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F. K. Kong MA, MSc, PhD, CEng, FICE, FIStructE, R. H. Evans CBE, DSc, D ès Sc, DTech, PhD, CEng, FICE, FIMechE, FIStructE (auth.)-Reinforced and Prestressed Concrete-Springer US (1987)

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224 Shear, bond and torsion

stresses. In the first and second editions (1975 and-1980 respectively) ofthis

book, the authors wrote: 'Provided the anchorage length is sufficient, the

local bond stress does not seem to have much significance.... It is

desirable that (the requirement to check) local bond stresses will be

dropped in future revisions of CP 110.'

6.7 Equilibrium torsion and compatibility torsion

BS 8110 implicitly differentiates between two types of torsion: equilibrium

torsion (or primary torsion), which is requi.red to maintain equilibrium in

the structure, and compatibility torsion (or secondary torsion), which is

required to maintain compatibility between members of the structure. To

distinguish between the two types, it is helpful to note that (a) in a statically

determinate structure, only equilibrium torsion can exist; (b) in an

indeterminate structure both types may exist, but if the torsion can be

eliminated by releasing redundant restraints then it is a compatibility

torsion.

In general, where the torsional resistance or stiffness of members has

not been explicitly taken into account in the analysis of the structure,

no specific ca1culations for torsion will be necesary. Thus, BS 8110:

Part 2: Clause 2.4.1 states that: 'In normal slab-and-beam or framed

construction specific ca1culations are not usually necessary, torsional

cracking being adequately controlled by shear reinforcement.' In other

words, compatibility torsion may, at the discretion of the designer, be

ignored in the design ca1culations; however, equilibrium torsion must be

designed for.

6.8 Torsion in plain concrete beams

It is only recently that a substantial amount of experimental data has

enabled engineers to obtain a reasonable working knowledge of torsion in

structural concrete [33-37].

Figure 6.8-1 shows a plain concrete beam subjected to pure torsion. The

torsional moment T induces shear stresses which produce principal tensile

stresses at 45° to the longitudinal axis. When the maximum tensile stress

reaches the tensile strength of the concrete, diagonal cracks form which

tend to spiral round the beam [38). For a plain concrete beam, failure

immediately follows such diagonal cracking.

Fig. 6.8-1 Diagonal cracking due to torsion [38]

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