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Experimental and Numerical Assessment of Reinforced Concrete Beams with Disturbed Depth
International Journal of Concrete Structures and Materials volume 13, Article number: 55 (2019)
Abstract
This paper investigates numerically and experimentally the performance of reinforced concrete (RC) beam with unequal depths subjected to combined bending and shear. Such beams can geometrically be considered for unleveled reinforced concrete (RC) floor slabbeam system. However, it may generate critical disturbances in stress flow at the reentrant corner (i.e. location of drop in beam depth). This research investigates the use of shear reinforcement and geometric properties to enhance cracking characteristics, yielding, ultimate loadcarrying capacity, and exhibiting ductile failure mode. Ten reinforced concrete (RC) beams were constructed and tested experimentally considering the following key parameters: recess length, depth of smaller beam nib, and amount and layout of shear reinforcement at reentrant corner. Finite element analysis (FEA) with material nonlinearity was conducted in two RC beams that were tested experimentally to validate the computer modelling. The FEA models were then extended to conduct a parametric study to investigate the influence of geometric parameters (beam shape and width) and amount and arrangement of shear reinforcement on the structural response. Results confirmed that geometric properties and ratio of shear reinforcement at the reentrant region significantly affect the behavior of reinforced concrete beam with unequal depths in terms of first cracking, yielding level, ultimate load carrying capacity and mode of failure.
Introduction
Recently, reinforced concrete (RC) beams with constant depth are commonly employed in RC structures. Beams with unequal depth can geometrically be considered to accommodate unleveled floor slab system and to allow for utilities (i.e. pipes and HVAC ducts) to go through the beam depth without increasing floor height. Figure 1a shows a schematic diagram of this beam of depth “t” and length “L” that has a reduced depth, h_{n}, over a length l_{n} (called recess length herein). The length of the beam with smaller depth is called “beam nib” and the region at which the beam depth changes from t to h_{n} is called “reentrant corner” as depicted in Fig. 1a. The presence of abrupt change in beam depth is expected to lead to (i) very critical flow of internal flexural stresses with its peak at the reentrant corner (NagyGyörgy et al. 2012; Sas et al. 2014; Lim et al. 2016) and (ii) significant change in initial cracking, yielding level, ultimate loadcarrying capacity and mode of failure (Kassem 2015; Zhong et al. 2017). Such critical transition zone can be called as disturbed region (Dregion).
Another type of concrete beam with unequal depth is the one used in precast concrete beams and girders at their supports which is referred to as “dappedend beams” (Hawileh et al. 2017). However, such beam configuration is outside the scope of the current research. Few researchers investigated the effect of spantodepth ratio and shear spantodepth ratio on the shear strength of concrete beams including the Dregions and dapped ends (Hu and Wu 2018; Choi et al. 2018; Qeshta et al. 2016; Naik and Kute 2013). Addition of shear reinforcement to intercept the Dregion with excessive tensile stresses added to the ductile failure and ultimate load carrying capacity of the beam (NagrodzkaGodycka and Piotrkowski 2012). Desnerck et al. (2016, 2017) investigated experimentally the impact of the reinforcement layout and amount as well as anchorage zone cracking on the load capacity of RC beams with dapped region, called “halfjoint beams” in their research. They concluded that the arrangement of shear reinforcement in the form of vertical steel bars, Ushape bars and diagonal bars at the dapped end affect the initiation of concrete cracking, yielding of reinforcement and load capacity at this disturbed beam end. Zhong et al. (2017) proposed an evaluation system to assess conveniently the performance of Dregions designed using different strutandtie models. Results showed that reinforcement layout, respect to strutandtie models, can significantly affect mode of failure and ultimate capacity. Aswin et al. (2015) examined experimentally the behavior of dappedend beam failed by excessive shear stresses at the nib area. Using ductile engineered cementitious composite (ECC) at dappedend zone would lead to enhanced shear strength and ductility as demonstrated for composite girder investigated elsewhere (Hamoda et al. 2017; Hossain et al. 2015). Fang et al. (2018) studied experimentally horizontal shear behavior of normal and lightweight concrete composite Tbeam. Fernández et al. (2018) studied experimentally the performance of beams having Dregion designed using fundamentals of strutandtie model. Others (Desnerck et al. 2018; Pradhan et al. 2018; Alam et al. 2017; El Bitouri et al. 2017; Nosheen et al. 2018; Demir et al. 2016; Chiu et al. 2016; Kobielak and Zamiar 2017) investigated experimentally and numerically the shear behavior of reinforced concrete members with various types of reinforcement layout.
Literature review revealed that the structural behavior of reinforced concrete beam with reduced beam depth over a significant portion of the beam span, as depicted in Fig. 1a, is as yet unavailable. Such change in beam depth within the beam span would cause significant flexural stiffness loss and would lead to premature brittle failure at the reentrant corner due to stress concentration and change in beam flexural and shear stiffness. As such, the objective of this research is to investigate the structural response of such beam configuration under increasing static loading to collapse as affected by (i) the ratio between beam depths (h_{n}/t), (ii) recess length/beam span ratio (l_{n}/L), (amount and arrangement of shear reinforcement and the reentrant region, and (vi) change in beam width at the disturbed region. Ten RC beams were constructed and then tested under increasing static loading up to failure. A nonlinear threedimensional finite element analysis (FEA), utilizing an available concrete damage plasticity (CDP) model, was performed in two of the tested beams to expand on the study of key parameters affecting the structural response of beams with abrupt change in its depth within its span. The experimental test results and the numerical modelling are presented for discussion herein in the form of cracking and yielding characteristics, loadcarrying capacity and failure mode. Then, conclusions are drawn regarding improving crack appearance, ductility, and loadcarrying capacity of the studied beams. The outcome of this research will allow designers to better understand the structural performance of such structural elements for practical construction applications, particularly in buildings.
Experimental Study
The experimental testing program included the construction of 10 simplysupported reinforced concrete beams, followed by testing them under static loading to failure. The tested beams were divided into 5 groups with respect to the length of the beam nib, l_{n}, depth of the beam nib, h_{n}, and amount and layout of shear reinforcement at the reentrant corner. In all these beams, the beam width, b, was taken as 100 mm, the overall depth, t, was taken as 200 mm and the beam span, L, was taken as 2100 mm. All beams were subjected to a concentrated load which was applied at 0.33 L to ensure that the reentrant corner and the beam nib are subjected to high shear stresses, leading to failure on that side of the beam. Figure 1a shows beam dimensions and a schematic diagram of the threepoint loading arrangement, while Fig. 1b shows a photo of the beam setup before testing. The following subsections summarize the description of beam groups, materials properties, test setup and test procedure. Table 1 summarize the details of the tested beam groups.
Description of Tested Beam Groups
Figure 2 summarizes the reinforcement details for each of the 10 beams considered in this study. To study few geometric parameters and effect of shear reinforcement on the ultimate capacity and failure modes, the tested beams have similar flexural reinforcement in the form of 2#10 bars in the tension side of the beam and 4#10 bars in the compression side of the beams as depicted in Fig. 2 to ensure tensioncontrol failure based on the size of the beam and the availability of minimum steel bar sizes to conduct such small scale testing. The development length of the tension bars in the beam nib projecting into the beam portion with deeper section was taken 150 mm for all beams as depicted in Fig. 2d.
Beam group (1) consisted of two beams, namely: B0 and B2. Beam B0 was constructed with constant depth of 200 mm, while beam B2 had a nib with depth, h_{n}, of 120 mm (i.e. h_{n}/t = 0.6) and recess length, l_{n}, of 600 mm (i.e. l_{n}/L = 0.3). Figure 2a, b) show dimensions and reinforcement details for beams B0 and B2, respectively. Such group aims at assessing the major difference of ultimate loadcarrying capacity and failure mode observed from the conventional beam B0 and beam B2 with reentrant corner.
Beam group (2) consisted of three beams, namely: B1, B2 and B3. Beams B1 and B3 were identical to beam B2 with respect to geometry and reinforcement except that the recess lengths, l_{n}, were 630, 525, and 315 mm, respectively, leading to l_{n}/L ratios of 0.30, 0.25 and 0.15. Figure 2c, d show dimensions and reinforcement details of beams B1 and B3, respectively. This group was intended to examine the effect of the recess length with reduced depth on the structural behavior of the beam.
Beam group (3) had 3 beams, namely: B1, B4 and B5. Beams B4 and B5 were identical to beam B1 with respect dimensioning and reinforcement, especially the recess length, l_{n}, of 525 m. However, their nib depth, h_{n}, were taken 80, 120 and 160 mm for beams B4, B1 and B5, respectively, leading to h_{n}/l_{n} ratios of 0.15, 0.23 and 0.3. Figure 2e, f show dimensions and reinforcement details for beams B4 and B5, respectively. The main objective of this beam group was to evaluate the effect of nib depth on the beam ultimate capacity and failure mode.
Beam group (4) consisted of 3 beams, namely; B1, B6 and B7. These beams were identical with respect to beam geometry and arrangement and amount of flexural reinforcement. However, the amount of shear reinforcement in each of these beams was different. The amount of stirrups to resist shear force in the beam portion with depth, t, of 200 mm, was taken as 5#8/m, 8#8/m and 5#8/m for beams B1, B6 and B7, respectively, leading to shear reinforcement ratio, V_{sb}%, as 0.50, 0.80 and 0.50, respectively. On the other hand, the amount of stirrups to resist shear force in the beam nib with depth, h_{n}, of 120 mm, was taken as 5#8/m, 5#8/m and 8#8/m for beams B1, B6 and B7, respectively, leading to shear reinforcement ratio in the beam nib, V_{sd}%, as 0.50, 0.50 and 0.80, respectively. Figure 2g, h show dimensions and reinforcement details for beams B6 and B7, respectively. The main objective of this beam group was to evaluate the effect of the amount of stirrups in the beam full depth or in the beam nib on the beam ultimate capacity and failure mode.
Beam group (5) consisted of 3 beams, namely; B1, B8 and B9. These beams were identical with respect to beam geometry and arrangement and amount of flexural reinforcement. However, the amount of shear reinforcement in each of these beams was different. The amount of stirrups to resist shear force in beam B1 was taken 5#8/m, leading to shear reinforcement ratio, V_{sb}%, or V_{sd}% of 0.50. On the other hand, the amount of stirrups to resist shear force in beam B8 increased to 8#8/m as depicted in Fig. 2i, leading to shear reinforcement ratio, V_{sb}% or V_{sd}% of 0.80. To address the effect of local strengthening of the reentrant corner in shear, 2#8 bentup bars were added at 45° angle at the interface between the beam nib and the beam portion with deeper section as depicted in Fig. 2j. This leads to an average shear reinforcement ratio (V_{sb}% or V_{sd}%) of 0.52. The main objective of this beam group was to evaluate the effect of the amount of shear reinforcement when it is kept constant all over the span of the beam.
Material Properties
Normal strength concrete was employed for casting. Such concrete consisted of Ordinary Portland Cement, natural siliceous sand, crushed pink hard limestone with 10 mm maximum nominal size and water, with mix proportions by weight as 1: 2: 3.18. The concrete mix had water cement ratio of 0.53. The average value of concrete compressive strength was about 32.0 MPa, however, average concrete compressive strength for each beam is listed is Table 1. Two types of reinforcing steel bars were used in this study. Deformed steel bars with 10 mm diameter conforming with Grade 369/534 steel was used as tension and compressive reinforcement for flexural resistance. Plain bars of 8 mm diameter conforming with Grade 293/467 steel was used for vertical stirrups and bentup bars as shear reinforcement. Idealized stress–strain curves for concrete in compression and tension used in the finite element analysis (FEA) modelling are shown in Fig. 3a. Steel material stress–strain curves obtained from testing steel coupon tensile testing as well as idealized stress–strain curves adopted for FEA modeling are shown in Fig. 3b.
Test Setup and Test Procedure
After 28 days from casting, each beam was placed, centered and leveled at the support zone as shown in Fig. 1b. All beams rest over hinged support on one side, allowing for rotation with no displacement, while the other support allows for horizontal movement and rotation, simulating roller support. A concentrated load was applied at 0.33 L as depicted in Fig. 1a in order to generate high shear force at the reentrant corner. It should be noted that the distance between the edge of the steel base plate, transferring the applied load to the beam, to the reentrant corner was taken as 100 mm as depicted in Fig. 2b for all tested beams. Electrical strain gauges were installed in selected steel bars as depicted in Fig. 4. Three strain gauges were attached at the solid beam. B0 as depicted in Fig. 4a, while four gauges were mounted on beams with unequal depths as shown in Fig. 4b. One dial gauge of 0.01 mm accuracy was used to record beam vertical deflection at load location as shown in Fig. 1b. The load was applied in 0.2 kN increments up to failure. During each load increment, cracks (if any) were marked and deflection and steel strain readings were recorded. The duration of each increment was about 2 min. Failure was considered attained when the beam could not take further load.
Test Results and Discussion
Figures 5, 6, 7, 8 and 9 shows photos of the crack pattern after failure of each beam. Table 2 provides the experimental findings in the form of cracking load (P_{cr}), and corresponding beam deflection (Δ_{cr}), zone at which first crack appeared, yield load (P_{y}) and first location of bar yield, ultimate load (P_{u}) and corresponding deflection at failure (Δ_{u}) and failure mode for each tested beam. The following subsection discuss the experimental findings in details.
Crack Pattern and Failure Mode
First Group (G1)
For the first group, the first visible hair crack for the control beam B0 (with no nib zone) was flexuralshear appearing at the bottom surface of section at applied load location at about 15.20 kN (34% of ultimate load). As the applied load increased, several flexural and flexuralshear cracks appeared close to the bottom surface of the beam and gradually extended towards its top surface. However, a major diagonal crack appeared at beam middepth at a load of 38 kN (86% of ultimate load). Such crack continued to enlarge at higher loads and propagated towards the top surface close to edge of the loading plate and downward towards the bottom surface close to the supporting plate. Then, sudden concrete crushing occurred at the top surface close to loading plate, as shown in Fig. 5a, causing beam failure at an ultimate load of 44.40 kN in a shearcompression failure mode.
Beam B2 shown Fig. 5b in first group (G1) had the first visible flexural crack at an applied load of about 3.00 kN (19% of ultimate load) initiating from the reentrant corner of the nib zone, as expected. Then, a few cracks grew from the first initial one at a load ranging from about 26% to 58% of the ultimate load. As the applied load increased, a few flexural and shearflexural cracks appeared. These cracks continued to enlarge and propagate from the bottom of the beam towards the top surface of the beam. Just before failure, the flexural major crack formed at reentrant corner propagated towards the compressive side of the beam and spread laterally giving the signs of approaching concrete crushing at the top surface of the beam as depicted in Fig. 5b. The beam could not take an applied load beyond 15.10 kN presenting a pure flexural failure mode at the reentrant corner of the nib region.
Second Group (G2)
The second group (G2) was considered to study the effect of recess length, l_{n}, of 630 mm, 525 mm and 315 mm, for beams B2, B1, and B3, respectively (i.e. l_{n}/L = 0.3, 0.25 and 0.15, respectively). Beam B1 with a nib lengthtobeam length (l_{n}/L) of 0.25 exhibited the first visible hair crack at the reentrant corner at an applied load of about 3.00 kN (19% of ultimate load). As the load increased, several cracks appeared in the reentrant zone as shown in Fig. 6a. In addition, very few flexural cracks appeared at the bottom surface at section close to loading plate and propagated towards the top of the beam with increase in applied loading. Just before failure, the major crack formed at the reentrant corner became wider propagating upward toward the top surface at an angle leading to shearcompression failure mode at a load of 15.70 kN with signs of concrete crushing at the top fibers.
Figure 6b shows crack pattern for beam B3 with l_{n}/L of 0.15. As expected, the first visible crack appeared at the reentrantcorner of nib zone at an applied load of about 4.30 kN (17% of the ultimate load). As the load increased, several cracks appeared before and after the reentrant corner. These cracks propagated at an angle towards the top surface as well as the direction of the loading plate, leading to sudden concrete crushing in concrete at the top surface of the beam beside the steel loading plate as shown in Fig. 6b. with an ultimate load, P_{u}, of 24.80 kN. The beam could not sustain an applied load beyond 24.8 kN due to shearcompression failure.
By comparing the results of the three beams in this group, one may observe the change in the failure mode from flexural in a beam with longer beam nib (beam B2) to shearcompression failure in a beam with shorter beam nib (beams B1 and B3). Also, it can be observed that the beam load carrying capacity increases with decrease in beam nib length. For example, the beam capacity increased by 64% with decrease of nib length from 630 mm to 315 mm. On the other hand, slight increase in beam capacity (i.e. 2%) when reducing the nib length from 630 to 525 mm. Similar behavior was observed in case of observed cracking load of beams B2, B1 and B3.
Third Group (G3)
The third group (G3) was considered to investigate the change in the depth of the beam nib to the main beam depth on the structural response. In this case, Beams B4, B1 and B5 had the same nib length of 525 mm while the nib depth, h_{n}, was taken as 80, 120 and 160 mm, respectively.
For beam B4 with h_{n} of 80 mm, the first visible crack appeared at the reentrant corner at a load of about 2.60 kN (25% of the ultimate load). As the load increased, several flexuralshear cracks appeared in the beam nib region and propagated towards the top surface of the beam. A sudden concrete crushing occurred at the top surface of the beam between the edge of loading plate and the reentrant corner causing shearcompression failure at a load of 10.40 kN as depicted in Fig. 7a.
For beam B5 with h_{n} of 160 mm, the first visible crack occurred at the reentrant corner at a load of 5.50 kN (31% of ultimate load). The first flexural crack appeared at bottom surface close to the loading location at a load of 9.30 kN (53% of ultimate load). With increase in the applied load, several flexuralshear cracks appeared in the nib zone and propagated towards the steel loading plate direction, leading to sudden concrete crushing at the top surface of the beam between the loading plate and the reentrant corner as shown in Fig. 7b. The beam failed in a shearcompression failure mode at an ultimate load of 21 kN.
By comparing the results of the three beams in this group, one may observe that the increase in the depth of the beam nib compared to the main depth of the beam did not alter the failure mode which was shearcompression failure. However, the beam load carrying capacity increased with increase in beam nib depth, as expected. For example, the beam capacity increased by 51% and 102% with increase of nib depth from 80 mm to 120 mm and 160 mm, respectively. Also, the beam first cracking load increased by 15% and 211% with increase of nib depth from 80 mm to 120 and 160 mm, respectively, as expected.
Fourth Group (G4)
The main purpose of the fourth group G4 was to examine the effect of the amount of stirrups in the beam nib and the beam portion with the main depth of 200 mm on the structural response. In this case, 3 beams (B1, B6 and B7) of equal nib length and depth of 525 mm and 120 mm, respectively, were considered but with different stirrup spacing in each of the beam nib and the main beam portion. Beam B6 was reinforced with rectangular closed stirrups with diameter of 8 mm placed at 200 mm spacing in the main beam portion, while the nib region had the same stirrups at 125 mm spacing. Figure 8a shows the crack pattern of beam B6 after failure. The first crack appeared at the reentrant corner with a load of 3.60 kN (23% of the ultimate load). Also, the first flexural crack was recorded at the bottom surface of loading location at a load of 8.20 kN (53% of ultimate load). As the load increased, several hair cracks were generated and propagated to the top surface of the beam in the region between the reentrant corner and the loading plate. However, no cracks were detected at the nib region as shown in Fig. 8a. The main diagonal shear crack at the reentrant corner propagated to the edge of the loading plate causing slight concrete crushing at an ultimate load of 20.5 kN in a form of shearcompression failure mode.
Beam B7 had stirrup arrangement opposite to that for beam B6. Beam B7 was reinforced with rectangular closed stirrups with diameter of 8 mm placed at 125 mm spacing in the main beam. As shown in Fig. 8b, the first visible crack appeared diagonally at the reentrant corner at a load of 3.20 kN (24% of the ultimate load). In contrast to beam B6, flexural and flexuralshear cracks appeared in both sides of the reentrant corner of Beam B7. Failure of Beam B7 occurred due to sudden concrete crushing at the top surface of the beam beside the loading plate. Perfect shearcompression failure mode was observed at an ultimate load of 19 kN. Comparison between beams B1 and B6 in this group showed that the increase in stirrup amount in the nib region has significant effect in the load carrying capacity (i.e. 31% difference), with the cracking load increased by 20%. Comparison between beams B6 and B7 in this group showed that the increase in stirrup amount in the main beam segment rather that the nib region decreased the load carrying capacity and the cracking load by 8% and 13%, respectively.
Fifth Group (G5)
The last group aimed at studying the effect of shear reinforcement amount when it is maintained the same all over the beam span. Figure 9a shows cracking pattern of the tested beam B8 with stirrup spacing of 125 mm. The first visible crack appeared at the reentrant corner at a load of 4.30 kN (25% of the ultimate load). The first flexural crack remarked at the bottom surface of nib region as well as loading location at a load of 5.50 and 8.20 kN (32% and 48% of the ultimate load) respectively. As the load increased, several flexural cracks appeared and propagated towards the top surface of the beam. the flexural crack at the reentrant corner propagated vertically towards the top surface of the beam, followed by sudden concrete crushing as shown in Fig. 9a. Flexural failure mode was observed at an ultimate load of 21 kN.
Beam B9 was identical to beam B1 with respect to stirrup spacing of 200 mm all over the length of them beam except that 2#8 bentup bars were added at 45° angle at the reentrant corner as depicted in Fig. 2j. In beam B9, the first crack was observed at a load of 5.90 kN (34% of the ultimate load) initiating from reentrant corner. As the applied load increased, other flexural and flexuralshear cracks appeared and propagated towards the top surface of the beam. However, major diagonal shear crack at the reentrant corner zone propagated to the top surface of beam causing sudden concrete crushing, as depicted in Fig. 9b, at an ultimate load of 21.00 kN. The comparison between beams B9 and B8 showed that the number of flexural cracks in beam B8 were almost greater than those observed from other counterparts which may attributed to the presence of augmented closed stirrups along the entire beam span including the nib region. In addition, the failure mode was mainly flexural in contract to the shearcompression failure modes in other beams in this group. Also, one may observe that the increase in stirrup amount increased the ultimate load and the cracking load by 33% and 43%, respectively, when comparing beams B1 and B8.
When comparing beams B1 and B9, it can be observed that the addition of the 2#8 bentup bars at the reentrant corner increased the cracking load and the ultimate load by 97% and 34%. In conclusion, the increase of shear reinforcement delayed the start of flexural cracks and increased the ultimate load capacity in the studies beams.
Load–Deflection Response
Figure 10 summarizes the load–deflection relationship for the tested beams in each group. It should be noted that beam deflection was recorded at the location of the applied load. Table 2 provides the deflection values at cracking load (Δ_{cr}) and ultimate load (Δ_{u}).
As it can be seen in Fig. 10, the all tested groups showed a linear response before the cracking load which was recorded to be between 3.0 and 5.9 kN for the beams with nibs and 15.2 kN for the beam with constant depth. Then, the load–deflection responses were almost linear to the yield load level, and became almost nonlinear afterwards. As expected, the recess length (nib length) appeared to have a significant influence on the deflection values all over the loading history.
For beam group G2, Fig. 10b shows similar deflection response for beams with recess lengths of 630 and 525 mm, with very much less deflection in the beams with 315 mm recess length at the same load level, as expected. Given the increase in ultimate load capacity in beam B3, its ultimate deflection was recorded as 23.75 mm compared to 15.65 and 15.14 mm for beams B2 and B1, respectively.
Figure 10c shows the load–deflection relationship for beam group G3 at which the nib height was the main variable. At the cracking load level, one may observe the increase in cracking load deflection with increase in nib depth. Similar behavior was observed for the ultimate deflection at failure. As depicted in Table 2, it can be observed that although the failure mode of all beams in this group is compressionshear failure, the ultimate deflection increases with the increase in nib depth.
Load–deflection relationship for beam group G4 is shown in Fig. 10d. Since the load–deflection curves overlapped with each other, one may conclude that the change in the amount of shear reinforcement in each of the main beam portion or the beam nib does has insignificant effect on the deflection values at a given load. Similar conclusion is observed in Fig. 10e with the change in the amount of stirrup spacing all over the beam span or with the addition of the bentup bars at the reentrant corner for beam group G5.
Steel Stress–Strain Relationship
Figures 11, 12, 13 and 14 show the loadsteel strain relationship recorded during testing. For each group, loadsteel strain were depicted from four gauges mounted on compressive bar, vertical stirrup, flexural bar and horizontal bar (gauges S1, S2, S3 and S4, respectively, in Fig. 4b). Table 2 shows the load value at which the yield strain first reached and the corresponding location in these bars. Based on the tensile testing of the bar specimens, the yield strain considered in this study is 0.00185 (359 MPa yield stress/200,000 MPa modulus of elasticity = 0.00185 yield strain).
Figure 11 shows the loadsteel strain relationships at recorded locations in the horizontal bar in the beam nib, vertical stirrup close to the reentrant corner, the flexural bar compression bars just at the load location. It can be observed that out of all these bars, yield strain reached in the horizontal bar in the tension side of the nib at the reentrant location, as expected. The yield loads were at 76%, 93% and 90% of the ultimate load for beams B2, B1 and B3, respectively. This confirms the type of failure exhibited in each of these beams. Results show the ductile flexural failure in beams B2 of 630 mm nib length and the brittle shearcompression failure in case of beam B1 and B3 with nib lengths of 525 and 315 mm, respectively. This means that the shorter the nib length, the more brittle the failure mode.
Group G3 has similar behavior as group G2 as the yield strain reached first in the horizontal bar in the nib tension side at the reentrant corner. The yield loads were at 82%, 93% and 88% of the ultimate load for beams B6, B1 and B7, respectively. Such change in yield load values does not provide a trend with the increase in nib height from 80 mm to 120 and 160 mm for this group as the failure mode of all beam were identical as shearcompression failure.
Group G4 exhibited the yield strain reaching first in the horizontal bar in the nib tension side at the reentrant corner. The yield loads were at 93%, 87% and 88% of the ultimate load for beams B1, B6 and B7, respectively. Group G5 exhibited the yield strain reaching first in the horizontal bar in the nib tension side at the reentrant corner. The yield loads were at 93%, 94% and 79% of the ultimate load for beams B1, B8 and B9, respectively. From results of groups G4 and G5, one may conclude that such change in yield load values does not provide a trend with the increase in amount of stirrups in the beam. However, the addition of the bent bar at the reentrant corner rather than increasing the stirrup amount provided greater ductile behavior given the lower yield load level compared to other beams in the same group.
Numerical Simulations
This section provides detailed investigations on a developed nonlinear threedimensional finiteelement analysis (FEA) simulation, using ABAQUS software (ABAQUS/CAE 2014), for modeling simplysupported RC beam with and without unequal depths, identical to that tested experimentally. The FEA model was validated using the experimental findings in terms of loadcarrying capacity, crack pattern, failure mode, load–deflection response, loadsteel strain relationship. Then, the model was used to conduct a parametric study and used for further researches.
Material Properties of Concrete and Steel in the FE Modeling
Concrete damage plasticity (CDP), smeared cracked and brittle cracking modelling defined in ABAQUS/Standard (ABAQUS/CAE 2014) were utilized to define concrete material properties. However, CDP model was used to constitute the plastic mechanical behavior of concrete herein over brittle or smeared cracked counterparts, since it utilizes the concept of isotropic damage elasticity in combination with isotropic compression and tension plasticity to simulate the nonlinear behavior of concrete under tensile and compressive stresses. The concrete stress–strain response employed for modeling was calibrated respected to concrete compressive strength and splitting test tested experimentally. The stress–strain behavior used in the constitutive model for compression incorporates a formula developed by Carreira and Chu (Carreira and Chu 1985) as shown in Fig. 3a. The uniaxial tensile stress–strain exhibition was selected as a linear elastic response priorto collapse stress value obtained experimentally, beyond which, the stress was decreased linearly to zero value at which strain was about 0.005.
Based on the literature, the Yield Criteria (YC) developed by Lubliner et al. (1989), followed by some modifications by Lee and Fenves (1998), shown in Eq. (1) was employed for concrete:
where \(\sqrt {3I_{2} }\) is the classical deviatoric stress measure, I_{1} refers to the hydrostatic pressure, (\(\overline{{\hat{S}}}_{max}\)) is the algebraically maximum principal stress, the dimensionless values α, β and γ are can be evaluated as follows:
The ratio of biaxialtouniaxial compressive yield stresses (\({{{\text{s}}_{\text{bo}} } \mathord{\left/ {\vphantom {{{\text{s}}_{\text{bo}} } {{\text{s}}_{\text{co}} }}} \right. \kern0pt} {{\text{s}}_{\text{co}} }}\)), used in Eq. (2), may be chosen in between 1.10 and 1.16 (Lubliner et al. 1989). It is worth mentioning that 1.16 was respected in the current study because of the good agreement.
The dimensionless value of \(\beta\) can be estimated according to Eq. (3) by knowing the ratio of compressivetotensile effective cohesion stresses \(\left( {s_{c} *\varepsilon_{cc}^{pl} } \right)\) and \(\left( {s_{t} *\varepsilon_{tc}^{pl} } \right),\) respectively.
where \(\varepsilon_{\text{tc}}^{\text{pl}}\) and \(\varepsilon_{\text{cc}}^{\text{pl}}\) are the tensile and compressive effective cohesion plastic strains, respectively, while s_{t} and s_{c} are the tensile and compressive stresses, respectively.
By knowing the tensiletocompressive meridian ratio namely in ABAQUS (ABAQUS/CAE 2014) program by (\(K\)), the constant \(\gamma\) can be calculated in Eq. (4):
The ratio of K can be selected in between 0.64 and 0.80 (Lubliner et al. 1989; Lee and Fenves 1998), while the default value of K = 0.66 (referred by ABAQUS program) showed an acceptable results.
The real stress–strain response for reinforcing steel bar tested experimentally can be shown in Fig. 3b. To constitute the FEA model with saved computational cost, the actual stress–strain relationship tested experimentally was idealized to piecewise linear curve representing an elastic zone followed by both hardening and softening behavior prior to failure as shown in Fig. 3b.
Model Setup
A nonlinear threedimensional FEA model was developed considering three main elements, namely: RC composite material, reinforced steel bars and rigid steel plates. The RC concrete beam was modelled as a solid continuum, while steel bars were modelled using wire elements. The model utilized the threedimensional and eightnode linear hexahedral solid elements with reduced integration, namely: C3D8R to simulate concrete beam shape, in conjunction threedimensional, twonode, truss elements, namely: T3D2 in ABAQUS software to simulate steel bars. Three thick steel plates with higher elastic stiffness were used in this modeling; one plate at the loading area and two plates at supports. Figure 15 shows view of the developed FEA model.
Perfect bond between reinforcing steel bars and the confined concrete was assumed to create the interaction between steel bars and surrounding concrete. This assumption was achieved using embedded element constraint available in ABAQUS software. In such constraint, steel bars were selected to be embedded in the concrete beam as a host region.
Sensitivity of Numerical Parameters
Several attempts in the FE modelling were executed aiming to investigate the sensitivity and setup the numerical parameters, namely: mesh density (l) and dilation angle (φ). These numerical parameters were examined against the experimental findings for the two control models (B0 and B2) in terms of load–deflection response.
The FEA models were meshed with varying element sizes, namely:10, 20, 25 and 50 mm, leading to dividing the beam width into 10, 5, 4 and 2 elements, respectively. The load–deflection response for control models obtained experimentally and using the FEA model can be seen in Fig. 16. It can be observed that mesh density with size of 10 and 20 mm presented a very close correlation with the experimental results prior to the ultimate stage with minor differences not exceeding about 2% in assessing the ultimate capacity. Due to the higher computational cost that was observed for the FEA model with 10 mm mesh density, 20 mm mesh size was employed in model validation and assessment of the rest of the FEA models.
The dilation angle mainly used in the CDP modeling is to represent the vector direction of plastic strain increment as well as the increase of stress at shearnormal stress plane (p–q) response. Since the shear region located beam the applied load location and the support in the modelled beam is subjected to biaxial or triaxial confinement, the angle value can significantly affect the numerical analysis. The angle of dilation may be selected as 10°, 25° and 40° for thick flat slabs, shallow beams and corbels/deep beams, respectively (Bompa and Elghazouli 2017; Wosatko et al. 2015). The sensitivity study revealed that mesh density of 20 mm and dilation angle of 23° provided the best prediction of the structural response when compared to the experimental findings.
The other sensitive parameters used in the CDP model recommended elsewhere (Lubliner et al. 1989; Lee and Fenves 1998; Schickert and Winkler 1977) showed a satisfactory numerical results against those observed experimentally with negligible differences and acceptable computational cost. Such sensitive parameters were defined as follows: ratio of the second stress invariant on the tensile meridian to that on the compressive meridian (k) = 0.666, flow potential eccentricity (e) = 0.1, the ratio of biaxial to uniaxial compressive yield stresses (\(f_{bo} /f_{co}\)) = 1.16 and the time relaxation parameter (viscosity parameter) = 0.00.
Model Validation
Crack Pattern and Failure Mode
This section discusses and compares the results obtained experimentally and numerically from the static tests performed on the two control beams B0 and B2. Table 3 provides the recorded values of first visual cracking load P_{cr FE}, ultimate load P_{u FE}, maximum deflection at both cracking and ultimate stages; ∆_{cr} and ∆_{u} respectively. Figures 17 and 18 provide the tensile and compressive cracking visualization for the numerical models B0 and B2, respectively. It should be noted that cracking pattern view is available in ABAQUS software through maximum plastic strain. Cracking can be considered in CDP models when maximum principle stresses achieve the positive sign. Also, the crack propagation is assumed to be perpendicular to maximum principle plastic strain.
Similar to experimental crack pattern of beam B0 shown in Fig. 5, numerical simulation shown in Fig. 17 shows tensile stresses causing the first cracking at the bottom beamsurface close to loading section at a load P_{cr FE} of 17.94 kN. Also, model B2 presented very critical stresses leading to first crack extending from reentrant corner identical to that one observed experimentally as shown in Figs. 5 and 18 for experimental and numerical modeling, respectively. Such cracking was predicted at a plastic tensile stress shown in Fig. 18a at a load P_{cr FE} of 3.81 kN.
At higher increments, significant compressive strut connecting between loading location and supporting plates for beam B0 was captured numerically as shown in Fig. 17b and experimentally in Fig. 5a. Significant tensile cracking stresses were observed initiating from reentrant corner of beam B2 expanding upward towards the loading plate zone as shown in the FEA model views in Fig. 18a and experimentally in Fig. 5b through appearance of flexural cracks.
Just before failure of beam B0, the major strut formed at shear zone grew presenting higher compressive stresses at its two ends (i.e. close to loading and supporting plates) as shown in Fig. 17b. However, such compressive stresses were slightly excessive close to loading plate leading to failure at P_{u FE} of 40.40 kN (about 91% of P_{u EXP} as depicted in Table 3) with similar failure mode observed experimentally as shown in Fig. 5a. For FEA model B2, the major tensile cracking stresses formed at reentrant corner propagated upward towards top surface as shown in Fig. 18a, and then compressive stresses peaked at top surface in contact with the loading plate as shown in Fig. 18b, leading to failure at an ultimate load P_{u FE} of 16.85 kN (about 11% greater than P_{uEXP} as shown in Table 3). Such numerical compressive failure was almost similar to the brittle concrete crushing observed experimentally at the edge of loading plate shown in Fig. 5b reflecting the occurrence of compressive action.
Load–deflection response
Experimental and numerical load–deflection relationship measured at thirdpoint of the beam span of the beams B0 and B2 are depicted in Fig. 19. Other than the earlier discussion regarding cracking load and mode of failure, one may observe that both numerical and experimental results showed similar elastic behavior ending at almost the same yield load with a difference of about 11% as shown in Table 3. Also, the load–deflection response for beam B2 shown in Fig. 19b shows good agreement between the FEA Modelling and the experimental findings.
LoadSteel Strain Relationship
Figures 20 and 21 show experimental and numerical loadsteel strain response observed from gauges mounted on horizontal steel bar, vertical steel stirrup, flexural and compressive bars, respectively, for the two control beams B0 and B2. Table 3 compares the yield load values observed experimentally and numerically. Figures 17c and 18c present axial strain distributed along steel bars observed from FEA modelling for beams B0 and B2, respectively. Numerical results showed that the first observed yield load occurred in the flexural bar with a value very close to that obtained experimentally for beam B0 (only with a difference about 9%) as shown in Table 3, while no yield was recorded in the flexural bar for beam B2 as shown in Fig. 21c. However, the FEA model of beam B2 showed that the horizontal bar had the identical essentiality experimental observation reflected, since it exhibited very similar yield load value recorded experimentally. In this context, it should be mentioned that FEA modelling results agreed with experimental outcome in terms of the yield location which occurred at the reentrant corner, as expected Also, numerical results indicated that negligible contribution was obtained from the vertical steel stirrups positioned in both sides of reentrant corners. Therefore, it may be concluded that for beams with unequal depths, the sensitivity of the horizontal bar as shear reinforcement seemed to have a significant consideration compared to vertical closed stirrups. This may be attributed to the angle of crack propagation from reentrant corner as shown in Figs. 18a and 5b for the numerical simulation and tested beam, respectively.
Numerical Parametric Study
Based on the verified FEA models, a parametric study was conducted to investigate the influence of various geometric variables on the structural response. These parameters are impact of Tsection and width of Dregion. FEA Results were compared in terms of cracking visualization, values of first cracking load and ultimate capacity, and the load–deflection response.
Influence of TSection
This section examines the RC slab cast integrally with the beam with two unequal depths. Such Tshape beam was examined previously elsewhere (Kotsovou et al. 2016) when it is case with constant depth. Ciesielczyk et al. (2017) provided a numerical analysis to investigate material and geometric parameters mainly impact on Tsection reinforced concrete beams. Results showed that slab thickness interacting with the beam has a significant influence on the ultimate capacity. However, the numerical models with thinner slab thickness may not provide a satisfactory contribution in beams with shearcompression failure mode. Deifalla and Ghobarah (2014) examined experimentally the behavior of inverted Tshaped RC beams subjected to combined shear and torsion stresses. The value of torsiontoshear ratio significantly affects the performance of the inverted Tshaped beams in terms of cracking pattern; ultimate shear capacity and mode of failure. Also, it was found that the slab stirrups have significant effect in ultimate capacity.
To investigate the effect of the slab cast integrally with the beam of unequal depths on the overall behavior, two FEA models for beam B2 were developed examined with Tshaped section shown in Fig. 22a, b for the fulldepth and partial depth portions of the beam. The slab thickness (t_{f}) used in two models was 50 mm, while the slab width (B) was presented as the main variable per Kotsovou and Cotsovos (2018). In the first FEA model, the slab width shown in Fig. 22 was taken as B = 4t_{f} + b where b is the beam width, leading to slab width B of 300 mm. In the second FEA model, the slab width B was taken as 2d where d is the effective depth of beam, leading to B equal to 360 mm. The two FEA models were labeled as B300 and B360 for those having slab width of 300 and 360 mm, respectively, as shown in Table 4 and Fig. 22. It should be noted that other parameters in the two FEA modelling were kept constant. Figure 22 shows geometrical details for the two FEA Models.
Test results shown in Fig. 22d shows significant increase in the load capacity of the beam with unequal depths with the addition of the slab to resist applied load with the rectangular beam. Beam B300 having a slab of width 300 mm exhibited a first cracking load 7 times greater than that for the same beam with rectangular crosssection. In case of the 360 mm slab, the first crack load was 7 times greater than that for a similar beam with rectangular section. Similar trend was observed in case of the yield load, showing an increase of 5 and 6 times that for a beam of rectangular section for B300 and B360 beams, respectively. Just before failure, it should be mentioned that the two FEA models yielded at approximately similar load values as shown in Table 4 which occurred at the horizontal bar positioned at the reentrant corner as shown in Fig. 22e. The two FEA models failed due to excessive at the reentrant corner followed compression failure in the slab. The contribution of the slab over the beam with unequal depth enhanced the ultimate capacity by 4 and 5 times that for a similar beam with rectangular crosssection for B300 and B360 models, respectively, as shown in Table 4. Moreover, results showed that the slaboverunequal depth beam can significantly affect the mode of failure from the sudden compressive mode (with lower ultimate capacity) to a ductile counterpart. Such ductile failure was observed by yielding the horizontal bar located at reentrant corner followed by slab crushing at a higher load level.
Influence DRegion Breadth
This section presents the influence of beam with depth having augmented width at the Dregion as an attempt to enhance the ultimate capacity. György et al. (NagyGyörgy et al. 2012) carried out an experimental and numerical assessment on dappedend RC beams with variables, namely: strengthening using sheets of fiber reinforced polymers, dappedend height, h_{n}, recess, l_{n}, and crosssection web width, b. It was observed that both sheartospan ratio as well as element geometric properties of crosssection can significantly affect yield load value recorded at steel bar reinforcing reentrant corner. Conforti et al. (2015) performed an experimental study on RC wideshallow beams subjected to a shear force, focusing on the role of the widthtoeffective depth ratio (b/d) and on the beneficial influence of newly developed polypropylene fibers. Results indicated that beams having widthtoeffective depth ratio from 2 to 3 presented a very higher ultimate shear stress compared to the other rivals by about 30–40%.
In order to gain a better insight into the impact of width on the current unequal depth beam, three FEA models were numerically executed. Two FEA models were created with the identical overall geometric and material properties defined earlier for beam B2 except the width of Dregion changed to 150 mm and 200 mm (namely B150 and B200 respectively as listed in Table 5). The increased width was set along sufficient specified length of Dregion (l_{d}) as shown in Fig. 23a where the tensile stresses reached its peak. Such l_{d} length was taken as 400 mm. The third FE model B1502100 had the same increase width of 150 mm but over the entire length of beam of 2100 mm. The third FEA model was aimed at presenting the major variance compared to the second counterpart B150. Table 5 presents the geometric details of the three FEA models along with the original FEA model for beam B2.
Table 5 showed that first cracking stage has been affected by the beam breadth at Dregion, since both FEA models B150 and B200 presented higher cracking load than that of FEA model for beam B2 (see column 7 in Table 5). The first cracking appearance was also detected diagonally extending from reentrant corner. It should be noted that comparison between B150 and B1502100 resulted in approximately similar first cracking load which was about 2.8 times P_{cr} obtained from the FEA model for beams BS. Table 5 shows the first yield load, which was recorded by horizontal bar at point located close to reentrant corner, was greater than that obtained for beam B2 by about 82%, 117% and 68% for models B150, B200 and B1502100, respectively. It should be mentioned that yield stage was observed at a level just prior to the ultimate load which was about 92%, 96% and 83% of P_{u} for models B150, B200 and B1502100, respectively. Beyond yield, the executed FEA models lost the ability to sustain any applied load leading to failure at the reentrant corner due to excessive stresses as shown Fig. 23b. The ultimate load was augmented above that for beams B2 by about 48%, 72% and 54% for models B150, B200 and B1502100, respectively.
Comparison between B150 and B1502100 model resulted in almost very similar enhancement compared to the control beam B2. So, improving cracking, yield and ultimate performance of unequal depth beams by increasing the breadth of Dregion was found to be a better candidate compared to increasing the beam width long the whole span length, especially when the minimum cost is the main requirement in design.
Conclusion
This paper investigates the behavior of RC beam with unequal depths in the form of cracking load, yield load, ultimate carrying capacity and crack pattern. Depth and length of the beam nib were the geometrical variables, while variation in shear reinforcement was considered through an additional steel ratio and layout. Ten RC beams were experimentally tested up to failure. A nonlinear threedimensional FEA analysis was created on two RC beams and validated using the experimental findings. The following conclusions can be drawn from this study:

The location of reentrant corner affects cracking characteristics, yield load, and ultimate load capacity. Experimental results showed that increasing the beam nib heighttorecess length ratio from 0.19 to 0.23 and 0.38 increases the yield load by 27% and 94% and ultimate load by 4% and 64%, respectively. In addition, the mode of failure changes from pure flexural to compressionshear failure with the decrease in nib length.

Experimental results showed significant enhancement in the beam ultimate load carrying capacity when using additional closed stirrups along the entire beam span excluding/including nib zone. On the other hand, adding closed stirrups at only the nib zone seemed to have negligible contribution to the loadcarrying capacity.

The use of bentup bars with ratio of 0.52% at the reentrant corner resulted in better deflection response and lower damage at reentrant corner compared to the findings due to the increase in the shear reinforcement ratio along the entire span.

Good agreement between experimental and FEA results proved the efficiency of the developed numerical model in capturing the nonlinear behavior of the RC beam with unequal depths as depicted from load–deflection response, cracking, failure modes and strain development in reinforcement. Hence, the developed threedimensional FEA model can be used as a tool for further studies in future.

Numerical and experimental results confirmed that for RC beams with unequal depths, the sensitivity of the horizontal bar as shear reinforcement seemed to have a significant effect compared to vertical closed stirrups at the reentrant corner. This may be attributed to the angle of crack growing from reentrant corner. Also, the position of reentrant corner can significantly affect the yield load since a higher yield load was reached when using smaller recess length.

Numerical and experimental findings showed that critical stresses have been generated from reentrant corner at the initiation of first shear cracking. Also, numerical results agreed with experimental observation in terms of yield location which occurred at the reentrant corner due to excessive tensile stresses.

The presence of RC slab, that is cast integrally over the beam with unequal depth, has significant contribution to crack patterns and characteristics (by about 7 to 8 times higher than the nonslab one) as well as yield load values (by about 5 to 6 times higher than the nonslab one) based on the size of the beams considered in this research. Moreover, the presence of the slab changed the mode of failure from the sudden compressive mode (with lower ultimate capacity) to the ductile counterpart (with higher ultimate load).

Numerical results showed that increasing breadth at Dregion (where reentrant corner exists) by about 50% to 100% resulted in an increase in initial cracking and yield load. Also, the ultimate load capacity has been augmented by about 48% to 72% based on the studies widths in this research. The increase in beam width in only the Dregion was found to be more economical and gives better results compared to increasing beam breadth along the whole span length.

Given the proper development length of the nib tension reinforcement at the reentrant zone, bond/anchorage failure of such bars was precluded in this study. Design engineer should be attention to bar anchorage length in practice to promote global failure of the beam.
Availability of data and materials
The experimental data can be obtained through email communication with the first author at ahmed_hamoda@eng.kfs.edu.eg.
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Acknowledgements
The authors acknowledge the contributions of technical staff at Kafrelsheikh University, Egypt, for providing great assistance and helpful comments in executing the experimental program.
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Hamoda, A., Basha, A., Fayed, S. et al. Experimental and Numerical Assessment of Reinforced Concrete Beams with Disturbed Depth. Int J Concr Struct Mater 13, 55 (2019). https://doi.org/10.1186/s4006901903695
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DOI: https://doi.org/10.1186/s4006901903695
Keywords
 beam with unequal depth
 shear resistance
 reentrant corner
 finite element simulation
 concrete damage plasticity model
 beam nib
 ultimate loadcarrying capacity