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Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

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Page 1: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Fracture of Divertor StructuresJake BlanchardARIES MeetingApril 2011

Page 2: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

OutlinePrimer on Fracture MechanicsPreliminary Results for Divertor

StructuresFuture Plans

Page 3: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Design of Engineering StructuresIn early 20th century, design of

metal structures was strictly stress based

Onset of high performance ships (Liberty ships, WWII) changed things

Page 4: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

What happened?

stress

Temperature

fracture

Low strength

high strength

Page 5: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Fracture MechanicsSize and Orientation of CracksStress FieldsMaterial Properties

Page 6: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Crack Tip Stress Fields (Elastic)Consider a sharp crack in an

elastic material

K is stress intensity factorFunction of geometry and

loadingFracture occurs when K

reaches critical value (KIC – fracture toughness)

r

Page 7: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

An ExampleConsider an infinite plate with a

through crack

a

K

KaK

ICallow

ICI

Glass: KIC=1 MPa-m0.5

Al: KIC=20 MPa-m0.5

For a=100 microns, fracture stresses are 56 MPa for glass and 1,100 MPa for Al

Page 8: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Fracture Toughness (room temp)

Material Toughness (MPa – m^0.5)

7075 Aluminum 24

4340 Steel 50

Silicon Carbide 4

Polystyrene 1

Tungsten (polycrystalline) 5

Beryllium 10

These values depend strongly on processing.

Page 9: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Ductile vs. Brittle

Page 10: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Temperature Dependence

Page 11: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Stress Fields in Ductile MaterialsDuctile materials will develop

plastic deformation at crack tipsThis toughens material and resists

catastrophic crack growthPrevious analysis is not validAnalysis uses integral around crack

tip, rather than stress intensity factor

Page 12: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Failure Criterion for Ductile MaterialsBase failure

prediction on work required to create fresh fracture surface

Write as line integral

EKJ

dsx

utWdxJ

ICIC

I

3

1 22

12

W=strain energy densityT=tractionsU=displacement

Page 13: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Irradiated Materials

Page 14: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Fatigue Crack GrowthPrevious analyses refer to

catastrophic, unstable crack growth

Repeated application of loads can lead to incremental crack growth

Page 15: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Characterizing CracksKey Question: What is initial crack

size?We need non-destructive examination

(NDE)Options:

◦Dye penetrant◦Ultrasound◦X-rays◦Eddy currents◦Thermography◦Etc.

Costs and capabilities vary

Page 16: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

ITER Structural Design CriteriaPrimary Loads

Primary + Secondary Loads

Elasto-Plastic Analysis

CI KK 33.0

CI KK 67.0

CI JJ 67.0

Page 17: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

ANSYS Finite Element Model of Circumferential Crack

Crack face

• Stress intensities along crack face using the ANSYS CINT command• Elastic-Plastic material properties for Tungsten used• Currently only pressure loads are considered, but thermal stresses to be included

Page 18: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Initial Fracture Studies Based on T-Tube Geometry and Pressure Loads

t = 1 mm

OD = 15 mm

Coolant pressure ~ 10 MpaCoolant inlet temperature ~ 600 oC

Tungsten

Page 19: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Initial Studies Compute Stress Intensities for Axial Cracks in Pressurized Cylinder

Case 1: Circular crack; c/a=1

Case 2: Elliptical crack; c/a=2

Use elastic-plastic propertiesfor tungsten.

Calculate J1 and then reportequivalent KI.

Page 20: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Variation of Stress Intensity with Location along Crack Tip (a = 0.1 mm)

f

Case 1: Circular crack; c/a=1

Case 2: Elliptical crack; c/a=2

a = 0.1mm

0 15 30 45 60 75 900.8

0.9

1

1.1

1.2

1.3

cylindrical

elliptical

( )f degrees

K1 (

MP

a-m

1/2

)

Page 21: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

Maximum Stress Intensity as a Function of Crack Depth

0 0.1 0.2 0.3 0.4 0.5 0.60

0.5

1

1.5

2

2.5

3

3.5

Cylindrical

Elliptical

Crack Depth (mm)

K1 (

MPa-m

1/2

)

Page 22: Fracture of Divertor Structures Jake Blanchard ARIES Meeting April 2011

ConclusionsWe’ve got to include fracture in

our design analysis, particularly when using materials with limited ductility

So far, there are no major red flags

We will include thermal stresses in the future