3. Modélisation A#

3.1. Caractéristiques de la modélisation#

Le modèle est composé de 10 éléments poutre droite d’Euler.

Section S1: section circulaire variable

à l’encastrement,

\(\mathrm{R1}=0.1m\) (section pleine)

à l’extrémité libre,

\(\mathit{R2}=0.05m\) (section pleine)

Section S2: section rectangulaire variable

à l’encastrement,

\({H}_{\mathit{y1}}=0.05m\)

\({H}_{\mathit{z1}}=0.10m\)

à l’extrémité libre,

\({H}_{\mathit{y2}}=0.05m\)

\({H}_{\mathit{z2}}=0.05m\)

Section S3 : section générale variable

à l’encastrement,

\({A}_{1}={10}^{2}{m}^{4}\)

\({I}_{\mathit{y1}}=8.3333{10}^{6}{m}^{4}\)

à l’extrémité libre,

\({A}_{2}=2.5{10}^{3}{m}^{2}\)

\({I}_{\mathit{y2}}=5.20833{10}^{7}{m}^{4}\)

3.2. Caractéristiques du maillage#

3 sections \(\times\) 10 éléments POU_D_E

3.3. Grandeurs testées et résultats#

Cas de charge

Section

Identification

Référence

Tolérance %

1

\(\mathit{S1}\)

\(u(l)\)

3.1831E–08

1.00E-05

\(n(0)\)

1.0000E+02

1.00E-05

\(n(l)\)

1.0000E+02

1.00E-05

\({\sigma}_{xx}(0)\)

3.1831E+03

1.00E-05

\({\sigma}_{xx}(l)\)

1.2732E+04

1.00E-05

2

\(\mathit{S1}\)

\(v(l)\)

4.2441E–06

1.00E-05

\({\theta}_{z}(l)\)

8.4882E–06

1.00E-05

\({v}_{y}(0)\)

1.0000E+02

1.00E-05

\({v}_{y}(l)\)

1.0000E+02

1.00E-05

\({\mathit{mf}}_{z}(0)\)

1.0000E+02

1.00E-05

\({\mathit{mf}}_{z}(l)\)

0.0000E+00

1.00E-05

\({\sigma}_{xx}(0)\)

1.2732E+05

1.00E-05

\({\sigma}_{xx}(l)\)

0.0000E+00

1.00E-05

3

\(\mathit{S1}\)

\({\theta}_{x}(l)\)

3.8621E–05

1.00E-05

\({m}_{x}(0)\)

1.0000E+02

1.00E-05

\({m}_{x}(l)\)

1.0000E+02

1.00E-05

4

\(\mathit{S1}\)

\(w(l)\)

–8.4882E–06

1.00E-05

\({\theta}_{y}(l)\)

2.9708E–05

1.00E-05

\({v}_{z}(0)\)

0.0000E+00

1.00E-05

\({v}_{z}(l)\)

0.0000E+00

1.00E-05

\({\mathit{mf}}_{y}(0)\)

1.0000E+02

1.00E-05

\({\mathit{mf}}_{y}(l)\)

1.0000E+02

1.00E-05

\({\sigma}_{xx}(0)\)

1.2732E+05

1.00E-05

\({\sigma}_{xx}(l)\)

1.0185E+06

1.00E-05

5

\(\mathit{S1}\)

\(u(l)\)

1.2296E–08

1.00E-02

\(n(0)\)

1.0000E+02

1.00E-05

\(n(l)\)

0.0000E+00

1.00E-03 (absolu)

\({\sigma}_{xx}(0)\)

3.1831E+03

1.00E-05

\({\sigma}_{xx}(l)\)

0.0000E+00

1.00E-03 (absolu)

6

\(\mathit{S1}\)

\(v(l)\)

1.3486E–06

1.00E-02

\({\theta}_{z}(l)\)

2.1220E–06

1.00E-02 (absolu)

\({v}_{y}(0)\)

1.0000E+02

1.00E-05

\({v}_{y}(l)\)

0.0000E+00

1.00E-03 (absolu)

\({\mathit{mf}}_{z}(0)\)

5.0000E+01

1.00E-02

\({\mathit{mf}}_{z}(l)\)

0.0000E+00

1.00E-03 (absolu)

\({\sigma}_{xx}(0)\)

6.3662E+04

1.00E-05

\({\sigma}_{xy}(0)\)

3.1831E+03

1.00E-05

Cas de charge

Section

Identification

Référence

Ecart %

1

\(\mathit{S2}\)

\(u(l)\)

1.3862E–07

1.00E-05

\(n(0)\)

1.0000E+02

1.00E-05

\(n(l)\)

1.0000E+02

1.00E-05

\({\sigma}_{xx}(0)\)

2.0000E+04

1.00E-05

\({\sigma}_{xx}(l)\)

4.0000E+04

1.00E-05

2

\(\mathit{S2}\)

\(v(l)\)

1.8969E–04

2.30E-02

\({\theta}_{z}(l)\)

3.0238E–04

2.70E-02

\({v}_{y}(0)\)

1.0000E+02

1.00E-05

\({v}_{y}(l)\)

1.0000E+02

1.00E-05

\({\mathit{mf}}_{z}(0)\)

1.0000E+02

1.00E-05

\({\mathit{mf}}_{z}(l)\)

0.0000E+00

1.00E-03 (absolu)

\({\sigma}_{xx}(0)\)

2.4000E+06

1.00E-05

\({\sigma}_{xx}(l)\)

0.0000E+00

1.00E-03 (absolu)

\({\sigma}_{xy}(0)\)

2.0000E+04

1.00E-05

\({\sigma}_{xy}(l)\)

4.0000E+04

1.00E-05

3

\(\mathit{S2}\)

\({\theta}_{x}(l)\)

8.3506E–04

5.70E-02

\({m}_{x}(0)\)

1.0000E+02

1.00E-05

\({m}_{x}(l)\)

1.0000E+02

1.00E-05

\({\sigma}_{xy}(0)\)

1.5600E+06

1.00E-05

\({\sigma}_{xy}(l)\)

4.0371E+06

5.00E-02

\({\sigma}_{xz}(0)\)

1.5600E+06

1.00E-05

\({\sigma}_{xz}(l)\)

4.0371E+06

5.00E-02

4

\(\mathrm{S2}\)

\(w(l)\)

–1.2000E–04

3.00E-03

\({\theta}_{y}(l)\)

3.600E–04

4.00E-03

\({v}_{z}(0)\)

0.0000E+00

1.00E-03 (absolu)

\({v}_{z}(l)\)

0.0000E+00

1.00E-03 (absolu)

\({\mathit{mf}}_{y}(0)\)

1.0000E+02

1.00E-05

\({\mathit{mf}}_{y}(l)\)

1.0000E+02

1.00E-05

\({\sigma}_{xx}(0)\)

1.2000E+06

1.00E-05

\({\sigma}_{xx}(l)\)

4.8000E+06

1.00E-05

5

\(\mathit{S2}\)

\(u(l)\)

6.1370E–08

1.00E-05

\(n(0)\)

1.0000E+02

1.00E-05

\(n(l)\)

0.0000E+00

1.00E-03 (absolu)

\({\sigma}_{xx}(0)\)

2.0000E+04

1.00E-05

\({\sigma}_{xx}(l/2)\)

1.3333E+04

1.00E-05

\({\sigma}_{xx}(l)\)

0.0000E+00

1.00E-03 (absolu)

6

\(\mathrm{S2}\)

\(v(l)\)

6.8626E–05

2.00E-02

\({\theta}_{z}(l)\)

9.4847E–05

2.40E-02

\({v}_{y}(0)\)

1.0000E+02

1.00E-05

\({v}_{y}(l)\)

0.0000E+00

1.00E-03 (absolu)

\({\mathrm{mf}}_{z}(0)\)

5.0000E+01

1.00E-02

\({\mathrm{mf}}_{z}(l)\)

0.0000E+00

1.00E-03 (absolu)

\({\sigma}_{xx}(0)\)

1.2000E+06

1.00E-05

\({\sigma}_{xx}(l)\)

0.0000E+00

1.00E-03 (absolu)

7

\(\mathrm{S3}\)

\(w(l)\)

–3.8259E–05

1.00E-02

\({\theta}_{y}(l)\)

5.7388E–05

1.00E-02

\({v}_{z}(0)\)

–4.4633E+02

1.00E-03

\({\mathrm{mf}}_{y}(0)\)

1.7535E+02

1.00E-02

3.4. Remarques#

La modélisation étant faite en poutres d’Euler, les coefficients de cisaillement sont \(\mathit{ky}=\mathit{kz}=1\) .