Laser-ultrasonic measurement of elastic properties of a thin sheet and of tension applied thereon

• US 6,543,288 B1
• Filed: 08/06/2001
• Issued: 04/08/2003
• Est. Priority Date: 11/04/1998
• Status: Expired due to Term

• Current Assignee: National Research Council Canada
• Original Assignee: National Research Council Canada
• Inventors: Reid, Benoit, Monchalin, Jean-Pierre, Blouin, Alain
• Primary Examiner(s): Larkin, Daniel S.
• Assistant Examiner(s): MILLER, ROSE MARY
• Application Number:
  US09/830,710
• Time in Patent Office: 610 Days
• Field of Search: 736/43, 736/45, 736/46, 736/55, 736/57, 731/59
• US Class Current: 73/643
• CPC Class Codes: G01L 5/042 by measuring vibrational characteristics of the flexible member
• CPC Class Codes: G01L 5/105 using electro-optical means
• CPC Class Codes: G01N 2291/0237 Thin materials, e.g. paper, membranes, thin films
• CPC Class Codes: G01N 2291/02827 Elastic parameters, strength or force
• CPC Class Codes: G01N 2291/02854 Length, thickness
• CPC Class Codes: G01N 2291/0421 Longitudinal waves
• CPC Class Codes: G01N 2291/0427 Flexural waves, plate waves, e.g. Lamb waves, tuning fork, cantilever
• CPC Class Codes: G01N 2291/048 Transmission, i.e. analysed material between transmitter and receiver
• CPC Class Codes: G01N 2291/2632 flat
• CPC Class Codes: G01N 29/041 on the surface of the material, e.g. using Lamb, Rayleigh or shear waves
• CPC Class Codes: G01N 29/2418 using optoacoustic interaction with the material, e.g. laser radiation, photoacoustics photoacoustic cells G01N21/1702; measuring characteristics of vibrations by using radiation-sensitive means G01H9/00; acousto-optical conversion techniques for short-range imaging G01S15/8965; sound-producing devices using laser bundle G10K15/046
• CPC Class Codes: G01N 29/27 by moving the material relative to a stationary sensor
• CPC Class Codes: G01N 29/42 by frequency filtering or by tuning to resonant frequency
• CPC Class Codes: G01N 29/4418 with a model, e.g. best-fit, regression analysis
• CPC Class Codes: G01N 29/449 Statistical methods not provided for in G01N29/4409, e.g. averaging, smoothing and interpolation

Abstract

A method and an apparatus for non-contact and non-invasive characterization of a moving thin sheet and in particular of a paper web on a production line. The method uses a laser for the generation of sonic and ultrasonic waves in the thin sheet and a speckle insensitive interferometric device for the detection of these waves. The generation is performed in conditions to avoid damage impeding further use of the sheet. When the generation and detection spots overlap, the method provides a measurement of the compression modulus. When the generation and detection spots are separated by a known distance and plate waves (Lamb waves) are generated and detected, the method provides a measurement of the in-plane modulus and of the tension applied to the sheet. By detecting waves propagating in various directions, either by rotating the detection sensor head or multiplexing the signals provided by several detection or generation locations, the anisotropy of the in-plane modulus is determined.

Claims

1. A method for non-contact characterization of a rapidly moving sheet, comprising the steps of:

illuminating the sheet at a first location with a first pulsed laser beam for generating acoustic waves propagating through the sheet thickness and over its surface,

illuminating the sheet at a second location with a second laser beam, on the same side or the opposite side of the sheet, this second location being spaced from the first location by a predetermined distance, said sheet scattering the second beam to produce a scattered beam with a plurality of speckles,

collecting the scattered beam, such collected scattered beam having a phase or frequency modulation representative of the acoustic motion at the second location, and

demodulating the phase or frequency modulation to provide an electrical signal representative of the acoustic motion at the second location, and

analyzing the electrical signal to determine a characteristic or a set of characteristics of the sheet,

characterized in that said first laser has a wavelength selected to ensure progressive absorption below the surface of the sheet so as to produce a distributed acoustic source below the surface and an intensity below a threshold value to avoid damage to the sheet, and said demodulating of the phase or frequency modulation is carried out with a speckle-insensitive interferometer.

2. A method as described in claim 1 wherein the sheet is a paper web.

3. A method as described in claim 2 whereby the sheet is a paper web used for printing.

4. A method as described in claim 1 whereby the sheet is of a polymer.

5. A method as described in claim 1 whereby the sheet is of metal.

6. A method as described in claim 1 whereby the characteristic is the tension applied to the sheet.

7. A method as described in claim 1 whereby the characteristic is an elastic modulus.

8. A method as described in claim 1 whereby the set of characteristics consists in the variation of the in-plane elastic modulus in various directions.

9. A method as described in claim 1 and applied to a paper web whereby, the set of characteristics is the Tensile Stiffness Index in various directions of the paper web.

10. A method as described in claim 1 including further the averaging of signals obtained at various times during sheet motion to further minimize additional noise introduced by sheet motion.

11. A method as described in claim 1 whereby additional noise introduced by sheet motion is substantially diminished by subtracting a signal representative of the fluctuations of intensity of the collected light prior to demodulation.

12. A method as described in claim 1 whereby second laser beam is sent substantially perpendicular to the sheet surface and scattered light is collected in a direction also substantially perpendicular to the sheet surface or second laser beam and collection direction are at an angle and are substantially symmetric with respect to the normal to the sheet surface to detect through thickness ultrasonic motion or out-of-plane motion associated to the AO Lamb acoustic wave.

13. A method as described in claim 1 whereby the second laser beam is directed substantially perpendicular to the sheet surface and the scattered beam is collected at an angle or the other way around or both are substantially in the same direction at an angle with respect to the normal to the sheet to detect in-plane acoustic motion associated to SO Lamb ultrasonic wave.

14. A method as described in claim 1 whereby second laser beam is sent substantially perpendicular to the sheet surface and scattered light is collected at an angle or the other way around or both are substantially in the same direction at an angle with respect to the normal to the sheet to detect both out-of-plane and in-plane acoustic motion.

15. A method as described in claim 1 whereby the step of signal analyzing consists of deriving the tension applied to the sheet from the asymptotic low frequency value of the phase or group velocity dispersion curve calculated from the out-of-plane displacement signal associated to the AO Lamb wave mode.

16. A method as described in claim 1 whereby the step of signal analyzing consists of deriving the in-plane modulus from the velocity calculated from the in-plane displacement signal associated to the SO Lamb wave mode.

17. A method as described in claim 1 whereby the second location overlaps the first location and whereby signal analysis consists in deducing from the through-thickness echoes the through-thickness velocity and from the through-thickness velocity the compression modulus or compressibility.

18. A method as described in claim 1 whereby several detection locations are used to measure simultaneously the velocity of SO and AO modes in various directions and to obtain the angular distribution of tension and tensile modulus.

19. A method as described in claim 1 whereby several generation locations are used to measure simultaneously the velocity of SO and AO modes in various directions and to obtain the angular distribution of tension and tensile modulus.

20. An apparatus for non-contact and non-invasive characterization of a rapidly moving sheet, comprising:

a first means for illuminating a first location of the sheet with a first laser beam and for generating acoustic waves propagating through the sheet thickness and over its surface,

a second means for illuminating a second location of the sheet with a second laser beam, on the same side or the opposite side, the second location being spaced from the first location by a predetermined distance,

a third means for collecting the scattered beam, such collected light having a phase or frequency modulation representative of the acoustic motion at this second location,

means for demodulating the phase or frequency modulation so as to provide an electrical signal representative of the acoustic motion at this second location, and

analyzing means for analyzing the electrical signal so as to determine a characteristic or a set of characteristics of the rapidly moving sheet,

characterized in that said first means has a wavelength selected to ensure progressive absorption below the surface of the sheet so as to produce a distributed acoustic source below the surface and an intensity below a threshold value to avoid damage to the sheetd, and said demodulating means comprises speckle-insensitive interferometer.

21. An apparatus as described in claim 20 whereby the sheet is a rapidly moving paper web.

22. An apparatus as described in claim 21 whereby the sheet is a paper web used for printing.

23. An apparatus as described in claim 20 whereby the sheet is of a polymer.

24. An apparatus as described in claim 20 whereby the sheet is of a metal.

25. An apparatus as described in claim 20 whereby the characteristic is the tension applied to the sheet.

26. An apparatus as described in claim 20 whereby the characteristic is an elastic modulus.

27. An apparatus as described in claim 20 whereby the set of characteristics consists in the variation of the in-plane elastic modulus in various directions.

28. An apparatus as described in claim 20 and used on a paper web whereby the set of characteristics is the Tensile Stiffness Index in various directions of the paper web.

29. An apparatus as described in claim 20 further including averaging means acting on the signals obtained at various times during sheet motion and used prior to analysis to further minimize additional noise introduced by sheet motion.

30. An apparatus as described in claim 20, including further detector means to measure the fluctuations of intensity ahead of interferometric means and subtraction means to subtract detector means signal from said electrical signal to minimize additional noise introduced by sheet motion.

31. An apparatus as described in claim 20 whereby second means sends second laser beam substantially perpendicular to the sheet surface and third means collects scattered light in a direction also substantially perpendicular to the sheet surface or second means sends laser beam at an angle and third means collects scattered light in a direction substantially symmetric with respect to the normal to the sheet surface to detect through thickness ultrasonic motion or out-of-plane motion associated to the AO Lamb acoustic wave.

32. An apparatus as described in claim 20 whereby second means sends second laser beam in a direction making an angle with respect to the sheet surface and third means collects scattered light in a direction substantially normal to the sheet surface or the other way around or both means have directions substantially the same and making an angle with respect to the sheet surface to detect in-plane acoustic motion associated to SO Lamb acoustic wave.

33. An apparatus as described in claim 20 whereby second means sends second laser beam in a direction making an angle with respect to the sheet surface and third means collects scattered light in a direction substantially normal to the sheet surface or the other way around or both means have directions substantially the same and making an angle with respect to the sheet surface to detect both out-of-plane and in-plane acoustic motion.

34. An apparatus as described in claim 20 whereby the analyzing means derives the tension applied to the sheet from the asymptotic low frequency value of the phase or group velocity dispersion curve calculated from the out-of-plane displacement signal associated to the AO Lamb wave mode.

35. An apparatus as described in claim 20 whereby the signal analysis means derives the in-plane modulus from the velocity calculated from the in-plane displacement signal associated to the SO Lamb wave mode.

36. An apparatus as described in claim 20 whereby the second location overlaps the first location and whereby the analyzing means first derives the through-thickness velocity from the through-thickness echoes and hence the compression modulus or compressibility from the through-thickness velocity.

37. An apparatus as described in claim 20 further including means for providing several detection locations to measure simultaneously the velocity of SO and AO modes in various directions and to obtain the angular distribution of tension and tensile modulus.

38. An apparatus as described in claim 20 further including means for providing several generation locations to measure simultaneously the velocity of S_o and A_o modes in various directions and to obtain the angular distribution of tension and tensile modulus.

39. An apparatus as described in claim 20 whereby the first means is a transversely excited atmospheric pressure carbon dioxide laser.

40. An apparatus as described in claim 20 whereby first means has a wavelength suitable to be absorbed by an OH band of the sheet material.

41. An apparatus as described in claim 20 whereby the speckle-insensitive interferometer is a confocal Fabry-Perot interferometer.

42. An apparatus as described in claim 20 whereby speckle-insensitive interferometer is based on two-wave mixing in a non-linear optical material.

43. An apparatus as described in claim 20 whereby the interferometric means is based on the photoelectromotive force effect in an optical material.