1
(cl Improved Fracture Behaviour of Thin Tungsten Foils Vladica Nikolić 1* , Stefan Wurster 2 , Reinhard Pippan 1 1 Erich Schmid Institute of Materials Science, Austrian Academy of Sciences, Leoben, Austria 2 Department of Materials Physics, Montanuniversität Leoben, Austria I Motivation II Why tungsten? III Results & Discussion IV Outlook References Future fusion reactors are associated with challenging operating conditions which will require the utilization of advanced materials with extreme mechanical, heat and neutron load capacities. Tungsten and tungsten based materials have been investigated in the last few years as potential candidates for divertor and plasma facing components. Tungsten is a metal with an interesting combination of many advantageous properties, which makes it a premium candidate for high temperature applications. W can be used as : structural material armour material LOW DBTT HIGH FRACTURE TOUGHNESS Problem?! Its inherent brittleness. A promising ductilization strategy is the synthesis of: Composite materials W laminates assembled from layers of thin tungsten foils (superior fracture behaviour!) [2] 99.97% pure tungsten foil, with a thickness of 100μm. Elongated grains along the rolling direction (RD). Pronounced texture with an orientation in (100)<011>. ITER Tokamak, Cadarache (France) [1] Investigated Material Sample Preparation Testing Procedure Crack initiation was done in the following steps: Samples were vacuum brazed (at 780°C and 1100°C) to steel holders using AgCu and Cu foils. Experiments were conducted taking into account several parameters: testing direction , , 45° to RD testing temperature -196°C to 800°C testing speed 0.4mm/min, 20mm/min = × × () This work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training programme 2014-2018 under grant agreement No 633053. The views and opinions expressed herein do not necessarily reflect those of the European Commission or those of the European Commission. Future experiments: Fracture experiments of potassium doped WVM. Annealed materials for investigating the fracture behaviour of recrystallized W foils. Two additional crack systems, with crack propagating perpendicular to the foil plane and within the foil plane. taken from [3] * corresponding author: [email protected] II Experimental work -196ºC RT 200ºC 400ºC 600ºC 800ºC K=16,4 Temperature [°C] diamond wire saw razor blade FIB Fracture mechanical tests were performed on an universal tensile testing device (Zwick). Testing at 400°C and above was performed in vacuum. Steel holder Tungsten foil Pre crack The stress intensity factor K is used in fracture mechanics to predict the stress state near the tip of a crack caused by loading. Conditional fracture toughness values K q were calculated from the maximum force. Fracture Toughness -196°C 200°C 400°C 600°C RT 800°C Fracture Surfaces K q [MPam 1/2 ] CTOD Measurements ~ × × 20μm An improved fracture behaviour Higher degree of deformation leads to higher toughness. Ductile brittle transition temperature (DBTT) of investigated crack system is expected to be at RT. Experimental results are in correlation with tensile experiments [4] of the same material. Decrease in toughness at high temperatures attributable to increase in in-plane toughness? [1] www.efda.org [2] J. Reiser et al, J. Nucl. Mat 423 (2012) 1-8 [3] Y. Murakami, Stress Intensity Factors Handbook, Volume 1, Pergamon Press [4] J. Reiser et al, J. Nucl. Mat 434 (2012) 357- 366 [5] T.L.Anderson, Fracture mechanics, 2nd edition, CRC Press brittle fracture (cleavage) F - maximum load A - area a - crack length F I - geom. factor α = a/W W - width delamination K=64,3 K=77,5 K=66,7 K=54,7 K=41,5 delamination delamination ductile ductile fracture ductile fracture 10μm 10μm 10μm 10μm 10μm 10μm The crack tip opening displacement (CTOD) is a parameter used to determine fracture toughness of materials that show some plastic deformation before failure occurs, causing the tip to stretch open. E - Young‘s modulus σ Y - tensile strength A stereophotogrammetric reconstruction of fracture surfaces done by analyzing scanning electron microscope (SEM) images. Digital Elevation Models (DEMs) of the investigated surface degree of deformation of the metallic fracture surface. taken from [5] 5 μm 5 μm

Improved Fracture Behaviour of Thin Tungsten Foils · 2019. 1. 21. · • The stress intensity factor K is used in fracture mechanics to predict the stress state near the tip of

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Page 1: Improved Fracture Behaviour of Thin Tungsten Foils · 2019. 1. 21. · • The stress intensity factor K is used in fracture mechanics to predict the stress state near the tip of

(cl

Improved Fracture Behaviour of Thin Tungsten Foils

Vladica Nikolić 1*, Stefan Wurster 2, Reinhard Pippan1

1 Erich Schmid Institute of Materials Science, Austrian Academy of Sciences, Leoben, Austria 2 Department of Materials Physics, Montanuniversität Leoben, Austria

I – Motivation II – Why tungsten?

III – Results & Discussion

IV – Outlook References

• Future fusion reactors are associated with challenging

operating conditions which will require the utilization of

advanced materials with extreme mechanical, heat and

neutron load capacities.

• Tungsten and tungsten based materials have been

investigated in the last few years as potential candidates for

divertor and plasma facing components.

• Tungsten is a metal with an interesting combination of many advantageous properties, which

makes it a premium candidate for high temperature applications. W can be used as :

structural material

armour material

LOW DBTT HIGH FRACTURE TOUGHNESS

• Problem?! Its inherent brittleness. A promising ductilization strategy is the synthesis of:

Composite materials W laminates assembled from layers of thin tungsten foils (superior fracture behaviour!) [2]

• 99.97% pure tungsten foil, with a thickness of 100μm.

• Elongated grains along the rolling direction (RD).

• Pronounced texture with an orientation in (100)<011>.

ITER Tokamak, Cadarache (France) [1]

Investigated Material Sample Preparation Testing Procedure

• Crack initiation was done in the following steps:

• Samples were vacuum brazed (at 780°C and 1100°C)

to steel holders using AgCu and Cu foils.

• Experiments were conducted taking into

account several parameters:

testing direction ∥ , ⊥, 45° to RD

testing temperature -196°C to 800°C

testing speed 0.4mm/min, 20mm/min

𝐾𝑞 =𝐹

𝐴× 𝜋 𝑎 × 𝐹𝐼(𝛼)

This work has been carried out within the framework of the EUROfusion Consortium and has received funding from the Euratom research and training programme 2014-2018 under grant agreement No 633053. The views and opinions expressed herein do not necessarily reflect

those of the European Commission or those of the European Commission.

• Future experiments:

Fracture experiments of potassium doped WVM.

Annealed materials for investigating the fracture behaviour of recrystallized W foils.

Two additional crack systems, with crack propagating perpendicular to the foil plane and within

the foil plane.

taken from [3]

* corresponding author: [email protected]

II – Experimental work

-196ºC

RT

200ºC

400ºC

600ºC

800ºC

K=16,4

Temperature [°C]

diamond – wire saw

razor blade

FIB

• Fracture mechanical tests were performed on an universal tensile

testing device (Zwick). Testing at 400°C and above was performed

in vacuum. Steel holder

Tungsten foil

Pre – crack

• The stress intensity factor K is used in fracture mechanics to predict the stress state near the tip of a crack caused by loading.

Conditional fracture toughness values Kq were calculated from the maximum force.

Fracture Toughness

-196°C

200°C

400°C

600°C

RT

800°C

Fracture Surfaces

Kq [

MP

am1

/2]

CTOD Measurements

𝐾𝑞~ 𝐶𝑇𝑂𝐷 × 𝜎𝑌 × 𝐸

20µm

• An improved fracture behaviour Higher degree of deformation leads to higher

toughness.

• Ductile – brittle transition temperature (DBTT) of investigated crack system is

expected to be at RT.

• Experimental results are in correlation with tensile experiments [4] of the same

material.

• Decrease in toughness at high temperatures attributable to increase in in-plane

toughness?

[1] www.efda.org

[2] J. Reiser et al, J. Nucl. Mat 423 (2012) 1-8

[3] Y. Murakami, Stress Intensity Factors

Handbook, Volume 1, Pergamon Press

[4] J. Reiser et al, J. Nucl. Mat 434 (2012) 357-

366

[5] T.L.Anderson, Fracture mechanics, 2nd

edition, CRC Press

brittle fracture (cleavage)

F - maximum load A - area

a - crack length FI - geom. factor

α = a/W W - width

delamination

K=64,3

K=77,5

K=66,7

K=54,7

K=41,5

delamination

delamination ductile

ductile fracture

ductile fracture

10µm

10µm

10µm

10µm

10µm

10µm

• The crack tip opening displacement (CTOD) is a parameter used to determine fracture toughness of materials that show some plastic deformation

before failure occurs, causing the tip to stretch open.

E - Young‘s modulus

σY - tensile strength

• A stereophotogrammetric reconstruction of fracture surfaces

done by analyzing scanning electron microscope (SEM)

images.

• Digital Elevation Models (DEMs) of the investigated surface

degree of deformation of the metallic fracture surface.

taken from [5]

5 µm 5 µm