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Effects of Microstructures on Radiative Properties of YSZ Thermal Barrier Coatings Bo-Xiang Wang School of Mechanical Engineering Shanghai Jiao Tong University Email:[email protected] 16 th CSS-EEST, Nov. 13-15, 2014

2014PNU_CSS_BoxiangWang_SJTU

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Page 1: 2014PNU_CSS_BoxiangWang_SJTU

Effects of Microstructures on Radiative

Properties of YSZ Thermal Barrier Coatings

Bo-Xiang Wang

School of Mechanical Engineering

Shanghai Jiao Tong University

Email:[email protected]

16th CSS-EEST, Nov. 13-15, 2014

Page 2: 2014PNU_CSS_BoxiangWang_SJTU

Outline

Background: Thermal barrier coatings

Simulation and experimental methods

Microstructural effects on radiative properties

Page 3: 2014PNU_CSS_BoxiangWang_SJTU

Temperature distribution across thermal barrier

Heat conductivity of EB-PVD YSZ coating as a function

of temperature

Thermal Barrier Coatings

Page 4: 2014PNU_CSS_BoxiangWang_SJTU

The microstructures of Air Plasma Sprayed (APS) and EB-PVD

thermal barrier coatings

Standard thermal barrier coatings have a typical porosity of 10–20%

Page 5: 2014PNU_CSS_BoxiangWang_SJTU

SEM micrographs of fracture surfaces of as-sprayed YSZ top coats

Page 6: 2014PNU_CSS_BoxiangWang_SJTU

MATERIALS

Nowadays Typical state-of-the-art TBCs utilize ZrO2 partially with 6-8 wt% Y2O3

Table 1.Thermal physical properties and electromagnetic performance parameter of ZrO2

Name Value SI unit

6.0

2700

4300

0.2~3.5

86

12.5 ~

Refractive index n 2.1 ~

Page 7: 2014PNU_CSS_BoxiangWang_SJTU

θ

a

b

mic-crack

void

pore

Simulated Structures

Page 8: 2014PNU_CSS_BoxiangWang_SJTU

Simulation Methods

Plane wave source

TBC coating

Per

iod

ical

bound

ary c

ondit

ion

Per

iod

ical

bound

ary c

ondit

ion

PML obsorbing boundary condition

PML obsorbing boundary condition

-ln( ( ) / (0)) -ln( ( ))I L I LK

L L

ln( ( ) / (0)) ln( ( ))I L I LK

L L

0 r

EH

t

0

HE

t

Maxwell’s equations Extinction coefficient

Page 9: 2014PNU_CSS_BoxiangWang_SJTU

Measurement principle of hemispherical transmittance/reflectance

Measurement principle

Page 10: 2014PNU_CSS_BoxiangWang_SJTU

1 2 3 4 5 6

0.00

0.05

0.10

0.15

0.20

0.25

0.30

0.35

Tra

nsm

itta

nce

Wavelength (m)

Experimental data

Calculated data

Experimental data vs. simulation results

Experimental data: thickness=200μm, porosity=15%

Simulation data: 10% spherical pores (radius=1μm) and 5% cracks (a=1 μm,b=5 μm)

Page 11: 2014PNU_CSS_BoxiangWang_SJTU

1 2 3 4 5 6

500

1000

1500

2000

2500

3000

3500

4000

4500

5000

5500

6000

6500

7000

Exti

nct

ion c

oef

fici

ent

K (

1/m

)

Wavelength (m)

random arrangement

regular arrangement

Extinction coefficient of coating for different arrangement of spherical pores

Microstructural effect on the radiative properties

Page 12: 2014PNU_CSS_BoxiangWang_SJTU

1 2 3 4 5 6

3000

3500

4000

4500

5000

5500

6000

6500

7000

7500

8000

8500

9000

9500

10000

porosity=20%

porosity=15%

Exti

nct

ion c

oef

fici

ent

1

/m)

Wavelength (m)

porosity=5%

porosity=10%

(a)5 10 15 20

3000

4000

5000

6000

7000

8000

9000

Tota

l ex

tinct

ion c

oef

fici

ent

K (

1/m

)

Porosity (%)(b)

Extinction coefficient of the coating for different porosity

Microstructural effect on the radiative properties

Page 13: 2014PNU_CSS_BoxiangWang_SJTU

0 1 2 3 4 5 6 7

2000

3000

4000

5000

6000

7000

8000

9000

10000

Exti

nct

ion c

oef

fici

ent

(1/m

)

Wavelength (m)

r=0.3m

r=0.5m

r=1m

r=1.5m

(a)

0.2 0.4 0.6 0.8 1.0 1.2 1.4 1.6

4500

5000

5500

6000

6500

7000

7500

8000

pore radius (m)

Tota

l ex

tinct

ion c

oef

fici

ent

(1/m

)

(b)

Extinction coefficient of the coating for different pore radius

Microstructural effect on the radiative properties

Page 14: 2014PNU_CSS_BoxiangWang_SJTU

a b

a

a

a

b

b

b

b/a=1

b/a=2

b/a=4

b/a=6

(a)

θ

(b)

Schematic of microstructures with different shapes (a), and orientations (b)

Microstructural effect on the radiative properties

Page 15: 2014PNU_CSS_BoxiangWang_SJTU

1 2 3 4 5 6

3000

3500

4000

4500

5000

5500

6000

6500

7000

7500

8000

8500

9000

Exti

nct

ion c

oef

fici

ent

(1/m

)

Wavelength (m)

b/a=1

b/a=2

b/a=4

b/a=8

b/a=12

a=0.5m

(a)0 2 4 6 8 10 12

3000

4000

5000

6000

7000

8000

9000

Tota

l ex

tinct

ion c

oef

fici

ent

(1/m

)

Shape coefficient b/a(b)

Extinction coefficient of the coating for different microstructure shape

Microstructural effect on the radiative properties

Page 16: 2014PNU_CSS_BoxiangWang_SJTU

0 1 2 3 4 5 6

0

1000

2000

3000

4000

5000

6000

7000

8000

9000

10000

11000

12000

13000

14000

15000

Exti

nct

ion c

oef

fici

ent

(1/m

)

Wavelength (μm)

=0

=30

=60

=90

(a)0 30 60 90

2000

4000

6000

8000

10000

12000

Tota

l ex

tinci

ton c

oef

fici

ent

(1/m

)Orientation ()(b)

Extinction coefficient of the coating for different orientations

Microstructural effect on the radiative properties

Page 17: 2014PNU_CSS_BoxiangWang_SJTU

Many thanks for your attention!