Abstract

Grain size is an important parameter in evaluating the properties of microstructures in metals. In this paper, the attenuation coefficient of Rayleigh waves is introduced to characterize grain size in heat treated 316L stainless steel. Rayleigh wave attenuation is measured using an angle beam wedge transducer as the transmitter and an air-coupled transducer as the receiver. The results show that the grain size in 316L stainless steel increases due to heat treatment time, the hardness decreases accordingly, and the attenuation coefficient of Rayleigh waves increases. This indicates that the Rayleigh wave attenuation is sufficient in distinguishing the changes in the properties of the heat-treated stainless steel. It is found that compared with the measurement method using an angle beam wedge receiver, the measured results are efficient, more stable and less influenced by the surface state when an air-coupled receiver is used. In addition, comparison results also show that the Rayleigh wave attenuation is more sensitive to changes in material properties than the longitudinal wave attenuation, as the wavelength of the Rayleigh wave is shorter than that of the longitudinal wave at the same frequency.

Highlights

  • IntroductionPublisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations

  • The coordinate system x1 y1 z1 is located on the surface of the angle beam wedge transducer, x2 y2 z2 is on the contact surface of the wedge and the specimen, and x3 y3 z3 is on the surface of the air-coupled transducer

  • Was found that when the grain size increased due to heat treatment ment

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Summary

Introduction

Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations. The backscatter grain noise has no requirement of parallel front-wall and back-wall surfaces and known wall thickness of a specimen, but more complicated statistical methods are required to combine the ultrasonic signals from different sets of grains at different transducer spatial positions [13]. This method loses accuracy in the case of coarse-grained materials. The relationship between the grain size and the Rayleigh wave attenuation coefficient are discussed

Measurement Method and Theory
Schematic
Experiments
A 10-cycle signal with a center of the frequency of 2MHz and an of 10-cycle
Microstructure of theProperties
Measurement
Errors measurementresults results shown shown in Number
Experimental measurement results andand leastleast squares fitting curve
Measurement of the Attenuation Coefficient for Heat Treatment Stainless Steel
10. The hardness can reflect
Experimental and resultsofofRayleigh
5.5.Conclusions
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