Thermomechanical characterization of coatings for harsh ... · Thermomechanical characterization of...

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Thermomechanical characterization of coatings for harsh temperatures and irradiation environments E. Besozzi PhD program in “Energy and Nuclear Science and Technology” (started Nov. 2014) Politecnico di Milano, Department of Energy, Via Ponzio 34/3, Milano (IT) www.nanolab.polimi.it Motivations Thermomechanical properties: FLEX Aims of the research Mechanical properties: Brillouin Spectroscopy Conclusions & F uture P erspectives Temperature changes Deformed array Reference array Provide lab-scale investigation of thermomechanical properties of PFMs coatings Mechanical characterization by unconventional techniques Thermomechanical analysis (Thermal stress evolution, fatigue, thermal expansion (CTE)) Development of a new experimental setup (FLEX) + (Brillouin Spectroscopy + nano-indentation) Coatings exposure to ITER-relevant conditions Electron beam Plasma Ions W and W-compounds coatings deposited by Pulsed Laser Deposition (PLD) External collaborations Plasma PFMs interactions Particle bombardment effects Erosion and sputtering Co-deposition and Re-deposition Helium bubble formation and swelling Nuclear fuel retention and permeation Radiation damage Thermal Effects High thermal stress induced by transient and steady loads Fatigue (pulsed regime) Melting Knowing thermal and mechanical behavior of Plasma Facing Materials (PFMs) is crucial to guarantee integrity and operational stability Severe material modifications at different scales (mm, μm, nm) Laboratory deposited μm thick coatings (PVD, CVD techniques) Mimicking of various tokamaks PFMs scenarios Coatings in operating tokamaks Mimicking of co/re deposits Mimicking of damaged PFMs Correlation with thermomechanical properties is still an open issue N. Gordillo et al., Applied Surface Science 316 (2014) Tungsten ( W) and W - compounds Coating stress determined by substrate curvature measurement Our experimental setup: Versatile Transparent/opaque films Thermal and residual stresses Stress relaxation process Coating CTE Non-destructive, contactless Low power laser scanning Different information: 1− 2 1 6 = Stoney equation Substrate curvature Film stress Substrate elastic properties Relative distance between laser spots Coatings mechanical properties not needed Heating stage provides thermal ramps from ambient temperature to 1000°C (ITER relevant) Background gas inlet allows thermal treatments at different atmospheres [1] J.A Floro et al., Journal of Electronic Materials, Vol. 26, No. 9, 1997 Elastic moduli of coatings Brillouin spectroscopy Laser photon acoustic phonon inelastic interaction Theoretical Experimental data Acoustic waves dispersion relation Fitting of the two dispersion relation sets Elastic moduli of coatings Tuning of coating nanostructure Nanocrystalline Amorphous-like Different mechanical properties expected W-Ta alloy Ductilization Amorphous-like W co/re-deposits Nanocrystalline W W proxy PFMs [email protected] PLD of W films Conclusions FLEX setup allows us to determine thermal stresses in coatings with accuracy up to few MPa. The determination of coatings CTE is thus feasible and it can be found in strictly relation with coating nanostructure Brillouin spectroscopy can be extremely sensitive to morphology and structure modifications up to the nanoscale. This peculiar property combined with the intrinsic nature of W and W-compounds coatings can validate Brillouin spectroscopy as an alternative characterization technique for coatings mechanical properties within the elastic regime Brillouin spectroscopy provides quantitative information about Young modulus (E), shear modulus (G) and Poisson’s ration (v) at the same time. These properties can be then combined to infer qualitative information also about the plastic material behavior (ductility) Future perspectives Stress relaxation analysis by FLEX: crack formation and propagation Thermal fatigue behavior under cycling irradiation by pulsed laser beams Development of a numerical tool to determine the dynamic stress developed during laser irradiation Possibility to extend this case of study to transient thermal loads representative of ITER transient events Exposure of W and W-compounds coatings to ITER-relevant conditions and their consequent thermomechanical characterization 100 200 300 400 500 600 0 50 100 150 200 250 Curvature Radius (m) Temperature (°C) Theory Data calculated from [1] Our method 0 100 200 300 400 500 600 -20 -10 0 10 20 30 R/R [%] Temperature (°C) Time (s) Deviaon from theory ̴ 5% Thermal Stress (GPa) Preliminary results: Non-destructive, contactless Low power laser Versatile Transparent/opaque films thickness No bulk properties Typical Brillouin spectrum of nanocrystalline W Supervisors: D. Dellasega and M. Beghi – Tutor: M. Passoni

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Page 1: Thermomechanical characterization of coatings for harsh ... · Thermomechanical characterization of coatings for harsh temperatures and irradiation environments E. Besozzi PhD program

Thermomechanical characterization of coatings for harsh temperatures and irradiation environments

E. Besozzi

PhD program in “Energy and Nuclear Science and Technology” (started Nov. 2014)Politecnico di Milano, Department of Energy, Via Ponzio 34/3, Milano (IT)

www.nanolab.polimi.it

Motivations

Thermomechanical properties: FLEX

Aims of the research

Mechanical properties: Brillouin Spectroscopy

Conclusions & Future Perspectives

Temperature changes

Deformed array

Reference array

Provide lab-scale investigation of thermomechanical

properties of PFMs coatings

Mechanical characterization by unconventional techniques

Thermomechanical analysis (Thermal stress evolution,

fatigue, thermal expansion (CTE))

Development of a new experimental setup

(FLEX)

+

(Brillouin Spectroscopy + nano-indentation)

Coatings exposure to ITER-relevant conditions

• Electron beam

• Plasma

• Ions

W and W-compounds coatings deposited by Pulsed Laser

Deposition (PLD)

External collaborations

Plasma – PFMs interactions

Particle bombardment effects

• Erosion and sputtering

• Co-deposition and Re-deposition

• Helium bubble formation and swelling

• Nuclear fuel retention and permeation

• Radiation damage

Thermal Effects

• High thermal stress induced

by transient and steady loads

• Fatigue (pulsed regime)

• Melting

Knowing thermal and mechanical behavior of Plasma Facing Materials (PFMs) is crucial to guarantee integrity and operational stability

Severe material modifications at

different scales (mm, µm, nm)

Laboratory deposited µm thick coatings

(PVD, CVD techniques)

Mimicking of various

tokamaks PFMs scenarios

• Coatings in operating tokamaks

• Mimicking of co/re – deposits

• Mimicking of damaged PFMs

Correlation with thermomechanical properties is

still an open issue

N. Gordillo et al., Applied Surface Science 316 (2014)

Tungsten (W) and W - compounds

Coating stress determined by substrate curvature measurement

Our experimental setup:

• Versatile Transparent/opaque films

Thermal and residual stresses Stress relaxation process

Coating CTE

• Non-destructive, contactless Low power laser scanning

• Different information:−

𝐸𝑠1 − 𝑣𝑠

ℎ𝑠2

ℎ𝑓

1

6𝑅= 𝜎𝑓

Stoney equation

Substrate curvature

Film stressSubstrate elastic

properties

Relative distance between laser spots

Coatings mechanical

properties not neededHeating stage provides thermal ramps from ambient

temperature to 1000°C (ITER – relevant)

Background gas inlet allows thermal treatments at

different atmospheres

[1] J.A Floro et al., Journal of Electronic Materials, Vol. 26, No. 9, 1997

Elastic moduli of coatingsBrillouin spectroscopy

Laser photon –

acoustic phonon

inelastic interaction

Theoretical

Experimental data

Acoustic waves

dispersion relation

Fitting of the two dispersion

relation setsElastic moduli of coatings

Tuning of coating

nanostructure

Nanocrystalline Amorphous-like

Different mechanical

properties expected

• W-Ta alloy Ductilization

• Amorphous-like W co/re-deposits

• Nanocrystalline W W proxy PFMs

[email protected]

PLD of

W films

Conclusions

• FLEX setup allows us to determine thermal stresses in coatings with accuracy up to few MPa. The determination

of coatings CTE is thus feasible and it can be found in strictly relation with coating nanostructure

• Brillouin spectroscopy can be extremely sensitive to morphology and structure modifications up to the

nanoscale. This peculiar property combined with the intrinsic nature of W and W-compounds coatings can validate

Brillouin spectroscopy as an alternative characterization technique for coatings mechanical properties within

the elastic regime

• Brillouin spectroscopy provides quantitative information about Young modulus (E), shear modulus (G) and

Poisson’s ration (v) at the same time. These properties can be then combined to infer qualitative information also

about the plastic material behavior (ductility)

Future perspectives

• Stress relaxation analysis by FLEX: crack formation and propagation

• Thermal fatigue behavior under cycling irradiation by pulsed laser beams

Development of a numerical tool to determine the dynamic stress developed

during laser irradiation

Possibility to extend this case of study to transient thermal loads representative of

ITER transient events

• Exposure of W and W-compounds coatings to ITER-relevant conditions and their

consequent thermomechanical characterization

100 200 300 400 500 600

0

50

100

150

200

250

Cu

rvatu

re R

ad

ius (

m)

Temperature (°C)

Theory

Data calculated from [1]

Our method

0 100 200 300 400 500 600

-20

-10

0

10

20

30

R

/R [

%]

Temperature (°C)

Time (s)

Deviation from theory ̴ 5%

Th

erm

al S

tre

ss (

GP

a)

Preliminary results:

• Non-destructive, contactless

Low power laser

• Versatile

Transparent/opaque films

thickness

No bulk properties

Typical Brillouin spectrum of nanocrystalline W

Supervisors: D. Dellasega and M. Beghi – Tutor: M. Passoni