f.m. with finite element analysis - wall elliptical crack, sub- clad

34
Task 6 - Safety Review and Licensing On the Job Training on Stress Analysis Pisa (Italy) June 15 – July 14, 2015 F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad semielliptical crack and Elastic-Plastic calculation of the J parameter (ANSYS Workbench/ Apdl) Davide Mazzini – Ciro Santus

Upload: lamhuong

Post on 03-Jan-2017

229 views

Category:

Documents


3 download

TRANSCRIPT

Page 1: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

Task 6 - Safety Review and LicensingOn the Job Training on Stress Analysis

Pisa (Italy)June 15 – July 14, 2015

F.M. with Finite Element analysis - Wall Elliptical crack, Sub-Clad semielliptical crack and Elastic-Plastic calculation of the

J parameter (ANSYS Workbench/ Apdl)Davide Mazzini – Ciro Santus

Page 2: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

2

Content

• Calculation example of a wall subsurface Elliptical crack

• The effect of the cladding properties on a semielliptical sub-clad

surface crack, ANSYS Workbench

• J parameter calculation with ANSYS Workbench with Elastic-Plastic

material

Table of content

Pisa, June 15 – July 14, 2015

Page 3: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

3

Definition of the problem

Half model (symmetry), with an elliptical shape crack

ANSYS Workbench

0

25mm60 mm

30 mm

2 15 mm2 30 mm

100 MPa

tWh

ac

t

W h

2a2b

Pisa, June 15 – July 14, 2015

Page 4: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

4

Solution with Tetrahedrons mesh

ANSYS Workbench

Refinement at the two most significant points

Solution accurate, however tetrahedrons not ok for the CINT command

Pisa, June 15 – July 14, 2015

Page 5: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

5

Solution with Hexahedrons mesh

ANSYS Workbench

The model is divided into solids for keep Hexahedrons mesh near the crack front

Pisa, June 15 – July 14, 2015

Page 6: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

6

Mesh options

ANSYS Workbench

The Hex dominant option works with this

toroid shape

Pisa, June 15 – July 14, 2015

Page 7: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

7

Solution

ANSYS Workbench

Symmetry boundary up to the crack front

Accurate solution

Pisa, June 15 – July 14, 2015

Page 8: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

8

CINT,SIFS calculation

ANSYS Workbench

Coordinate systems introduced in Workbench then useful for the CINT calculation in ANSYS Apdl

Pisa, June 15 – July 14, 2015

Page 9: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

9

CINT,SIFS calculation

ANSYS Workbench

Coordinate systems 12Coordinate systems 13

Pisa, June 15 – July 14, 2015

Page 10: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

10

CINT,SIFS calculation

ANSYS Workbench

Pisa, June 15 – July 14, 2015

Page 11: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

11

CINT,SIFS calculation

ANSYS Workbench

- Unreliable values at the boundary of the crack front- Outer contours interact with the boundary of the toroid volume

Pisa, June 15 – July 14, 2015

Page 12: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

12

ANSYS Apdl command in the Workbench environment

ANSYS Workbench

Pisa, June 15 – July 14, 2015

Page 13: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

13

Results verification through handbook

ANSYS Workbench

0

25mm30 mm

2 15 mm2 30 mm

100 MPa

th

ac

/ 0/ 2

2 / 0.6

e tc a

a t

AI 0

I

492 MPa mm

(ANSYS Wb, 3D) 475MPa mmOk!possibileeffect of the limited width

mK f a

K

Pisa, June 15 – July 14, 2015

Page 14: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

14

Content

• Calculation example of a wall subsurface Elliptical crack

• The effect of the cladding properties on a semielliptical sub-clad

surface crack, ANSYS Workbench

• J parameter calculation with ANSYS Workbench with Elastic-Plastic

material

Table of content

Pisa, June 15 – July 14, 2015

Page 15: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

15Pisa, June 15 – July 14, 2015

Sub-clad surface semielliptical crack

The model

Wall

Clad

Crack only on the wall part

Page 16: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

16

Sub-clad surface semielliptical crack

The model

Hide a body to pick any other surface behind

Create the surface semielliptical crack through the usual steps

Pisa, June 15 – July 14, 2015

Page 17: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

17

Sub-clad surface semielliptical crack

The model

The attachment between the wall and the clad cannot be continuous across the entire surface

A circle can give a dimension of the discontinuity between the two parts

Pisa, June 15 – July 14, 2015

Page 18: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

18

Sub-clad surface semielliptical crack

SIF results

First result can be obtained without any connection between the two parts

Pisa, June 15 – July 14, 2015

Page 19: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

19

Sub-clad surface semielliptical crack

SIF results

Then calculation is repeated with connection outside the circle

Pisa, June 15 – July 14, 2015

Page 20: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

20

Sub-clad surface semielliptical crack

SIF results

Finally the full surface connection can be activated, after imposing plastic properties of the clad

Clad Elastic-Plastic properties

Pisa, June 15 – July 14, 2015

Page 21: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

21

Sub-clad surface semielliptical crack

SIF results

Finally the full surface connection can be activated, after imposing plastic properties of the clad

Pisa, June 15 – July 14, 2015

Page 22: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

22

Sub-clad surface semielliptical crack

SIF result comparison

I 510MPa mmK I 426 MPa mmK I 369MPa mmK

Which one is the most realistic result?

Pisa, June 15 – July 14, 2015

Page 23: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

23

Content

• Calculation example of a wall subsurface Elliptical crack

• The effect of the cladding properties on a semielliptical sub-clad

surface crack, ANSYS Workbench

• J parameter calculation with ANSYS Workbench with Elastic-Plastic

material

Table of content

Pisa, June 15 – July 14, 2015

Page 24: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

24

J parameter as an option of the Wb automatic Crack tool

Elastic calculation – Relation between KI and J

CT specimen example

2I

22I

(ANSYS) 782MPa mm (ANSYS) 2.786 mJ/mmConversion, validation: 200000MPa, 0.3

2.782mJ/mm OK!

K JE

KJE

Pisa, June 15 – July 14, 2015

Page 25: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

25

Elastic-Plastic steel, Bilinear Isotropic Hardening

CT specimen example

Pisa, June 15 – July 14, 2015

Page 26: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

26Pisa, June 15 – July 14, 2015

Elastic-Plastic steel, Bilinear Isotropic Hardening

CT specimen example

Page 27: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

27

Elastic-Plastic steel, Bilinear Isotropic Hardening

CT specimen example

2

2

Sameload , Elastic-Plastic material:(ANSYS) 2.748mJ/mm

Previous (just Elastic):(ANSYS) 2.786 mJ/mm

% 1.4%

PJ

J

Pisa, June 15 – July 14, 2015

Page 28: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

28

Elastic-Plastic steel, Bilinear Isotropic Hardening

CT specimen example

I(II,III)

I

I

Sameload , Elastic-Plastic material: is also calculated,

though theoretically not available(just the output of CINT,SIFS command)

(ANSYS) 800MPa mm

Previous (just Elastic):

(ANSYS) 782MPa mm

% 2.3

PK

K

K

%

Pisa, June 15 – July 14, 2015

Page 29: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

29

Small Scale Yielding

CT specimen example

I and similar values,with respect to theprevious just elastic calculation,due to the very smallplastic region

K J

Pisa, June 15 – July 14, 2015

Page 30: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

30

Increasing load – Multiple time step simulation

CT specimen example

Pisa, June 15 – July 14, 2015

Page 31: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

31

Increasing load – Multiple time step simulation

Non linear analysis – iterative solution

CT specimen example

Pisa, June 15 – July 14, 2015

Page 32: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

32

Increasing load – Multiple time step simulation

Increasingly discrepancy of KI with respect to J

CT specimen example

Elastic-Plastic, ANSYS WorkbenchS_Y, MPa B, mm

500 12P, kN K_I, MPa mm^0.5 J, mJ/mm^2 K_I, from J Delta % B_min for Pl. Strain

10 800 2.748 777 -2.9 6.0 => Pl. Strain20 1969 11.25 1572 -25.2 24.7 => Pl. Stress30 3712 27.32 2450 -51.5 60.0 => Pl. Stress40 6269 56.85 3535 -77.4 124.9 => Pl. Stress

ReliableUnreliable Equivalence

Pisa, June 15 – July 14, 2015

Page 33: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

33

Increasing load – Multiple time step simulation

Plastic region size

CT specimen example

2

Imin

Y

2

Ip

Y

10 kN 12mm

2.5 6.0mm

Pla

0.26m

ne st

m

rain

13

P B

KBS

KrS

2.0 mm

Pisa, June 15 – July 14, 2015

Page 34: F.M. with Finite Element analysis - Wall Elliptical crack, Sub- Clad

34

Increasing load – Multiple time step simulation

Plastic region size

CT specimen example

2

Imin

Y

2

Ip

Y

40 kN 12 mm

2.5 124.

Plane stress

1

9 mm

15.9mm

P B

KBS

KrS

2

I

Y

LEFM validity for Pl. Stress satnot isfied:

430 mm 57.9mmKaS

p 5 6mmr

Load <<80%offully plastic valueOk the useof J

Pisa, June 15 – July 14, 2015