Method for measuring surface and near surface properties of materials

• US 4,574,637 A
• Filed: 08/03/1984
• Issued: 03/11/1986
• Est. Priority Date: 08/03/1984
• Status: Expired due to Fees

• Current Assignee: Ohio State University
• Original Assignee: Ohio State University
• Inventors: Fitting, Dale W., Adler, Laszlo, de Billy, Michel
• Primary Examiner(s): NOT, DEFINED
• Application Number:
  US06/637,400
• Time in Patent Office: 585 Days
• Field of Search: 73/573, 73/588, 73/606, 73/620, 73/629, 73/633, 73/599
• US Class Current: 73/629
• CPC Class Codes: G01N 2291/0231 Composite or layered materials
• CPC Class Codes: G01N 2291/02854 Length, thickness
• CPC Class Codes: G01N 2291/0423 Surface waves, e.g. Rayleigh waves, Love waves
• CPC Class Codes: G01N 2291/048 Transmission, i.e. analysed material between transmitter and receiver
• CPC Class Codes: G01N 2291/101 one transducer
• CPC Class Codes: G01N 29/00 Investigating or analysing materials by the use of ultrasonic, sonic or infrasonic waves; Visualisation of the interior of objects by transmitting ultrasonic or sonic waves through the object G01N3/00, G01N5/00, G01N7/00, G01N9/00, G01N11/00, G01N13/00, G01N15/00, G01N17/00, G01N19/00, G01N21/00, G01N22/00, G01N23/00, G01N24/00, G01N25/00, G01N27/00 take precedence
• CPC Class Codes: G01N 29/041 on the surface of the material, e.g. using Lamb, Rayleigh or shear waves
• CPC Class Codes: G01N 29/11 by measuring attenuation of acoustic waves

Abstract

The properties of the surface layer of a material are measured by a technique which employs the transmission of ultrasonic waves from varying angles of incidence into a specimen, from a transducer at a point spaced from the specimen. The backscattered waves are detected and evaluated from the varying angles to detect the local maximum intensity, from which the corresponding properties of the material are determined.

Claims

1. A method of measuring the properties of the surface layer of a specimen having said surface layer and a subsurface layer, said surface layer having at least one physical property the value of which differs from the same physical property of said subsurface layer, which method comprises:

a. disposing an ultrasonic transducer at a point spaced from said specimen;

b. causing said transducer to generate a pulse of ultrasound which impinges upon said surface layer of said specimen;

c. detecting, by means of said transducer, the backscattered pulse produced by said impingement of said pulse upon said surface layer;

d. repeating the steps (b) and (c) after varying the angle of incidence of the pulse of ultrasound, and detecting the local maximum of intensity of said backscattered pulse which occurs when said angle of incidence is approximately equal to the Rayleigh angle of said surface layer; and

e. measuring said angle of incidence at said local maximum of intensity.

2. A method according to claim 1 wherein said transducer and at least the portion of said specimen on which said pulse impinges are immersed in a liquid, so that said pulse and said backscattered pulse travel through said liquid.

3. A method according to claim 1 wherein said specimen is mounted upon a pivotable specimen support with a part of said surface layer disposed substantially on the axis of pivoting of said specimen support, and wherein said pulse of ultrasound is arranged to impinge upon said part of said surface layer disposed substantially on said axis.

4. A method according to claim 1 wherein said specimen is held in a fixed position and said transducer is mounted on a pivotable support arranged so that said transducer can be pivoted about a point lying on said surface layer of said specimen, said transducer being arranged so that said pulse of ultrasound generated by said transducer impinges upon said point.

5. A method according to claim 1 wherein said steps (b) to (e) are carried out using at least two different frequencies of said ultrasound, said angle of incidence at said local maximum of intensity being measured separately for each of said frequencies.

6. A method according to claim 1 wherein the frequency of said ultrasound is in the range of about 0.5 to about 10 MHz.

7. A method according to claim 1 wherein said surface layer is of a different hardness from said subsurface layer and wherein said method is used to determine the depth of said subsurface layer.

8. A method according to claim 7 wherein said steps (b) to (e) are carried out using a plurality of different frequencies of said ultrasound, said angle of incidence at said local maximum of intensity being measured separately for each of said frequencies, thereby enabling the variation of hardness with depth of said specimen to be determined from the dispersion of said angles of incidence with said frequencies of said ultrasound.

9. A method according to claim 1 wherein said surface layer differs from said subsurface layer as a result of heat treatment.

10. A method according to claim 1 wherein said surface layer differs from said subsurface layer in the amount of residual stress therein.