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Amulu C. P., Ezeagu C. A. Page 45
Combined Torsion, Bending and Shear Analysis in Reinforced
Concrete beams
1Amulu C.P, and
2Ezeagu C. A.
Department of Civil Engineering, Faculty of Engineering Nnamdi Azikiwe University Awka.
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Abstract: This study investigates the effect of combined actions of torsion, bending and shear stresses on
rectangular cross-sectional plain and reinforced concrete beams at a given concrete mix design. The ultimate
torsional strengths and angle of cracks of the beams were determined experimentally through a simple test
arrangement set-up on fifteen beam specimens grouped into five groups; BC1 to BC5. The combined loading was
achieved through by loading the test beams at an eccentric distance away from the beam’s principal axis at the mid-
span, through a system of Universal Testing Machine at the Engineering laboratory of the Standard Organization of
Nigeria (Son), Enugu. Three international standard codes (BS 8110, Euro code 2 and ACI 318) were used to
calculate the ultimate torsional strengths predicted for torsional resistance provided by longitudinal and transverse
reinforcements and the strut of concrete cross-section. The values obtained from the codes were compared with that
of experimental results observation for validation. The ultimate torsional moments predicted by different classical
theories (elastic, plastic, skew-bending and Cowan’s equations) were also used to calculate the ultimate torsional
moments and compared with the experimental results. It was observed that the values predicted by the codes were
not the same with each other and the experimental results in some cases while in other cases, the predicted values
matches that of experimental results. This can be attributed to difference in certain assumptions, parameter and
constants taken during the formulation of their respective equations which influenced the results. It was also
observed from this study that ultimate torsional moments predicted by the classical theories are significantly
difference from that of experimental results. It was concluded from the study that the angle of cracks used in design
by different codes should not be fixed, but to be varied in other to obtain better economic and stable structures in
terms of longitudinal and transverse reinforcements together with high concrete section that can sustain the applied
loads.
Keywords: Bending, Flexural, Load, Moment and Torsion
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Amulu C. P., Ezeagu C. A. Page 46
Introduction: Beams are the simplest structural elements that are used extensively to support
loads. On several situations, beams and slabs are subjected to torsion in addition to bending
moment and shear force. Loads acting normal to the plane of bending will cause bending
moment and shear force. However, loads acting away from the plane of bending will induce
torsional moment along with bending moment and shear (Davison and Owens, 2005),
(Kharagpur, 2008) and the interaction among these forces is important. Torsion is a load that
subjects a member to couples/moments that twists the member spirally. This implies that torsion
occurs when applied loads are eccentric from the centroid and the resultant does not pass through
the beam’s shear centre (Amulu, Ezeagu and Obiorah, 2016), (Onouye and Kane, 2007). Torsion
may be induced in a member in various ways during the process of load transfer in a structural
system. Torsion happens because of integrity and continuity of members and also under the
effect of external loads in concrete structure (Barghlame and Lotfollahi-Yaghin, 2011).Torsion
generated in a member can be classified into two main types of situations based on necessity of
analysis and design for torsion (Sengupta and Menon).Primary or equilibrium torsion and
Secondary or compatibility torsion: If a member is not properly reinforced for torsion with
closed stirrups and longitudinal steels in case of reinforced concrete beam, a sudden brittle
fracture may occur, leading to failure of the beam at torsional cracking loads. Shear stresses due
to torsion create diagonal-tension stresses that produce diagonal cracking (Leet and Bernal,
1997). In structural analysis, the effects of torsion are usually neglected and only bending, shear
and axial forces are taken into consideration. This is because torsion was considered to be a
secondary effect that will be covered in the factor of safety (Kamara and Rabbat, 2007). When
torsion is encountered in reinforced member, it usually occurs in combination with flexure and
transverse shear. The interactive behavior of torsion with bending moment and flexural shear in
reinforced concrete beam is fairly complex, owing to non-homogeneous, non-linear and
composite nature of the material and presence of cracks (Pillai and Menon, 2009).
(Panchacharam and Belarbi, 2002) and (Kharagpur 2008).
Statement of Problem: The design provisions in the areas of combined analysis for shear and
torsion are not of the same level of rationality and general applicability. The absence of rational
models has resulted in highly empirical design procedures characterized by large difference in
values evaluated from different design codes when compared to experimental test results. The
Amulu C. P., Ezeagu C. A. Page 47
lack of fundamental behavioral models for reinforced concrete members subjected to shear and
torsional loading seems to be prime reason for the unsatisfactory nature of the highly empirical
design procedures used in design. This study provides the ideal of conceptual model to properly
represent the behavior of reinforced concrete member subjected to torsion and to compare results
obtained from different approaches in the standard design codes of practices with the ones
obtained experimentally. The study furthermore seeks to compare the response of reinforced
concrete and steel beams to torsional loading.
Aim of the Study: To optimize the effect of torsion on Reinforced concrete beams at a designed
mix ratio.
Objectives of study: The objectives of this study include:
1) To examine and compare the torsional design provisions/ procedures in BS 8110, Euro
code 2, and ACI 318 building code
2) To evaluate the torsional parameters (torsional crack load and failure load, ultimate
torsional capacity and angle of twist) of a reinforced concrete beams subjected to
combined shear, bending and torsional loading using standard design codes and
experimental work.
3) To validate the provisions of the codes by comparing the calculated design code values
with that of experimental results.
4) To evaluate the ultimate torsional strength of reinforced concrete beams obtained
experimentally, compare it with those predicted by theories: elasticity, plasticity, skew-
bending and space truss analogy.
Scope and limitations of the study: In this study, analysis and experimental work will be
carried out. In the analysis, torsional provisions of Euro code 2, BS 8110 and ACI 318 building
codes are evaluated against the experimental data for reinforced concrete beams under the
actions of combined shear, bending and torsion only. The experimental result will also be
evaluated with ultimate torsional strengths predicted analytically by different theories on torsion
in prismatic object.
Significance of the work: This study provides an evaluation of the design provisions for
combined actions of shear, bending and torsion given by the ACI 318 building code, BS 8110
and Euro Code 2 to experimental values. This study will make structural designers to be familiar
with the provisions of the BS 8110, Euro Code 2 and ACI 318 building code provisions to
torsional design and to determine the more conservative and consistent code among the three
codes studied. Specification recommendations are given for improving the design codes
Amulu C. P., Ezeagu C. A. Page 48
provisions. Structural standards and codes of practice are reviewed continuously and
improvements are implemented as research findings reveal more accurate methods of design.
LITERATURE REVIEW: Torsion may be induced in a member (reinforced concrete, timber
or steel beam) in various ways during the process of load transfer in a structural system. When a
beam is subjected to transverse loading such that the resultant force passes through the
longitudinal shear axis, the beam will not twist, but bends. However, when the resultant force
acts away from the shear center axis, moment is induced into the system (Davison and Owens,
2005). This moment causes a body to have tendency to rotate and if the system tries to resist
such rotational tendency, bending and /or torsion results (Onouye and Kane, 2007). This implies
that if applied loads are “eccentric” from the centroid and the resultant forces do not pass through
the member’s centroid, then torsion occurs. The distance from the centroid that the load passes
through is the “eccentricity” and the product of the eccentricity and the load gives the torsional
moment. This torsional moment tends to twist the beam to give a rotational displacement. There
are some other cases where beams are subjected to torsion as a result of external load acting
outside the ‘shear center’ axis of a given cross-section, or deformation resulting from the
continuity of beams or similar members that are joint at an angle to each other. In more general
cases, the determination of the torsional moment for any loading in torsion and shear requires
knowledge of location of the center of shear in addition to the geometric centroid (Ziegler,
1995), (Amulu, Ezeagu and Obiorah, 2016). Structural members subjected to torsion are of
different shapes such as T-shaped, inverted L-shaped, double T-shaped and box section. These
different configurations make the understanding of torsion in reinforced concrete members a
complex task (Panchacharam and Belarbi, 2002). Analysis of the torsional behavior of a
reinforced concrete member can be divided into three different phases namely i. pre-cracking
stage. ii. post-cracking stage.iii. the time of yielding of steel. (Csiko’s and Hegedus, 1998) and
(Barghlame and Lotfollahi-Yaghin, 2011).Prior to cracking, a torsional moment applied to a
concrete member is resisted by internal shear stresses. (Kamara and Rabbat, 2007). When a
concrete member is loaded in pure torsion, shear stresses develop. One or more cracks (inclined)
develop when the maximum principal tensile stress reaches the tensile strength of concrete.
(Pillai and Menon, 2009).From the uniqueness of solutions of the elasticity equations, it follows
that the assumed forms for the displacements are the exact solution to the torsional problems
Amulu C. P., Ezeagu C. A. Page 49
(Wolfram mathematical documentation centre), (Namiq, 2012), (Ezeagu, Osadebe and Anyata,
2014). The properties of a material, undergoing ‘elastic process’ are not the same in all
directions, it is called anisotropic (Sadd, 2005) and (Ezeagu and Nwokoye, 2008). The problem
with this equation is that the obtained results are unconservative by approximately 50% (Csikos
and Hegedus, 1998). However, Reinforced concrete is combined with two kinds of materials
namely: steel and concrete. These two materials have two different kinds of characteristics. Steel
is a kind of material which is homogeneous, whereas concrete is not a homogeneous material.
The homogeneity of steel versus concrete mechanical attribute of these materials depends on
time and environment (Barghlame and Yaghin, 2011). In other words, limitation of the above
model is that the failure of reinforced concrete to torsion is not elastic.
METHODOLOGY: The methodology used in this study will be based on two phases: the first
phase is on experimental design of fifteen rectangular Reinforced concrete beams all of these
specimens loaded eccentrically away from beams principal axis by a combined action of
bending, shear and torsional stresses, applied through a system of Universal Testing machine.
The second phase is on evaluation and comparison of torsional design provisions of the
international standards codes examined; BS 8110, Euro Code 2 and ACI 318 building code. The
calculated values from these codes will be analyzed and validated against the experimental
values measured and the response of reinforced concrete beams to torsional crack load will be
compared with those of classical theories: elasticity, plasticity, skew-bending theories and space
truss analogy.
EXPERIMENTAL DESIGN: Designs to be carried out:
I. Design of reinforced concrete beams to be used for the experimental work (which is an
eccentric loaded beam). The ultimate Torsional moment predicted by codes under this
study will be compared with the values to be observed from Experimental work as
presented in table 3.2.
II. Concrete mix Design for compressive strength of concrete cubes at 28 days
III. The design examples of reinforced concrete beams against torsion, bending and shear
stresses using BS 8110, Euro code 2 and ACI 318 codes for equilibrium and
compatibility Torsional cases, the flow chart in figure 3.4 will be used as guide.
Amulu C. P., Ezeagu C. A. Page 50
The torsional ultimate moments predicted by different theories (Elasticity, plasticity and skew-
bending theories) on torsion will be calculated and compared with the experimental values to be
observed using table 3.3 below as guide.
Choice of test assembles: The objective of the design of rectangular beam was to provide a
simplified test arrangement and to ensure a failure of the test beams in combined actions of
bending, shear and torsion without causing a failure in other elements. The test beam are seated
on two steel supports resting on the laboratory floor and could be loaded at any desired
eccentricity from the beam principal axis, through a system of Universal Testing machine with a
point-loading head. Thus, a known combination of torsional moment, bending moment and
shearing forces could be applied on the test beam simultaneously. The test beam is restricted at
both ends on the steel support in other to avoid rotation. To avoid failure in the steel support, it
was designed to have a higher compressive strength than the loaded test beam. The beam was
designed for stresses of 30𝑁/𝑚𝑚2 in concrete and 460𝑁/𝑚𝑚2 in reinforcement. The designed
test beam specimens are to carry a maximum load of 25𝑘𝑁/𝑚 at an eccentricity of 60𝑚𝑚,
required 8𝑚𝑚 diameter of stirrups at 150𝑚𝑚 centre to center and 10𝑚𝑚 diameter of
longitudinal reinforcement to resist calculated shear and torsion. However, the spacing of the
stirrups was varied for the test beam specimens to study the effect of transverse reinforcement on
the ultimate strength of the test beam.
Amulu C. P., Ezeagu C. A. Page 51
Specimen: Five groups of specimens, each group contains three 150*150*1300𝑚𝑚 long
rectangular reinforced concrete; all the samples have effective span of 1200𝑚𝑚 designed, to be
constructed and tested in the Standard Organization of Nigeria (SON) Engineering laboratory,
PRODA junction Enugu-Abakaliki Express Road, Emene Industrial Layout Emene, Enugu State,
under the combined actions of bending, torsion and shear forces simultaneously applied by
loading the test beams at an eccentric distance from the beams principal axis through a system of
Universal Testing machine. A group of control beams are design to fail in flexure, shear and
torsion. The cross-section of the beams is 150 ∗ 150𝑚𝑚. The groups of reinforced concrete
beams consist of one with control beam and four beams designed with varied ratio of both
longitudinal and transverse reinforcements (see table 3.1).
Details of assemblies: The arrangement of test beam specimens is detailed in figures 3.1 and
3.2. The test beam specimens have the same cross-section of 150 ∗ 150 ∗ 1300𝑚𝑚 with beams
BC2, BC3, BC4 and BC5 reinforced transversely and longitudinally, while BC1 is a plain
concrete beam without both transverse and longitudinal reinforcements. The spacing of
transverse reinforcement and number of longitudinal steels of Beams BC2, BC3, BC4 and BC5
are varied (see table 3.1).
Experimental set-up: The test beams are supported over an effective span of 1300𝑚𝑚 and
subjected to an eccentric loading through a system of Universal Testing machine with a point
load at the middle of the beam (figures 3.1 and 3.2). A series of tests are to be carried out with
plain and reinforced concrete beam specimens loaded to a combined action of twisting moment,
flexure and shearing forces, simultaneously. The reinforcement ratios are varied both in the
transverse and longitudinal directions, in order to study its effect on the resistance of the test
beams to all applied load. The differences in the reinforcements can be seen in Table 3.1. The
test is a destructive one and the equipment to be used includes; Universal Testing machine and
compressive testing machine at Standard Organization of Nigeria (SON) Engineering laboratory
Enugu State.The actual loading of the test beam will be done by a system of Universal Testing
machine at an eccentric distance away from beams axis. The load is applied at an increased rate
of 20 percent. The ultimate torsional moment is to be determined. The load at which there is a
crack on the test beam is determined and the load that leads to failure of the test beam is to be
Amulu C. P., Ezeagu C. A. Page 52
read from the digital measuring gauge on the machine. The beam is considered to have collapsed
when it could resist no more loads. Two methods are used to detect the cracking torsional
moment of the test beam; the first method is the visual observation of the test beam surfaces of
every load step. As the cracks began at the middle of the test beam, they are easily observable.
The second method is the observation of the sound of the cracking. The ultimate torsional
moment is taken as the maximum moment reached throughout the test. At every load step, the
cracks are marked. After the tests, these marks were drawn on paper so that the angle between
the cracks and the axis of the beam could be measured.
Table 3.1Summary of Reinforced Concrete Beams Tested (all the samples are 1500mm long).
Beam notation longitudinal bars (mm) Stirrups bars (mm) Spacing of links (mm)
BC1 Not reinforced
BC2 4T10 R8 200
BC3 4T10 R8 100
BC4 6T10 R10 200
BC5 6T10 R10 100
Figure 3.3 Loading and geometry details of reinforced concrete control beam
X 1200
1500
150 150
P
X e
150
P
150
X-X section
Amulu C. P., Ezeagu C. A. Page 53
Table 3.2: Ultimate Torsional moment predicted by codes.
Torsional resistance Euro Codec 2 ACI 318-11 BS 8110
Longitudinal
reinforcement 𝑇𝑅𝑑1 = 2𝐴𝑘
𝐴𝑠𝑙𝑓𝑦𝑙
𝑈𝑘
𝑡𝑎𝑛𝜃 𝑇𝑈1 =
2𝐴0𝐴𝑙𝑓𝑦𝑙
𝑃ℎ𝑡𝑎𝑛𝜃
𝑇𝑈𝑆1 =𝐴𝑙(0.8𝑥1𝑦1)(0.87𝑓𝑦𝑙)
(𝑥1+𝑦1)
Transverse
reinforcement
𝑇𝑅𝑑2 = 2𝐴𝑘(𝐴𝑠𝑤
𝑆) 𝑓𝑦𝑡𝐶𝑜𝑡𝜃 𝑇𝑈2 = 2𝐴0(
𝐴𝑡
𝑆) 𝑓𝑦𝑡𝐶𝑜𝑡𝜃
𝑇𝑈𝑆2 = 𝐴𝑠𝑣
𝑆(0.8𝑥1𝑦1)(0.87𝑓𝑦𝑡)
Concrete section 𝑇𝑅𝑑3
= 2𝑣𝑓𝑐𝑑𝐴𝑘𝑡𝑒𝑓𝑆𝑖𝑛𝜃𝐶𝑜𝑠𝜃
𝑣 = 0.6(1 − 𝑓𝑐𝑘/250)
Taken as:
𝑇𝑈3
= ∅𝜆√𝑓𝑐′
𝐴𝑐𝑝2
𝑃𝑐𝑝
Taken as:
𝑇𝑈𝑠3 =1
2𝜏𝑚𝑎𝑥ℎ𝑚𝑖𝑛
2 (ℎ𝑚𝑎𝑥 −ℎ𝑚𝑖𝑛
3)
𝜏𝑚𝑎𝑥 ≈ 0.2√𝑓𝑐𝑢
The minimum of this value from each code should be adopted as the ultimate Torsional
resistance.
Table 3.3: Torsional moments predicted by different theories
Elasticity Plasticity Skew-bending
Torsional moment 𝑇𝑐𝑟 = 𝛼𝑏2𝐷𝜏𝑚𝑎𝑥 𝑇 = 0.5𝜏𝑡ℎ𝑚𝑖𝑛2 (ℎ𝑚𝑎𝑥 − ℎ𝑚𝑖𝑛/3)
𝑇𝑈𝑆 = 𝑇𝑐 + 𝛼𝑡
𝑥1𝑦1 𝐴𝑡 𝑓𝑡𝑦
𝑆
Presentation of Results : To validate the experimental results obtained the three standard design
codes under study; BS 8110, Euro Code 2 and ACI 318 will be evaluated for verification of the
results. In order to provide the accuracy and efficiency of the experimental results, the results
obtained will be compared with those from design codes and theoretical predictions (elastic,
plastic and skew-bending theories).
Amulu C. P., Ezeagu C. A. Page 54
Table 4.1 the characteristics of tested beams
Sample test
Beam
Cross-
section
Length
(𝑚𝑚)
𝑓𝑐𝑢
(𝑀𝑝𝑎)
Dia. of
stirrup(𝑚𝑚)
Dia. of
main-bar
(𝑚𝑚)
𝑓𝑦𝑡
(𝑀𝑝𝑎)
𝑓𝑦𝑙
(𝑀𝑝𝑎)
S
(𝑚𝑚)
𝐴𝑡𝑆⁄
(𝑚𝑚2
/𝑚𝑚)
𝐴𝐿
(𝑚𝑚2)
BC1 150*150 1300 30 - - - - - - -
BC2 150*150 1300 30 8 10 434 445 200 0.503 314
BC3 150*150 1300 30 8 10 434 445 100 1.006 314
BC4 150*150 1300 30 8 10 434 445 200 0.503 471
BC5 150*150 1300 30 8 10 434 445 100 1.006 471
Table 4.2: Experimental results obtained from the tested beam samples
Sample Eccentricity e (𝑚𝑚)
Load at failure (𝑘𝑁)
Cracking Angle 𝜃 (𝑖𝑛 𝑑𝑒𝑔𝑟𝑒𝑒)
BC1
BC1
BC1
65
10.690
10.760
10.480
AVE 10.637
BC2
BC2
BC2
65
40.200
39.835
43.020
43
44
40
AVE 41.018 42.333
BC3
BC3
BC3
65
50.870
49.785
49.050
37
38
37
AVE 49.902 37.333
BC4
BC4
BC4
65
43.290
44.285
43.590
37
39
37
AVE 43.722 37.667
BC5
BC5
BC5
65
51.335
50.255
51.500
39
40
39
AVE 51.030 39.333
Amulu C. P., Ezeagu C. A. Page 55
Table 4.3A: Torsional strength/ultimate torsional moment of beams according to standard codes’
prediction and experimental test beams.
Beam
sample
BS 8110
(𝜃 = 450)
(𝑘𝑁𝑚)
Euro Code 2
(𝜃 = 450)
(𝑘𝑁𝑚)
ACI 318-11
(𝜃 = 450)
(𝑘𝑁𝑚)
Experimental
Test Result
(𝑘𝑁𝑚)
Element failed/
mode of failure
𝑻𝑩𝑺,𝑨𝑳 𝑻𝑩𝑺,𝑨𝒕 𝑻𝑩𝑺,𝒄𝒐𝒏𝒄 𝑻𝑬𝑪,𝑨𝑳 𝑻𝑬𝑪,𝑨𝒕 𝑻𝑬𝑪,𝒄𝒐𝒏𝒄 𝑻𝑨𝑪𝑰,𝑨𝑳 𝑻𝑨𝑪𝑰,𝑨𝒕 𝑻𝑨𝑪𝑰,𝒄𝒐𝒏𝒄 𝑻𝑬𝑹
BS EC2 ACI
BC1 - - 1.234 - - 4.2223 - - 1.3121 0.6914 - - -
BC2 5.0265 1.6104 1.234 6.5647 6.3096 4.2223 5.6097 3.652 1.3121 2.6662 T,C - C
BC3 7.5398 3.2208 1.234 6.5647 12.6193 4.2223 5.6097 7.3047 1.3121 3.2436 T,C - C
BC4 5.0265 1.6104 1.234 9.8470 6.3096 4.2223 8.4151 3.652 1.3121 2.8419 T,C - C
BC5 7.5398 3.2208 1.234 9.8470 12.6193 4.2223 8.4151 7.3047 1.3121 3.31695 T,C - C
Table 4.3B; Comparison of the ratio of ultimate torsional strength between standards’ prediction
and experimental result
Test
Beam 𝑻𝑩𝑺,𝑨𝑳
𝑻𝑬𝑹
𝑻𝑩𝑺,𝑨𝒕
𝑻𝑬𝑹
𝑻𝑩𝑺,𝒄𝒐𝒏𝒄
𝑻𝑬𝑹
𝑻𝑬𝑪,𝑨𝑳
𝑻𝑬𝑹
𝑻𝑬𝑪,𝑨𝒕
𝑻𝑬𝑹
𝑻𝑬𝑪,𝒄𝒐𝒏𝒄
𝑻𝑬𝑹
𝑻𝑨𝑪𝑰,𝑨𝑳
𝑻𝑬𝑹
𝑻𝑨𝑪𝑰,𝑨𝒕
𝑻𝑬𝑹
𝑻𝑨𝑪𝑰,𝒄𝒐𝒏𝒄
𝑻𝑬𝑹
BC1 - - 1.7848 - - 6.1042 - - 1.8977
BC2 1.8853 0.6040 0.4628 2.4622 2.3665 1.5836 2.1040 1.3697 0.4921
BC3 2.3245 0.9930 0.3804 2.0239 3.8905 1.3017 1.7295 2.2520 0.4045
BC4 1.7687 0.5667 0.4342 3.4649 2.2202 1.4857 2.9611 1.2851 0.4617
BC5 2.2731 0.9710 0.3720 2.9687 3.8045 1.2729 2.5407 2.2055 0.3962
Torsional shear strength of reinforced concrete beam according to standards’ code prediction and
experimental test result (𝑇𝐸𝑅). The torsional resistance provided by the longitudinal
reinforcement (𝑇𝐴𝐿), shear/transverse reinforcement(𝑇𝐴𝑡), and concrete cross-section ( 𝑇𝑐𝑜𝑛𝑐). L
–longitudinal reinforcement, T-transverse/vertical reinforcement, C-concrete section.
NB: an element is considered to have failed when the experimental value from the tested beam is
greater than that predicted by standard codes for the three variables under consideration.
Amulu C. P., Ezeagu C. A. Page 56
Table 4.4A: Torsional strength/ultimate torsional moment of beams according to standard codes’
prediction and experimental test beams.
Beam
sample
Euro Code 2
(𝜃 = 220)
(𝑘𝑁𝑚)
ACI 318-11
Experimental
Test Result
(𝑘𝑁𝑚)
Element failed
ACI (1) (𝜃 = 300)
(𝑘𝑁𝑚)
ACI (2) (𝜃 = 600)
(𝐾𝑁𝑚)
𝑇𝐸𝐶,𝐴𝐿 𝑇𝐸𝐶,𝐴𝑡 𝑇𝐸𝐶,𝑐𝑜𝑛𝑐 𝑇𝐴𝐶𝐼,𝐴𝐿 𝑇𝐴𝐶𝐼,𝐴𝑡 𝑇𝐴𝐶𝐼,𝑐𝑜𝑛𝑐 𝑇𝐴𝐶𝐼,𝐴𝐿 𝑇𝐴𝐶𝐼,𝐴𝑡 𝑇𝐴𝐶𝐼,𝑐𝑜𝑛𝑐 𝑇𝐸𝑅
EC2 ACI1 ACI2
BC1 - - 2.933 - - 1.3121 - - 1.3121 0.6914 - - -
BC2 2.6521 15.774 2.933 3.2390 6.3256 1.3121 9.7166 2.108 1.3121 2.6662 L C T,C
BC3 2.6521 31.5482 2.933 3.2390 12.652 1.3121 9.7166 4.217 1.3121 3.2436 L,C L,C C
BC4 3.9782 15.774 2.933 4.8589 6.3256 1.3121 14.575 2.108 1.3121 2.8419 - C T,C
BC5 3.9782 31.5482 2.933 4.8589 12.652 1.3121 14.575 4.217 1.3121 3.31695 C C C
Table 4.4B; Comparison of the ratio of ultimate torsional strength between standards’ prediction
and experimental result
Test
Beam 𝑇𝐸𝐶,𝐴𝐿
𝑇𝐸𝑅
𝑇𝐸𝐶,𝐴𝑡
𝑇𝐸𝑅
𝑇𝐸𝐶,𝑐𝑜𝑛𝑐
𝑇𝐸𝑅
𝑇𝐴𝐶𝐼1,𝐴𝐿
𝑇𝐸𝑅
𝑇𝐴𝐶𝐼1,𝐴𝑡
𝑇𝐸𝑅
𝑇𝐴𝐶𝐼1,𝑐𝑜𝑛𝑐
𝑇𝐸𝑅
𝑇𝐴𝐶𝐼2,𝐴𝐿
𝑇𝐸𝑅
𝑇𝐴𝐶𝐼2,𝐴𝑡
𝑇𝐸𝑅
𝑇𝐴𝐶𝐼2,𝑐𝑜𝑛𝑐
𝑇𝐸𝑅
BC1 - - 4.2421 - - 1.8977 - - 1.8977
BC2 0.9947 5.9163 1.10 1.2148 2.3725 0.4921 3.644 0.7906 0.4921
BC3 0.8176 9.7263 0.9042 0.9986 3.9006 0.4617 2.9956 1.300 0.4045
BC4 1.3998 5.5505 1.032 1.7097 2.2258 0.4617 5.1286 0.7418 0.4617
BC5 1.1994 9.5112 0.8842 1.4649 3.8143 0.3956 4.3941 1.2713 0.3956
Continuation of Tables 4.3 and 4.4 Experimental verification of ultimate capacity
Experimental verification of ultimate capacity
Test
Beam 𝑇𝐸𝑅
(𝑘𝑁𝑚)
𝑀𝐸𝑅
(𝑘𝑁𝑚)
𝑉𝐸𝑅
(𝑘𝑁)
BC1 0.6914 3.3271 5.7720
BC2 2.6662 12.4416 20.9628
BC3 3.2436 15.2066 25.4045
BC4 2.8419 13.2526 22.3145
BC5 3.31695 15.4451 25.9686
Amulu C. P., Ezeagu C. A. Page 57
The measured and calculated values of ultimate torsional moment (KN-m) obtained from
experiment and predicted by different theories on torsion.
Table 4.5 values of theoretical predictions and experimental measures of ultimate torsional
moment of prismatic rectangular cross-section.
Beam sample
Elasticity
(𝐾𝑁𝑚)
Plasticity
(𝐾𝑁𝑚)
Skew-
Bending (𝐾𝑁𝑚)
Cowan’s
equation (𝐾𝑁𝑚)
Experimental
Result (𝐾𝑁𝑚)
BC1 0.769 1.2324 1.235 0.769 0.6914
BC2 0.769 1.2324 2.3878 4.4711 2.6662
BC3 0.769 1.2324 2.8652 8.1732 3.2436
BC4 0.769 1.2324 2.6469 4.4711 2.8419
BC5 0.769 1.2324 3.2317 8.1732 3.3169
0
1
2
3
4
5
6
7
8
9
0 2 4 6
ult
imat
e t
ors
ion
al m
om
en
t (k
Nm
)
Elasticity
Plasticity
Skew-bending
Cowan's Equation
ExperimentalResult
Figure 4.1 scatter graph of ultimate torsional moment obtained from classical theoretical predictions
and experimental measures of ultimate torsional moment
Amulu C. P., Ezeagu C. A. Page 58
Figure 4.2. Crack pattern for BC1 beam
specimen
Figure 4.3.crack pattern for BC2 beam specimen
Figure 4.4. Crack pattern for BC3 beam
specimen
Figure 4.5.Crack pattern for BC4 beam
specimen
Figure 4.6. Crack pattern for BC5 beam specimen
Amulu C. P., Ezeagu C. A. Page 59
Table 4.6a calculations from simply supported beam subjected to combined actions of torsion,
shear and bending stresses. (example 1)
𝐴𝑠𝑟𝑒𝑞,𝑏𝑒𝑛𝑑𝑖𝑛𝑔
(𝑚𝑚2)
𝐴𝑡 𝑠,𝑠ℎ𝑒𝑎𝑟
⁄
(𝑚𝑚2/𝑚𝑚)
𝐴𝑠𝑟𝑒𝑞,𝑡𝑜𝑟𝑠𝑖𝑜𝑛
(𝑚𝑚2)
𝐴𝑡 𝑠,𝑡𝑜𝑟𝑠𝑖𝑜𝑛
⁄
(𝑚𝑚2/𝑚𝑚)
Area related
to shear
flow
(𝑚𝑚2)
Combined
transverse:
shear +
torsion
(𝑚𝑚2/𝑚𝑚)
Combined
longitudinal:
bending +
torsion
(𝑚𝑚2)
BS
8110
156 0.253 85 0.7845 8000 1.0375 241
ACI
318
273 0.272 90 0.442 8774 0.714 363
Euro
code 2
144 0.496 57 0.25 0.746 1.10 201
Table 4.6b calculations from precast footbridge slab (example 2)
𝐴𝑠𝑟𝑒𝑞,𝑏𝑒𝑛𝑑𝑖𝑛𝑔
(𝑚𝑚2)
𝐴𝑡 𝑠,𝑠ℎ𝑒𝑎𝑟
⁄
(𝑚𝑚2/
𝑚𝑚)
𝐴𝑠𝑟𝑒𝑞,𝑡𝑜𝑟𝑠𝑖𝑜𝑛
(𝑚𝑚2)
𝐴𝑡 𝑠,𝑡𝑜𝑟𝑠𝑖𝑜𝑛
⁄
(𝑚𝑚2/𝑚𝑚)
Area related
to shear
flow
(𝑚𝑚2)
Combined
transverse:
shear +
torsion
(𝑚𝑚2/
𝑚𝑚)
Combined
longitudinal:
bending +
torsion
(𝑚𝑚2)
BS
8110
929 0.63 401 0.78 51120 1.41 1330
ACI
318
571 0.6934 547 0.8861 88838.53 1.5795 1118
Euro
code 2
751 0.600 385 0.5 59166 1.10 1136
Summary of Result: In validating the ultimate torsional strengths observed from the experiment
on combined actions of torsion, bending and shear on 15 reinforced and non-reinforced concrete
beam samples, current international design codes’ predictions on the ultimate torsional strength
are used to calculate the corresponding values and compared with the experimentally observed
ones and values tabulated for comparison. Also, the ultimate torsional strengths predicted by
different classical theories on torsion: elastic, plastic, cowan and skew-bending theories are
Amulu C. P., Ezeagu C. A. Page 60
calculated using their respective equations and values tabulated for comparison with the
experimental observed values. Another result presented was on two design examples of
structures subjected to combined actions of torsion, shear and bending; using the three design
codes under this study to determine the ultimate torsional strengths, areas of longitudinal and
transverse reinforcements required to resist the applied loads and the values tabulated for
comparison. The next result is on the use of Ms-excel to predict the ultimate torsional strengths
proposed by the three codes under consideration, when the areas of both longitudinal and
transverse reinforcements are given and their values are tabulated for comparison. The crack
patterns are also displayed.
Discussion: The ultimate torsional strength for rectangular cross-section of 15 reinforced
concrete beams subjected to combined actions of torsion, shear and bending were determined
using experiment, BS 8110, ACI 318 and Euro code 2 design code equations. Also the classical
theories of elastic, plastic, Cowan and skew-bending equations on ultimate torsional strength
were determined. All the calculated values from the codes and theories are compared with the
experimental observed values. Table 4.1 present the characteristics/ properties of the tested
reinforced and non-reinforced concrete beams. These characteristics are used also in the design.
Table 4.2 presents the loads at failure and cracking angles of the 15 reinforced and non-
reinforced concrete beams specimens subjected to combined actions of torsion, shear and
bending, applied at an eccentric distance at the mid-span of the beam specimens. From this table,
the ultimate torsional strength, bending moment and shear forces are determined. It can also be
seen that angle of crack is not (𝜃 = 450) , as generally taken, but varies. Table 4.3A and B
presents for comparison the ultimate torsional strength of tested beams and observed from
experiment and values calculated from the equations predicted by BS 8110, ACI 318 and Euro
code 2 for the general accepted angle of cracking of (𝜃 = 450). The ultimate torsional strength
predicted by the codes under this study with respect to the torsional resistance provided by the
transverse reinforcement (𝑇𝐴𝑡), longitudinal reinforcement 𝑇𝐴𝐿 , and the concrete cross-section
( 𝑇𝑐𝑜𝑛𝑐), the mode of failure / element failed are also presented. The B part of the table presents
the ratios of the calculated values to the experimental results. From these tables, it can be
indicated that an element has failed when the experimental result is greater than any of those
predicted by the codes for longitudinal reinforcement L, transverse reinforcement T, or concrete
Amulu C. P., Ezeagu C. A. Page 61
section C. It can be seen from the table that some values predicted by the codes matches those
observed from experimental result. However, ultimate torsional strengths calculated for the
longitudinal reinforcement resistance from the three codes are higher than that observed from the
experiment. This indicates that the beams specimens failed before the longitudinal reinforcement
yield strength was reached. It can also be seen that the ultimate torsional strengths predicted by
the codes for Transverse reinforcement resistance are statistically the same to that obtained
experimentally except in Euro code 2 that over estimated its values when compared with
experimental results and the other two codes. The concrete section failed in the prediction by BS
8110 and ACI 318 codes while Euro code 2 predicted a higher value than that observed from
experiment. In other words, values calculated from Euro code 2 for the torsional resistance for
longitudinal and transverse reinforcements together with that of concrete section are highest,
followed by ACI 318, then BS 8110. Table 4.4 A and B presents for comparison, the ultimate
torsional strength predicted by the ACI 318 and Euro code 2, using the specified values of 𝜃
apart from 𝜃 = 450 . The B part of the table presents the ratios of the calculated values to the
experimental results. From the table, it can be observed that the ultimate torsional strength
predicted by Euro code 2 for longitudinal reinforcement resistance to torsion is statistically the
same with the experimental results while there was an over estimation by the torsional resistance
for transverse reinforcement. When the Euro code 2 values for 𝜃 = 450 𝑎𝑛𝑑 220 are compared,
it can be observed that the code was more conservative and consistence for 𝜃 = 220 for torsional
resistance provided by longitudinal reinforcement and concrete section while that for transverse
reinforcement was over estimated and non-conservative when compared with observed values
from experiment. This should be used where a higher torsional stresses are expected. The ACI
318 code using 𝜃 = 300 for torsional resistance provided by longitudinal reinforcement was
more conservative and consistent than those values gotten when 𝜃 = 450 while that provided by
the concrete section remain the same. The values provided by transverse reinforcement are over
estimated for 𝜃 = 300 than that of 𝜃 = 450. However, the ACI 318 code also gave a limit of
high value of 𝜃 = 600; the torsional resistance provided by longitudinal reinforcement is over
estimated when compared with the values gotten when 𝜃 = 450 𝑎𝑛𝑑 300. 𝜃 𝑣𝑎𝑙𝑢𝑒 for BS 8110
cannot be varied because the 𝜃 = 450 was built into the formulated equation for predicting
ultimate torsional moments. There is a continuation of tables 4.3 and 4.4 for Experimental
Amulu C. P., Ezeagu C. A. Page 62
verification of ultimate capacity of the tested beams and its interaction with torsion plus shear,
and torsion plus bending. Table 4.5 presents for comparison the experimental observed and
calculated ultimate torsional moments predicted by different classical theories; elastic, plastic,
Cowan and Skew-bending. The table indicated that values predicted by elastic and plastic
theories are the same through-out the beam specimens because of constant dimension of the
beams (fixed X and Y dimensions) respectively. The values predicted by Cowan’s equation are
over estimated by almost twice and are not conservative and consistent. The values observed
from experimental result are slightly higher than those predicted by skew-bending theory. In
other words, it is only skew-bending theory values that come closer to that obtained
experimentally. The values predicted by elastic and plastic theories are under estimated and over
conservative when compared with experimental result. This indicates that the failure of
reinforced concrete beam subjected to combined actions of torsion, shear and bending cannot be
attributed to the two theories. Tables 4.6 a and b presents for comparison the calculations from
(a) example1( the design of simply supported beam loaded eccentrically at a distance away from
the beams principal axis, but at the mid-span and (b) for precast footbridge slab (example 2). A
detailed calculation was done on a footbridge beam to determine the areas of reinforcement
required by BS 8110, ACI 318 and Euro code 2 to sustain torsional force.
From the table a, Euro code 2 gave values that are more conservative and consistence in
providing for the areas required for torsional resistance for both longitudinal and transverse
reinforcements. From table b, it can be observed that areas of longitudinal reinforcement
required for torsion is more conservative by the Euro code 2 predictions while ACI 318 code
value is higher. The area of transverse reinforcement required for torsion only is more
conservative in Euro code 2 than other two codes. In the combined action of torsion and shear,
Euro code 2 values are more conservative while ACI 318 has the highest value. However, for
combined torsion and bending, ACI 318 becomes more conservative while BS 8110 is the
highest. It is clear that using Euro code 2, the design will be more economical and conservative
than using ACI 318 and BS 8110. Figure 4.1 shows a graph of the ultimate torsional strengths
predicted by classical theories and that of the experimental result. From the figure, it can be
observed that Cowan’s predictions are over estimated while elastic and plastic theories gave the
over conservative values. The skew-bending theory values are the closest to the experimental
Amulu C. P., Ezeagu C. A. Page 63
result than any other theory. Figures 4.2 to 4.6 show a typical crack pattern for the various beam
samples from groups 1 to 5. The crack pattern in figure 4.2 indicated that the beam failed with
high cracking angle indicating no reinforcement in both longitudinal and transverse directions.
Figure 4.3 shows a crack pattern that has no provision for torsional reinforcement that is it
yielded as a result of bending stresses. While figures 4.4 to 4.6 show are crack pattern with
helical cracks inclined at an angle at an average of 𝜃 = 370.
Conclusions: The experimental investigation on the ultimate torsional strength of rectangular
cross-section reinforced concrete beams with plain, transverse and longitudinal reinforcement
subjected to combined actions of bending, shear and torsional stresses by using simple test
method was carried out. In this study, combined loading was achieved by applying an eccentric
load to the simply supported beams at the mid-span using universal testing machine. The
parameters in this study are eccentricity of the load which represents the magnitude of torsional
moment, variations in the amount of longitudinal and transverse reinforcements and given
compressive strength of concrete. The experimental results indicated that all beam specimens
failed by yielding of reinforcements or concrete crushing, or both after diagonal cracking which
is induced by the effect of combined actions of bending, shear and torsion. It can be concluded
that increase in the magnitude of ultimate torsional strength were as a result of increase in the
amount of longitudinal and transverse reinforcements. The comparison of the ultimate torsional
strength from the experimental results observed with the calculated values predicted by equations
of BS 8110, ACI 318 and Euro code 2 indicated that the codes studied in this work gave quite
consistent and conservative values in many cases while in few cases, uneconomic and non-
conservative results are obtained. This can be attributed to different values of 𝜃 specified by the
codes. Hence, it can be concluded that the value of angle of crack 𝜃 is not supposed to be fixed
as specified by the codes (𝜃 = 450), but a value that will ensure conservative and consistency in
providing the areas of reinforcement for both longitudinal and transverse direction. These values
should be between 300 𝑡𝑜 430 while lower values of 𝜃 = 220 should be used for highly stressed
reinforced concrete beams. 450 Value for 𝜃 was accepted generally based on the symmetric
arrangement of transverse reinforcements throughout the beam length. From the comparison of
ultimate torsional strengths predicted by different classical theories and experimental result, it
can be concluded that the classical theories were able to predict values that matches that of
Amulu C. P., Ezeagu C. A. Page 64
experimental result, except in Cowan that over estimated its values while elastic theory under
estimated its values and over economical/conservative. Therefore failure of reinforced concrete
beams subjected to combined actions of torsion, shear and bending cannot be attributed to elastic
theory. The plastic theory should also not be used as it gave a value smaller than that observed
experimentally.
Recommendations: This study recommends that the value of angle of cracks should not be fixed
at 𝜃 = 450, but a value that will ensure a better economic and stable design that is neither too
conservative nor over estimation. This 𝜃 value should be between 300 𝑡𝑜 430 while a lower
value may be used where applied stresses are expected to be high.
It also recommends that inclusion of torsional design for members that are subjected to
its effects, in design as increase in reinforcement due to torsional stresses in both longitudinal
and transverse directs of the beam increases the torsional strength and capacity of such beam.The
assumption taken in formulating the codes equations should be revisited, especially in the
improvement of strength capacity of concrete strut to resist torsion.
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