concrete specimen with epoxy. The inner and outer plates are connected to each other by bolts. Recently, this method was modified for the rectangular section of 100 mm by 100 mm and showed acceptable results [10].
In this study, the above method is further developed for cylindrical specimen (101.6 mm in diameter and 203.2 mm in height). Moreover, the stress uniformity of the proposed direct tension test method is evaluated using the finite element method. The stress uniformity along the specimen is compared with the stress uniformity of the direct tension test for rectangular specimen. As experimental results showed that the cracking location was concentrated at the top half of the vertically cured cylindrical specimens, the unit weight of the two broken parts was measured to examine the effect of unit weight on cracking strength and cracking location.
2. Proposed Test Setup
For the cylinder size of 101.6 mm diameter and 203.2 mm height, a double plate system with epoxy adhesive was adopted for the direct tension test setup as shown in Figure 1. The intention is to use cylinders similar to those used to evaluate the compressive strength of concrete in the concrete industry. The inner and outer plates were connected to each other by eight highstrength bolts. Tension load was applied through ball bearings in order to prevent the developing of bending and torsion stresses in the concrete specimen. The thickness of the inner plate was determined to be 38.1 mm according to the US Army Engineer Research and Development Center (ERDC), CRDC 16492 [12]. It was proposed that the thickness of the end plate should be higher than one third of the diameter of the test specimen. The thickness of the outer plate was chosen as one half of that of the inner plate. The bolting locations of the inner and outer plates were optimized by finite element analysis to get uniform stress distribution. The direct tension test conducted using the proposed test setup is shown in Figure 2.
3. Finite Element Analyses
Linear elastic finite element analyses were performed to investigate the stress distribution along the cylindrical and rectangular specimen, as proposed by others [10]. ANSYS^{®} 7.11 [13] was used for the finite element analyses. The test setups were modeled as 3D solid models. The epoxy, double end plates, and concrete were modeled using SOLID 45 [13], which is a solid cubic element with eight nodes having three degrees of freedom (DOF) for translations about the nodal , , and at each node. The material properties used for finite element analysis are presented in Table 1. The bolt connecting the outer and the inner plates was modeled using LINK 8 [13], threedimensional (3D) uniaxial tensioncompression element with three DOF for translations about the nodal , , and at each node.

The finite element analyses of the test setups for cylindrical and rectangular specimens are conducted. It is important to emphasize that the purpose of numerical modeling is to quantify the uniformity of the stress distribution in the tension specimen and not to examine cracking behavior of the concrete specimen. Therefore, only linear elastic region of concrete constitutive model is used for finite element analyses. Considering the symmetry of the test specimen and loading, a quarter of the specimen’s section and a half of the specimen’s length were modeled. The boundary conditions of the finite element models were adjusted to simulate symmetry conditions. For the finite element model of the cylindrical specimen, 320 solid elements in 8 layers were used to represent the outer steel plate while 640 solid elements in 8 layers were used to represent the inner steel plate. For the finite element model of the rectangular specimen, 400 solid elements in 4 layers were used to represent the outer steel plate while 800 solid elements in 8 layers were used to represent the inner steel plate. Concrete specimens for the cylindrical and rectangular specimens were modeled with 1600 and 2000 solid elements in 20 layers, respectively. The bolts were modeled using 3 line elements with compressive initial strain of 0.1% to model the bolting force that was initially applied when the outer and inner plates were connected. Using these finite element models, stress distributions were obtained to quantify stress uniformity along the concrete specimens.
The relative tensile stress is defined as the ratio of the tensile stress at any point to the average tensile stress calculated as the applied load divided by cross section area. The relative tensile stress is evaluated both at the top of the specimens and along the specimen. This analysis is performed for both cylindrical and rectangular specimens. The results for the cylindrical specimen showed that the relative tensile stresses across the section vary from 0.98 to 1.02 and the variations of stress distributions at the top of the cylinder were within ±2% of the average tensile stress. For the numerical results of the whole cylinder, the relative tensile stresses varied from 0.96 to 1.03 and the variation of stress distribution over the entire cylinder was within ±4% of the average tensile stress. The numerical results for the rectangular section of 101.6 mm by 101.6 mm showed that the relative tensile stresses across the section vary from 0.94 to 1.01, while those of the whole specimen vary from 0.9 to 1.03. The results for the tensile stress distribution at the top of the rectangular specimen of 100 mm by 100 mm agreed with the results reported by Zheng et al. [10].
3.1. Stress Uniformity along the Specimens
Although the significantly low variations of stress for the cylindrical specimen confirmed the uniformity of stress across and along the tension specimen, a method to quantify stress distribution similarity at different heights along the specimen was developed and is presented here. The degrees of similarity between the tensile stress distributions, as produced by the finite element analysis at various cross sections, and the applied tensile stress distribution were quantified. The degree of similarity was determined using principles of fuzzy image pattern recognition [14]. This method is one of the methods to determine the degree of similarity between two images. The method was applied to twodimensional (2D) slices. The similarity for two images that have the same size and number of pixels was calculated by comparing pixel values normalized to the interval . After the images were converted to three monochromatic basic color images in red (R), green (G), and blue (B), the similarity between two pixels was assigned to a pair of pixels in three monochromatic images according to the difference of pixel values according to Tolt and Kalaykov [15] and Su et al. [16] such as where and are the pixel values for the compared two figures and . is the pixel similarity value that represents the degree of similarity of two pixel values given a threshold . The advantage of such similarity measure is attributed to its ability to credit a degree of similarity between any two pixels with absolute difference less than . By taking the arithmetic mean of the similarity values for the monochromatic image pairs in R, G, and B, three scalar similarity values that correspond to R, G, and B were obtained. The similarity of the two images was identified by the arithmetic mean of those three similarity values.
Forty images representing the stress contours of 20 layers for each specimen spread at 5.1 mm were generated by the finite element analysis and were used to calculate the similarity of stress distributions along the cylindrical and rectangular specimens. The similarity between the tensile stress distributions at various cross sections is presented in Figure 3 along the specimen. By taking the arithmetic mean of the similarity values along the specimen, the overall similarity of the stress distribution was calculated as 0.933 and 0.921 for the circular specimen and the rectangular specimen, respectively. Given the similarity curves shown in Figure 3 and the mean similarity values, the stresses produced in the cylindrical specimen were more uniform than those of the rectangular specimen.
4. Experimental Methods
Three concrete mixtures with target compressive strengths of 25, 40, and 55 MPa were considered. Three batches of the concrete mixes were made for each target compressive strength case. Nine 101.6 mm in diameter and 203.2 mm in height cylinders and three 101.6 mm × 101.6 mm × 355.6 mm prisms were prepared from each batch of concrete mixture. Ordinary Portland cement and silica fume were used as cementing materials. The maximum size of the coarse aggregate was 10 mm. The particle distributions of the coarse and fine aggregates are presented in Figure 4. The slump of the concrete mixes was maintained between 50.8 and 69.9 mm. The mixture proportions of the concrete mixes are presented in Table 2. The proposed mix was selected to allow comparison of the experimental results of the new proposed test with those published by Zheng et al. [10].

All 9 cylinders and 3 prisms were demolded after one day of casting and left to cure in water until the day of the test. However, 3 cylinders, which were used for direct tension tests, were taken out of the water one day prior to testing. After grinding both sides of each specimen, the specimens were dried for 12 hours and adhered to the steel plates with epoxy, as shown schematically in Figure 1. The epoxy was left for 12 hours to dry to improve bond quality between the concrete specimen and the steel plate in the test setup. The compressive strength test, flexural strength test, and splitting tensile strength test were conducted in accordance with the ASTM C 39/C 39M [17], C 78 [8], and C 496/C 496M [9], respectively. The results are presented in Table 3. The flexural cracking strength of 101.6 mm × 101.6 mm × 355.6 mm prism, splitting cracking strength of cylinder specimens (101.6 mm in diameter and 203.2 mm in height), and direct tensile cracking strength of cylinder specimens (101.6 mm in diameter and 203.2 mm in height) were plotted against the corresponding compressive strength of cylinder specimens (101.6 mm in diameter and 203.2 mm in height) in Figure 5.

For the tests results, the relation between cracking strengths and the corresponding compressive strength was determined in this study based on the assumption that the cracking strength has linear relation with the two third (2/3) power of the corresponding compressive strength as reported by CEBFIP MC90 [18]. Regression analysis was performed and the following relations ((2) to (4)) were obtained: where , , , and are the flexural tensile strength, splitting tensile strength, direct tensile strength, and compressive strength, respectively. Moreover, test results of cracking strengths were also fitted using regression analysis with the assumption that they have linear relation to the square root of the compressive strength after ACI 31811 [3]. This analysis results in the following equations: The relationship between cracking strengths in this study will be It is important to note that the direct tensile strength of concrete in (7) is less than half the value proposed by ACI 31811 [3]. While ACI 31811 [3] proposes using the modulus of rupture, the use of tensile strength to express cracking has been recommended by many researchers [6, 19]. The proposed tension test should enable a cracking strength limit by ACI 31811 [3] lower than current limits obtained from the modulus of rupture experiments. It is also noticeable that the regression results for flexural strength test in (2) and (5) lie between the minimum and the average of the regression results reported by Légeron and Paultre [20]. Moreover, the cracking strength models proposed by CEBFIP MC90 [18] and ACI 31811 [3] lie between the regression results of splitting and the flexural strengths.
5. Cracking Location
Although uniform stress was developed in the concrete specimen subjected to tension by the proposed test setup, the cracking failure location in concrete is difficult to predict due to the inherent variations in concrete microstructures. The numerical analysis of the concrete specimen subject to tension shows that uniform stress was developed along the specimen with the assumption that material distribution is homogeneous and the response is linear elastic. If concrete has been properly placed and no variation in the unit weight of concrete along the specimen takes place, the cracking location in the proposed direct tension test is expected to be uniformly distributed along the specimen (i.e., cracking can take place at any location along the specimen). However, direct tension test results of 27 specimens (results in Table 3) by the proposed test setup showed that the cracking location was frequently concentrated in the top onethird of the specimen as shown in Figure 6. Statistical analysis of cracking location proved to be significantly different from mid height. This observation can be attributed to variation of the unit weight of concrete along the specimen. The increase in unit weight towards the bottom is a wellknown phenomenon due to higher consolidation with gravity at the bottom than at the top of the specimen [21].
To confirm this hypothesis, the unit weights of the two broken parts of all specimens tested by the direct tension test were measured. These measured unit weights were plotted according to the distance from the top of the specimen to the center of the measured parts as shown in Figure 7. A linear relationship between the unit weight and the distance from the top of the specimen in mm is determined as By considering the modulus of elasticity computational model that incorporates the unit weight [3], the modulus of elasticity variation along the specimen is calculated as With the distribution of modulus of elasticity along the specimen, another set of finite element analyses was conducted. Here, the cylinder was modeled in full height, but a quarter of the section was considered for symmetry conditions. The concrete cylinder was divided into 40 layers and the modulus of elasticity of each layer was calculated using (9) and (10). From the stress distribution along the cylindrical specimen, the maximum stress distribution along the specimen was obtained. By assuming that the maximum tensile stress at each layer is normally distributed, the probability of cracking at each layer can be calculated. As the maximum stress distribution at each layer is independent of that at other’s layer, the probability of cracking at each layer can be calculated as where is the probability density function (PDF) of the maximum stress at a layer . However, computation of the probability of cracking requires defining the tensile strength distribution along the specimen. Two methods were considered here. First, we consider the tensile strength variation along the specimen with respect to specimen unit weight according to ACI 209R92 [22] described as Second, the tensile strength variation can be derived by considering the correlation between cracking strength and modulus of elasticity, which is conventionally accepted to be fully correlated. Therefore, the tensile strength variation along the specimen can be determined by modifying (7) to vary linearly with the modulus of elasticity as where is the modulus of elasticity at the center of the specimen chosen to represent the mean modulus of elasticity of the whole specimen. By defining the tensile strength variation using (12) or (13), the probability of cracking integration in (11) can be computed using the Monte Carlo simulation [23] as where and are the cracking strength evaluated at the middle of the th and th layers using (12) or (13), respectively. The probabilities of cracking along the specimen were calculated using (14) by considering sampling iterations for each layer with the coefficient of variation (COV) of the maximum stress taken as 10%.
For two models of tensile strength variation using (12) or (13), the probabilities of cracking along the specimen are presented in Figures 8(a) and 8(b), respectively. The experimental observations of the cracking location in direct tension tests as shown in Figure 6 met the probabilistic prediction confirming the hypothesis of the significance of unit weight variation on cracking location. The probabilistic prediction using the linear variation of the tensile strength with respect to the modulus of elasticity (13) was capable of meeting the experimental observations better than that using the variation proposed by ACI 209R92 model [22] (12). The experimental and probabilistic prediction results of the cracking location seem to be caused by the effect of gravity on fresh concrete during setting time. Therefore, this might be correlated with the properties of fresh concrete. This effect can be exaggerated for relatively deep beams or slabs. In other words, cracking strengths at the top of a structural element would be less than what is predicted by using current design codes. Such variation in concrete properties was observed in bond strength with steel reinforcement [24] and is addressed in development length models by ACI design code [3]. Therefore, when the negative moment is acting on top regions of concrete structural elements, a reduced cracking strength might be considered for conservative serviceability calculations. Further research investigations are needed to confirm the effect of gravity on cracking strength distribution of concrete while considering the significance of aggregate volume fraction, size, and shape.
(a)
(b)
6. Conclusions
A new test setup of direct tension test for cylindrical concrete specimen (101.6 mm in diameter and 203.2 mm in height) is proposed. Experimental and numerical methods are used to support the proposed test setup. The stress uniformity along the specimen is examined using the finite element method aided by a fuzzy image pattern recognition algorithm. The unit weights distribution along cylindrical concrete specimen (101.6 mm in diameter and 203.2 mm in height) was determined. Measurements confirmed the increase in unit weight towards the bottom of the specimens. Distribution of unit weight is shown to significantly affect the probability of cracking along the tension specimens. The probabilities of cracking along the specimen were also calculated using Monte Carlo simulation. The probabilistic prediction results agree with the experimental observations confirming that cracking location in direct tension tests is a function of unit weight distribution along the specimen.
Notations
:  Images that have the same size and number of pixels 
:  Modulus of elasticity at in concrete specimen 
:  Compressive strength of concrete 
:  The maximum stress at th and th layer in finite element model 
:  Flexural strength of concrete (modulus of rupture) 
:  Splitting tensile strength of concrete 
:  Direct tensile strength of concrete 
:  Direct tensile strength at in concrete specimen 
:  th and th layer in finite element model 
:  Pixel values for the two figures and 
:  The number of sampling cases that satisfy the condition in brackets 
:  Total sampling numbers 
:  Probability of cracking of th layer 
:  Probability density function (PDF) of 
:  Unit weight at in concrete specimen 
:  Distance from the top of concrete specimen 
:  Threshold of similarity 
:  Pixel similarity. 
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
Acknowledgments
The first author would like to acknowledge the National Research Foundation (NRF) Grant funded by the Korean government (MOE) (no. 2013R1A1A2062784). The financial support to the second author by the Defense Threat Reduction Agency (DTRA) is also acknowledged.
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Copyright
Copyright © 2014 Jung J. Kim and Mahmoud Reda Taha. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.