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TECHNICAL PAPERS

Stress Intensity Factor of a Circumferential Crack in a Thick-Walled Cylinder Under Thermal Striping

[+] Author and Article Information
Toshiyuki Meshii

Fukui University, Department of Mechanical Engineering, 3-9-1, Bunkyo, Fukui, Fukui 910-8507, Japan

Katsuhiko Watanabe

University of Tokyo, 1st Division, Institute of Industrial Science, 4-6-1, Komaba, Meguro-ku, Tokyo 153-8505, Japan

J. Pressure Vessel Technol 126(2), 157-162 (May 05, 2004) (6 pages) doi:10.1115/1.1687797 History: Received November 06, 2002; Revised September 08, 2003; Online May 05, 2004
Copyright © 2004 by ASME
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References

Figures

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Circumferentially cracked cylinder under thermal striping
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Transient temperature distribution by Eq. (10) (rm/W=1, W=10 mm,κ=3.61 mm2/s,f=0.05 Hz,h=∞ kW/(m2⋅K)(α0=∞ m−1))
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Transient temperature distribution by Eq. (10) (rm/W=1,W=10 mm,κ=3.61 mm2/s,f=1 Hz,h=∞ kW/(m2⋅K)(α0=∞ m−1))
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Transient temperature distribution by Eq. (10) (rm/W=1,W=10 mm,κ=3.61 mm2/s, f=0.05 Hz, h=1.16 kW/(m2⋅K)(α0=91.7 m−1))
Grahic Jump Location
Transient temperature distribution by Eq. (10) (rm/W=1,W=10 mm,κ=3.61 mm2/s, f=1 Hz, h=1.16 kW/(m2⋅K)(α0=91.7 m−1))
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Convergence of the SIF range under thermal striping (rm/W=1,H=π/β,W=10 mm,a/W=0.15, κ=3.61 mm2/s,h=∞ kW/(m2⋅K) (α0=∞ m−1))
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Effect of f on ΔKmax under thermal striping (rm/W=1,H=π/β, W=10 mm, κ=3.61 mm2/s, h=∞ kW/(m2⋅K)(α0=∞ m−1))
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Effect of f on ΔKmax under thermal striping (rm/W=1,H=π/β,W=10 mm,κ=3.61 mm2/s, h=11.6 kW/(m2⋅K)(α0=917 m−1))
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Effect of f on ΔKmax under thermal striping (rm/W=1,H=π/β,W=10 mm,κ=3.61 mm2/s,h=1.16 kW/(m2⋅K)(α0=91.7 m−1))
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Transient IOTD for the first ten cycles (rm/W=1,W=10 mm, κ=3.61 mm2/s, h=∞ kW/(m2⋅K) (α0=∞ m−1))
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Comparison of u(r,tmin)(rm/W=1, W=10 mm,κ=3.61 mm2/s, h=∞ kW/(m2⋅K) (α0=∞ m−1))
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Comparison of u for thermal striping and step temperature change (rm/W=1, W=10 mm, κ=3.61 mm2/s,h=∞ kW/(m2⋅K) (α0=∞ m−1))

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