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THE IMPACT OF MATERIALS R&D ON THE OPERATION OF A WATER-COOLED DEMO DIVERTOR …

M. Rieth, S. Antusch, J. Hoffmann, M. Klimenkov, J. Reiser, S. Brezinsek, W. Biel, J. Coenen, J. Linke, Ch. Linsmeier, A. Litnovsky, Th. Loewenhoff, G. Pintsuk,

B. Unterberg, M. Wirtz, H. Greuner, A. Kallenbach, R. Neu, J. Riesch, J.H. You,

T. Barrett, F. Domptail, S. Dudarev, M. Fursdon, M. Gilbert, A. Galatanu, W. Pantelon,

L.M. Garrison, Y. Katoh, L.L. Snead, D. Armstrong, S. Roberts, and the WPMAT-HHFM team

AND VICE VERSA

(2)

Outline

Normal and Off-Normal loads in a plasma facing unit (PFU)

Basic thermo-mechanic analysis on the example of ITER

Identification of failure mechanisms and related material properties

The situation for a DEMO PFU

(3)

Simple Load Studies

Thermal off-normal 20 MW/m

2

#1 #2 #10000

2 fpy

normal 10 MW/m

2

t

HF 0.2-1 GW/m

2

ELM

15 MW/m 2 (30s), small monoblock 23 mm x 22 mm x 4 mm, D15 mm

water cooling, 200 °C M. Li, IPP

10 MW/m 2 + 0.4 GW/m 2 (1ms on, 50ms off) ITER type monoblock

28 mm x 28 mm x 12 mm, D17 mm

(4)

Load Analysis, Elastic

Mechanical, elastic

normal

t HF

10 MW/m

2

10s

pat h

-1200 +1200

path (mm) Temperature (°C)

Stress (MPa)

Yield Limit (MPa)

Sxx plastic deformation

under compression

+740 MPa

-670 MPa

Stress

(5)

Load Analysis, Plastic Deformation

Mechanical, plastic normal

t HF

10 MW/m

2

10s 20s

Plastic Deformation (10 s)

0.3 %

0 % Pl. Strain

0.1 % 0.2 %

Secondary Stresses (20 s)

365 MPa

-110 MPa Stress

0

200 MPa

7 mm

(6)

Failure Analysis

Mechanical, plastic normal

t HF

10 MW/m

2

10s 20s

Max. Stress during cooling

• Strain rate: 10 -3 /s – 10 -2 /s

• 150 °C < DBTT <250 °C

• T > 300 °C

ductile regime

no brittle fratcure

Mechanical, dynamic

(7)

properties depend strongly on specific material

Basic Properties

Rxx

DBTT

• brittle fracture

• no plastic deformation

• no yield limit

(8)

Microstructure, Grain Size, Rxx

as received 7 h, 1200 °C

25 h, 1200 °C

GS  150 µm x 50 µm GS  300 µm x 70 µm

GS  300 µm x 300 µm

4 mm W plate

PIM W, 2400 °C

GS  100 µm x 100 µm

(9)

Failure under Off-Normal Load

Thermal: T surf = 1800-2100 °C

Recrystallisation (Rxx) off-normal

t HF

20 MW/m

2

10s 20s

Dynamical: DBTT 250-350 °C (W-Rxx)

ductile-brittle regime

Fracture Mechanics

o K Ic = 5-8 MPa m 1/2 (W-Rxx)

o critical crack length = 16-40 µm

o grain size: min. 50 µm, max. >300 µm

ductile/brittle crack formation likely

Mechanical

o plastic surface deformation > 1%

during heating

o secondary surface tensile stresses after cooling down: > 710 MPa

710 MPa

-973 MPa Stress

-500 MPa

0

(10)

Relevant Material Properties

Comparison with experiment: ITER mockup, 300 x 20 MW/m 2 pulses

ductile or brittle crack depend on geometry and load history

relevant material properties for this particulare case:

o Recrystallisation Temperature o Toughness, static DBTT

o Crack formation strength & plasticity

6- 7.5 mm

Critical operating point for cracking

>1700°C

t Surface Temperature

20 MW/m

2

compression

10s 20s

<100°C DBTT

0 MW/m

2

tensile stress

(11)

Additional Load Conditions

Fatigue

#1 #2 #10000

2 fpy

normal 10 MW/m

2

t

HF 0.2-1 GW/m

2

ELM

0

t

stress t

T

o ELM discharges correspond to high strain rate, high temperature, High Cycle Thermal (Shock) Fatigue

this is not covered by usual material tests (LCF, LCTF, HCF, etc.)

specific requirements for thermal shock tests

possible surface modification, roughnening, crack initiation

(12)

Changing Conditions During DEMO Operation

Microstructure o Recrystallisation

o Cyclic plastic deformation

Strength, DBTT, toughness, ductility will vary during operation

Geometry o Erosion of armour surface due to PSI (max.

2-3 mm/fpy ?, depending on T ?)

Temperature and load will vary with time

Irradiation o Continuous increase of damage (2 dpa/fpy in striking point, 4 dpa/fpy elsewhere)

o Damage strongly depends on temperature

Inhomogeneous variation of material properties

Strength, DBTT, toughness, ductility, thermal

conductivity, fatigue properties, microstructure,

density (swelling), erosion rate?, others?

(13)

Irradiation Defects

Void Formation (Swelling) Transmutation to about 2% Rhenium

HFR irradiation, 900 °C, 4 dpa

o DEMO: about 0.5-1% Rhenium/fpy

Hardening, embrittlement, loss of conductivity, …

Exact extend unknown (lack of data)!!!

o Max. at 600-900°C

Embrittlement, …

(14)

DBTT shift due to n-irradiation

V. Barabash et al. / Journal of Nuclear Materials 283-287 (2000) 138-146

3-PB Tests

80 0 K sh ift

(15)

Situation with n-Irradiation Damage + ELMs

significant DBTT shift

possible surface roughening or microcracks

critical fracture limits (K c, J c, a c ) decrease

cracking very likely

6- 7.5 mm

>1700°C

t Surface Temperature

10s 20s

<100°C DBTT

0 MW/m

2

tensile stress 10 MW/m

2

+ ELMs

compression

(16)

Impact on DEMO Divertor Operation The “ITER limit”

o normal operation 10 MW/m 2 o target tilt and monoblock

shaping (edge shadowing) will lead to 15 MW/m 2

o off-normal transients up to 20 MW/m 2 possible for a limited period

The “DEMO limit”

1. If we use the same design, the requirements must be reduced.

2. If we want to meet the ITER

requirements, we have to change the design and/or concept.

Open question: What is the true minimum required ELM energy density for divertor lifetime?

R. Pitts, ITER

(17)

Impact on Armor Materials R&D

Mitigation by improved materials (topics in WPMAT)

W alloys (increased strength, higher Rxx) S. Antusch

W(fiber)-W composites J. Riesch, J.-H. You, J.W. Coenen

Mitigation by design (the ITER monoblock design seems not to be optimal for DEMO conditions)

Various concepts are under examination J.-H. You (WPDIV)

Close collaboration between DIV and MAT projects

Mitigation by experiment (increase knowledge)

Neutron irradiation campaigns will be launched in WPMAT

brief overview in WGIFT satellite meeting

Tailored High Heat Flux Tests

G. Pintsuk (WPMAT-HHFM programme)

(18)

Thank you !

Partners:

and joined universities

Disclaimer: „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 therein do not necessarily reflect those of the European

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