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Universit`a degli Studi di Padova
Analisi del comportamento dinamico di funi metalliche
spiroidali a seguito dell’applicazione di piccoli intagli
Relatore
Prof. Ing. Stefano Secchi
Candidato
Marco Caneve
20 aprile 2016
Introduzione:
• Possibile tranciamento completo
Lavori precedenti:
• Contri, Secchi - Snapping of ropes under stress - 2002.
• Contri, Secchi, Vitaliani - Recisione di funi sotto sforzo, a seguito di
piccoli intagli applicati bruscamente - Aimeta - Dicembre 2000;
2 di 21
Modello analitico:
• G2
ER3
2
= π
4 R2∆κ2
• H2
ER3
2
= π
4(1+ν) R2∆τ2
• T2
ER2
2
= πξ2
• N2
ER2
2
= H2
ER3
2
cos2
α2
r2/R2
−
G2
ER3
2
sin α2 cos α2
r2/R2
• X2
ER2
2
=
N2
ER2
2
sin α2 cos α2
r2/R2
− T2
ER2
2
cos2
α2
r2/R2
• F2
ER2
2
= m2
T2
ER2
2
sin α2 +
N2
ER2
2
cos α2
• F1
ER2
1
= πξ1
• Ftot = F1 + F2
[G.A Costello]
Validazione > Caso generale
3 di 21
Modello numerico:
R1 1.20 mm
R2 1.15 mm
r2 2.35 mm
α2 78.93 ◦
E 206000 MPa
passo 12 Φnom
p2 75.46 mm
Anom 31.06 mm2
Φnom 6.29 mm
A1 4.52 mm2
A2 4.15 mm2
Fr,1 7031.48 N
Fr,2 6457.73 N
Elementi ”trave”
Con formulazione dinamica in grandi
spostamenti (Updated Lagrangian)
Contatto
L 1000 Φnom
30000 nodi. 180000 gradi di libert`a
∆t = 10E-06 s 4 di 21
Validazione modello numerico:
p2
Φnom
∆zteoria ∆znum ∆
mm mm
10 17,49 17,64 0,85%
12 16,99 17,10 0,69%
14 16,66 16,74 0,50%
16 16,43 16,50 0,44%
p2
Φnom
Fext,teoria Fext,num ∆
N N
10 3501,5 3530,5 0,83%
12 3467,9 3489,4 0,62%
14 3442,0 3459,6 0,51%
16 3421,9 3435,9 0,41%
5 di 21
Analisi dinamica:
Variabili:
• A: Forza di pretensione;
• B: Coefficiente d’attrito;
• C: Diagramma costitutivo del
materiale.
F60 F70 F80 F90 F100
r,1 • • • • •
r,2 • • • •
r,3 • • •
r,4 • •
6 di 21
Procedura di calcolo:
7 di 21
Comportamento dinamico:
• Materiale elastico lineare:
8 di 21
Comportamento dinamico:
Materiale lineare Materiale elasto-plastico
9 di 21
Comportamento dinamico:
• Rottura:
10 di 21
Comportamento dinamico:
11 di 21
Confronto risultati al variare della forza di pretensione:
Andamento della forza assiale nel filo numero 3:
12 di 21
Confronto risultati al variare del coefficiente d’attrito:
13 di 21
Confronto al variare del diagramma costitutivo:
14 di 21
Dominio di rottura:
Casi limite:
• attrito nullo, deformazione
ultima infinita (non rottura);
• attrito infinito, materiale
elastico-lineare (rottura).
15 di 21
Interpretazione geometrica:
• EJmin = fili
E πR4
4
sin α2
• EJstick = fili
EA(r sin φ)2 sin3 α2
• EJslip =
fili
σT A(eµ sin α2φ
− 1)r sin φ sin α2/κ
• EJmax = fili
EJmin + EJstick = costante
• EJ = fili
EJmin + EJslip
16 di 21
Analisi energetica:
17 di 21
Analisi energetica:
18 di 21
Analisi energetica:
19 di 21
Conclusioni:
• Parametri che favoriscono la rottura:
◦ Forza di pretensione ↑;
◦ Coefficiente d’attrito ↑;
◦ Diagramma costitutivo (deformazione ultima) ↓.
• Interpretazione geometrica: la rottura `e causata dall’eccentricit`a
che si crea fra il nuovo e il vecchio baricentro;
• Interpretazione energetica: la rottura corrisponde a bassa
dissipazione e alti gradienti di energia al variare dell’ascissa.
20 di 21
GRAZIE PER L’ATTENZIONE
21 di 21

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Analysis of the dynamic behavior of spiral strands as a result of the application of small cuts

  • 1. Universit`a degli Studi di Padova Analisi del comportamento dinamico di funi metalliche spiroidali a seguito dell’applicazione di piccoli intagli Relatore Prof. Ing. Stefano Secchi Candidato Marco Caneve 20 aprile 2016
  • 2. Introduzione: • Possibile tranciamento completo Lavori precedenti: • Contri, Secchi - Snapping of ropes under stress - 2002. • Contri, Secchi, Vitaliani - Recisione di funi sotto sforzo, a seguito di piccoli intagli applicati bruscamente - Aimeta - Dicembre 2000; 2 di 21
  • 3. Modello analitico: • G2 ER3 2 = π 4 R2∆κ2 • H2 ER3 2 = π 4(1+ν) R2∆τ2 • T2 ER2 2 = πξ2 • N2 ER2 2 = H2 ER3 2 cos2 α2 r2/R2 − G2 ER3 2 sin α2 cos α2 r2/R2 • X2 ER2 2 = N2 ER2 2 sin α2 cos α2 r2/R2 − T2 ER2 2 cos2 α2 r2/R2 • F2 ER2 2 = m2 T2 ER2 2 sin α2 + N2 ER2 2 cos α2 • F1 ER2 1 = πξ1 • Ftot = F1 + F2 [G.A Costello] Validazione > Caso generale 3 di 21
  • 4. Modello numerico: R1 1.20 mm R2 1.15 mm r2 2.35 mm α2 78.93 ◦ E 206000 MPa passo 12 Φnom p2 75.46 mm Anom 31.06 mm2 Φnom 6.29 mm A1 4.52 mm2 A2 4.15 mm2 Fr,1 7031.48 N Fr,2 6457.73 N Elementi ”trave” Con formulazione dinamica in grandi spostamenti (Updated Lagrangian) Contatto L 1000 Φnom 30000 nodi. 180000 gradi di libert`a ∆t = 10E-06 s 4 di 21
  • 5. Validazione modello numerico: p2 Φnom ∆zteoria ∆znum ∆ mm mm 10 17,49 17,64 0,85% 12 16,99 17,10 0,69% 14 16,66 16,74 0,50% 16 16,43 16,50 0,44% p2 Φnom Fext,teoria Fext,num ∆ N N 10 3501,5 3530,5 0,83% 12 3467,9 3489,4 0,62% 14 3442,0 3459,6 0,51% 16 3421,9 3435,9 0,41% 5 di 21
  • 6. Analisi dinamica: Variabili: • A: Forza di pretensione; • B: Coefficiente d’attrito; • C: Diagramma costitutivo del materiale. F60 F70 F80 F90 F100 r,1 • • • • • r,2 • • • • r,3 • • • r,4 • • 6 di 21
  • 8. Comportamento dinamico: • Materiale elastico lineare: 8 di 21
  • 9. Comportamento dinamico: Materiale lineare Materiale elasto-plastico 9 di 21
  • 12. Confronto risultati al variare della forza di pretensione: Andamento della forza assiale nel filo numero 3: 12 di 21
  • 13. Confronto risultati al variare del coefficiente d’attrito: 13 di 21
  • 14. Confronto al variare del diagramma costitutivo: 14 di 21
  • 15. Dominio di rottura: Casi limite: • attrito nullo, deformazione ultima infinita (non rottura); • attrito infinito, materiale elastico-lineare (rottura). 15 di 21
  • 16. Interpretazione geometrica: • EJmin = fili E πR4 4 sin α2 • EJstick = fili EA(r sin φ)2 sin3 α2 • EJslip = fili σT A(eµ sin α2φ − 1)r sin φ sin α2/κ • EJmax = fili EJmin + EJstick = costante • EJ = fili EJmin + EJslip 16 di 21
  • 20. Conclusioni: • Parametri che favoriscono la rottura: ◦ Forza di pretensione ↑; ◦ Coefficiente d’attrito ↑; ◦ Diagramma costitutivo (deformazione ultima) ↓. • Interpretazione geometrica: la rottura `e causata dall’eccentricit`a che si crea fra il nuovo e il vecchio baricentro; • Interpretazione energetica: la rottura corrisponde a bassa dissipazione e alti gradienti di energia al variare dell’ascissa. 20 di 21