Non-Contact Stress Measurement during Tensile Testing Using an Emat for SH0-Plate Wave and Lamb Wave
Riichi Murayama
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DOI: 10.4236/jst.2011.13009   PDF    HTML     5,567 Downloads   12,560 Views   Citations

Abstract

The stress on a test specimen during tensile testing is generally measured by a strain gauge. This method has some problems in that it would influence the measurement conditions of the tensile test and can evaluate only the position at which the strain gauge is attached. The acoustoelastic method is proposed as a method replacing the strain gauge method. However, an ultrasonic sensor with a piezoelectric oscillator requires a coupling medium to inject an ultrasonic wave into a solid material. This condition, due to the error factor of the stress measurement, makes it difficult for the ultrasonic sensor to move on the specimen. We then tried to develop a non-contact stress measurement system during tensile testing using an electromagnetic acoustic transducer (EMAT) with an SH0-plate wave and S0-Lamb wave. The EMAT can measure the propagation time in which the ultrasonic wave travels between a receiver and a transmitter without a coupling medium during the tensile testing and can move easily. The interval between the transmitter and the receiver is 10mm and can be moved along the parallel direction or the vertical direction of the tensile load. The transit time was measured by a cross-correlation method and converted into the stress on the test specimen using the acoustoelastic method. We confirmed that the stress measurement using an SH0-plate wave was superior to that with an S0-Lamb wave.

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R. Murayama, "Non-Contact Stress Measurement during Tensile Testing Using an Emat for SH0-Plate Wave and Lamb Wave," Journal of Sensor Technology, Vol. 1 No. 3, 2011, pp. 65-70. doi: 10.4236/jst.2011.13009.

Conflicts of Interest

The authors declare no conflicts of interest.

References

[1] D. I. Crecraft, “The Measurement of Applied and Residual Stress in Metals using Ultrasonic Waves,” Journal of Sound and Vibration, Vol. 5, No. 1, 1967, pp. 173-192. doi:10.1016/0022-460X(67)90186-1
[2] K. Okada, “Stress-Acoustic Relation for Stress Measurement by Ultrasonic Techniques,” Journal of the Acoustical Society of Japan (E), Vol. 1, 1980, pp. 193-200.
[3] Y. H. Pao, W. Sache and H. Fukuoka, “Acoustoelasticity and Ultrasonic Measurement of Residual Stress,” Physical Acoustics, Vol. 15, 1984, pp. 61-143.
[4] M. Hirao, H. Fukuoka, H. Toda, Y. Sotani and S. Suzuki, “Non-Destructive Evaluation of Hardening Depth using Surface-Wave Dispersion Patterns,” Journal of Mechanical Working Technology, Vol. 8, No. 2-3, 1983, pp. 171-179. doi:10.1016/0378-3804(83)90035-9
[5] B. Raj, V. Rajendran and P. Palanichamy, “Ultrasonic transducers, in Science and Technology of Ultrasonics,” Alpha Science International Ltd., Oxford, 2004, pp. 37-67.
[6] R. B. Thompson, “A Model for the Electromagnetic Generation and Detection of Rayleigh and Lamb Wave,” IEEE Transaction on Sonics and Ultrasonics, Vol. 20, 1973, pp. 340-346.
[7] M. Hirao and H. Ogi, “Development of EMAT techniques in EMATS FOR SCIENCE AND INDUSTRY,” Kluwer Academic Publishers, London, 2003, pp. 13-82.
[8] G. Alers and H. Ogi, “Handbook of Elastic Properties of Solids, Liquids, and Gases,” M. Levy, H. Bass, R. Stern and V. Keppens, eds., EMAT Techniques, Academic Press, New York, 2001, pp. 263-281.
[9] H. Ogi, E. Goda and M. Hirao, “Increase of Efficiency of Magnetostriction SH-Wave EMAT by Angled Bias Field,” Japanese Journal of Applied Physics, Vol. 42, 2003, pp. 3020-3024. doi:10.1143/JJAP.42.3020
[10] M. Hirao, H. Ogi and H. Yasui, “Contactless Measurement of Bolt Axial Stress Using a Shear-Wave Electromagnetic Acoustic Transducer,” NDT & E International, Vol. 34, No. 3, 2001, pp. 179-183. doi:10.1016/S0963-8695(00)00055-4
[11] M. Hirao and H. Ogi, “On-line Texture Monitoring on Steel Sheets in EMATS FOR SCIENCE AND INDUSTRY,” Kluwer Academic Publishers, London, 2003, pp. 197-213.
[12] M. Hirao and H. Fukuoka, “Dispersion Relation of Plate Modes in Anisotropic Polycrystalline Sheets,” Journal of the Acoustical Society of America, Vol. 85, No. 6, 1989, pp. 2311-2315. doi:10.1121/1.397777
[13] E. P. Papadakis, “Ultrasonic Pulse Velocity by the Pulse-Echo-Overlap Method Incorporating Diffraction Phase Correlation,” Journal of the Acoustical Society of America, Vol. 42, 1967, pp. 1045-1051.
[14] H. J. McSkimin, “Pulse Superposition Method for Measuring Ultrasonic Wave Velocities in Solids,” Journal of the Acoustical Society of America, Vol. 33, No. 1, 1961, pp. 12-16. doi:10.1121/1.1908386

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