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EUROCODE 2 WORKED EXAMPLES - Federbeton

EUROCODE 2 WORKED EXAMPLES - Federbeton

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EC2 – worked examples 7-16<br />

0.1687 ⎛ 0.0223 ⎞<br />

σ s,cr = 0.6⋅3.086⋅ ⋅ ⎜1+ 15⋅ ⎟=<br />

41.78 MPa<br />

0.0223 ⎝ 0.1687 ⎠<br />

160 ⎛ 41.78 ⎞ ⎛ 0.1687 ⎞<br />

w k = ⋅ 1 3.4 50 0.17 26 0.12 mm<br />

5 ⎜ − ⎟⋅⎜ ⋅ + ⋅ ⋅ ⎟=<br />

2 ⋅10 ⎝ 160 ⎠ ⎝ 0.0223 ⎠<br />

The obtained values are in good agreement with those evaluated within the design.<br />

The values from the verification are slightly larger because of the fact that in the considered<br />

section the internal drive lever arm is lower than the approximated value 0.9d assumed in the<br />

approximated design procedure. In fact, being h0/d the adimensional lever arm in units of<br />

effective height d, in the three case we have<br />

kw = 1 h0/d = (43.70 – 19.59/3) / 43.70 = 0.85<br />

kw = 2/3 h0/d = (43.70 – 21.46/3) / 43.70 = 0.836<br />

kw = 1/3 h0/d = [(18·160·18.99 + 3·160·13.79 2 /18.99) / (18·160 + 3·160·13.79/18.99) +<br />

+ 2/3·24.71] / 43.70 ≅ 0.8<br />

Let’s remark that the presence of a compressed reinforcement is highly recommended to<br />

make ductile the section in the ultimate limit state. The reinforcement increase the lever arm<br />

of the section reducing the difference between the approximated values and those coming<br />

from the verification. The approximated method previously discussed can be successfully<br />

applied in the design of the ultimate crack state.<br />

The obtained results are reported in the Tables 7.1 and 7.2 and they are shown in Figure 7.9.<br />

Table 7.3 and Figure 7.10 report numerical values and graphs for the maximal diameter and<br />

the required reinforcement expressed as a function of fixed values for σs. Stating a suitable<br />

precision for the approximated method, those values are evaluated using the (7.16) (7.14).<br />

Table 7.1. Approximated method. Table 7.2. Exact method.<br />

w k (mm) A s (mm 2 ) σ s (MPa) h 0/d A s (mm 2 ) w k (mm) σ s (MPa) h 0/d<br />

0.1 11151 140 0.9 11151 0.120 160 0.811<br />

0.2 6903 221 0.9 6903 0.213 238 0.836<br />

0.3 5310 190 0.9 5310 0.306 304 0.85<br />

Table of Content<br />

Fig. 7.9. Comparison between the exact and approximated methods.

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