ultrasonic characterization of hydrogen induced stress in 4140 steel iopf2010-6001

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IOPF 2010 Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001 Don E. Bray, Ph. D., P. E., Don E. Bray, Inc. PO Box 10315, College Station, Texas 77842-0315 [email protected] http://brayengr.com Richard B. Griffin, Ph. D., P. E. TAMU Qatar Mechanical Engineering Program Doha, Qatar 10/21/10

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Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001. Don E. Bray, Ph. D., P. E., Don E. Bray, Inc. PO Box 10315, College Station, Texas 77842-0315 [email protected] http://brayengr.com - PowerPoint PPT Presentation

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Page 1: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

Ultrasonic Characterization of Hydrogen Induced Stress in 4140

Steel IOPF2010-6001

• Don E. Bray, Ph. D., P. E., Don E. Bray, Inc. PO Box 10315, College Station, Texas 77842-0315 [email protected] http://brayengr.com

• Richard B. Griffin, Ph. D., P. E. TAMU Qatar Mechanical Engineering Program Doha, Qatar

10/21/10

Page 2: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

Basis for LCR Experiments

• Assumption is that the block is fully charged with hydrogen in the autoclave.

• Chemical change to other forms of hydrogen or other chemistries is ignored.

• Upon removal of the block and returning to room temperature, shrinkage occurs, putting the outer surface in compression as the hydrogen escapes from the block.

Page 3: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

Setup

1 2 3

Test Blocks

1 Control Block2 & 3 Test Blocks

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Page 4: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

LCR Wave

Frequency = 5 MHz Wavelength = 1.2 mm

Page 5: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 201010/21/10

Page 6: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

Hydrogen Flow from Blocks

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Page 7: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

Equations Governing Hydrogen Movement – Fick’s Second Law

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Page 8: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 201010/21/10

Page 9: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

Experimental Procedures

•Blocks 2 and 3 sent to Honeywell for hydrogen

exposure.

•Block 1 held in lab as control block.

•Data obtained on blocks 1, 2 and 3 starting 20

and 14 days after leaving autoclave.

•Data plotted as velocity differences (2-1 and 3-1).

•Experimental error ± 3 m/s.

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Page 10: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 201010/21/10

Page 11: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 201010/21/10

Page 12: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

fp = peak frequency fc = central frequency

fa = low half power point fb = upper half power point

Frequency Analysis

Page 13: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

Results of Frequency Analysis

X

X – a likely anomaly

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Page 14: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

Summary of Results from Frequency Analysis

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1. Peak (fp) and low frequency (fa) groups shifted downward with hydrogen exposure.

2. No significant change after removal from autoclave.

Page 15: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

Summary from Photomicrographs

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1. Decarburization at depth of 0.2 mm.

2. Decarburization layer less than 1.2 mm wavelength,

3. No effect expected on velocity due to decarburization.

4. No hydrogen induced cracking found.

Specimen 3

Page 16: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

Summary from Texture Analysis

3/28/1

0

1. XRD showed texture differences for top and bottom surfaces.

2. Texture likely reason for velocity separation for tops and bottom sides.

3. Texture may be reason for differences in post autoclave velocity pattern with time.

Page 17: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

LCR2 Excitation on Opposite Wall

Page 18: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

LCR2 Arrivals at 75 and 150 mm probe spacing on 15 mm plate

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150 mm

75 mm

Page 19: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 201010/21/10

Conclusions

• LCR velocity change may be a reliable tool for research and application in measurement of reversible hydrogen buildup in metals.

Page 20: Ultrasonic Characterization of Hydrogen Induced Stress in 4140 Steel IOPF2010-6001

IOPF 2010

Acknowledgements

10/21/10

• The hydrogen environment was contributed by Honeywell Corrosion Solutions, Honeywell International, Inc., Houston, Texas.

• Dr. Malur Srinivasan of Lamar University contributed information on the texture difference between the two sides of the

blocks.

• Mr. Jonathan Dahmann collected and analyzed much of the data.