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4.2 - VSL

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For complicated structural systems, the<br />

determining mechanisms have to be found.<br />

Descriptions of such mechanisms are<br />

available in the relevant literature, e.g. [31],<br />

[36].<br />

In special cases with irregular plan shape,<br />

recesses etc., simple equilibrium considerations<br />

(static method) very often prove to be a<br />

suitable procedure. This leads in the simplest<br />

case to the carrying of the load by means of<br />

beams (beam method). The moment<br />

distribution according to the theory of elasticity<br />

may also be calculated with the help of<br />

computer programmes and internal stress<br />

states may be superimposed upon these<br />

moments. The design has then to be done<br />

according to Method A.<br />

3.12. Ultimate stength of a<br />

cross-section<br />

For given dimensions and concrete qualities,<br />

the ultimate strength of a cross-section is<br />

dependent upon the following variables:<br />

- Ordinary reinforcement<br />

- Prestressing steel, bonded or unbonded<br />

- Membrane effect<br />

The membrane effect is usually neglected<br />

when determining the ultimate strength. In<br />

many cases this simplification constitutes a<br />

considerable safety reserve [8], [10].<br />

The ultimate strength due to ordinary<br />

reinforcement and bonded post-tensioning<br />

can be calculated on the assumption,<br />

which in slabs is almost always valid, that<br />

the steel yields, This is usually true also for<br />

cross-sections over intermediate columns,<br />

where the tendons are highly concentrated.<br />

In bonded post- tensioning, the prestressing<br />

force in cracks is transferred to the concrete<br />

by bond stresses on either side of the crack .<br />

Around the column mainly radial cracks open<br />

and a tangentially acting concrete<br />

compressive zone is formed. Thus the<br />

so-called effective width is considerably<br />

increased [27]. In unbonded post-tensioning,<br />

the prestressing force is transferred to the<br />

concrete by the end anchorages and, by<br />

approximation, is therefore uniformly<br />

distributed over the entire width at the<br />

columns.<br />

Figure 27: Tendon extension without lateral restraint Figure 28: Tendon extension with rigid lateral restraint<br />

8<br />

Figure 26: ultimate strenght of a<br />

cross-section (plastic moment)<br />

For unbonded post-tensioning steel, the<br />

question of the steel stress that acts in the<br />

ultimate limit state arises. If this steel stress is<br />

known (see Chapter 3.1.3.), the ultimate<br />

strength of a cross-section (plastic moment)<br />

can be determined in the usual way (Fig. 26):<br />

m u =z s . (d s - xc ) + z p . (d p - xc) (3.9)<br />

2 2<br />

where<br />

z S= A S . fsy (3.10.)<br />

z p = A p .(σ p∞ + ∆σ p ) (3.11.)<br />

x c =<br />

zs + zp (3.12.)<br />

b . f cd<br />

3.1.3. Stress increase in unbonded<br />

post-tensioned steel<br />

Hitherto, the stress increase in the unbonded<br />

post-tensioned steel has either been<br />

neglected [34] or introduced as a constant<br />

value [37] or as a function of the<br />

reinforcement content and the concrete<br />

compressive strength [38].<br />

A differentiated investigation [10] shows that<br />

this increase in stress is dependent both upon<br />

the geometry and upon the deformation of the<br />

entire system. There is a substantial<br />

difference depending upon whether a slab is<br />

laterally restrained or not. In a slab system,<br />

the internal spans may be regarded as slabs<br />

with lateral restraint, while the edge spans in<br />

the direction perpendicular to the free edge or<br />

the cantilever, and also the corner spans are<br />

regarded as slabs without lateral restraint.<br />

In recent publications [14], [15], [16], the<br />

stress increase in the unbonded post-<br />

tensioned steel at a nominal failure state is<br />

estimated and is incorporated into the<br />

calculation together with the effective stress<br />

present (after losses due to friction, shrinkage,<br />

creep and relaxation). The nominal failure<br />

state is established from a limit deflection au .<br />

With this deflection, the extensions of the<br />

prestressed tendons in a span can be<br />

determined from geometrical considerations.<br />

Where no lateral restraint is present (edge<br />

spans in the direction perpendicular to the free<br />

edge or the cantilever, and corner spans) the<br />

relationship between tendon extension and<br />

the span I is given by:<br />

∆I<br />

= 4 . au . yp =3 . au . dp (3.13.)<br />

I I I I I<br />

whereby a triangular deflection diagram and<br />

an internal lever arm of yp = 0.75 • d, is<br />

assumed The tendon extension may easily<br />

be determined from Fig. 27.<br />

For a rigid lateral restraint (internal spans) the<br />

relationship for the tendon extension can be<br />

calculated approximately as<br />

∆I<br />

=2 .( au . ) 2 +4 . au . hp I I I I<br />

(3.14.)<br />

Fig. 28 enables the graphic evaluation of<br />

equation (3.14.), for the deviation of which we<br />

refer to [10]<br />

The stress increase is obtained from the<br />

actual stress-strain diagram for the steel and<br />

from the elongation of the tendon ∆I<br />

uniformly distributed over the free length L of<br />

the tendon between the anchorages. In the<br />

elastic range and with a modulus of elasticity<br />

E p for the prestressing steel, the increase in<br />

steel stress is found to be<br />

∆σ p = ∆I . I . E p = ∆I . E p (3.15)<br />

I L L<br />

The steel stress, plus the stress increase ∆σ p<br />

must, of course, not exceed the yeld strength<br />

of the steel.<br />

In the ultimate load calculation, care must be<br />

taken to ensure that the stress increase is<br />

established from the determining mechanism.<br />

This is illustaced diagrammatically

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