EUROCODE 2 WORKED EXAMPLES - Federbeton
EUROCODE 2 WORKED EXAMPLES - Federbeton
EUROCODE 2 WORKED EXAMPLES - Federbeton
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
EC2 – worked examples 6-19<br />
nodes tensioned – compressed by anchor logs in a fixed direction<br />
⎛ fck<br />
⎞<br />
⎜1- ⎟<br />
250 35<br />
σ 2Rd,max = k<br />
⎝ ⎠ ⎛ ⎞<br />
2 f cd = ⎜1-⎟19.83 = 17.05 N / mm<br />
0.85 ⎝ 250 ⎠<br />
nodes tensioned – compressed by anchor logs in different directions<br />
⎛ fck<br />
⎞<br />
⎜1- ⎟<br />
250<br />
35<br />
σ 3Rd,max = k<br />
⎝ ⎠ ⎛ ⎞<br />
3 f cd = 0.88 ⎜1-⎟19.83 = 15 N / mm<br />
0.85 ⎝ 250 ⎠<br />
Actions<br />
F Ed = 700 kN<br />
Load eccentricity with respect to the column side: e = 125 mm (Fig. 6.8)<br />
The beam vertical strut width is evaluated by setting the compressive stress equal to σ1Rd,max:<br />
x1= σ<br />
FEd 700000<br />
= ≅87<br />
mm<br />
b 20.12⋅ 400<br />
1Rd,max<br />
the node 1 is located x1/2 ≅ 44 mm from the outer column side (Fig. 6.9)<br />
We state that the upper reinforcement is located 40 mm from the upper cantilever side; the<br />
distance y1 of the node 1 from the lower border is evaluated setting the internal drive arm z<br />
equal to 0.8⋅d (z = 0,8⋅360 = 288 mm):<br />
y1 = 0.2d = 0.2·360 = 72 mm<br />
rotational equilibrium: FEda Fz c<br />
Table of Content<br />
700000 ⋅ (125 + 44) = F ⋅ 288<br />
= c<br />
700000 ⋅ (125 + 44)<br />
Fc = Ft = = 410763 N ≅ 411 kN<br />
288<br />
node 1verification:<br />
F 411000<br />
c<br />
2 2<br />
σ = = = 7.14 N/mm ≤ σ1Rd,max = 20.12 N/mm<br />
b ( 2 y1 ) 400 ( 2⋅ 72)<br />
Main upper reinforcement design:<br />
F 411000<br />
A 1050 mm<br />
t<br />
2<br />
s = = = we use 8φ14 (As = 1232 mm<br />
fyd 391.3<br />
2 )<br />
Secondary upper reinforcement design:<br />
The beam proposed in EC2 is indeterminate, then it is not possible to evaluate the stresses for<br />
each single bar by equilibrium equations only, but we need to know the stiffness of the two<br />
elementary beams shown in Fig. 6.10 in order to make the partition of the diagonal stress<br />
⎛ Fc<br />
FEd<br />
⎞<br />
⎜Fdiag<br />
= = ⎟ between them;<br />
⎝ cosθ senθ ⎠<br />
2<br />
2