Method and device for measuring wall thickness of a pipe in a pipe-rolling mill

• US 7,116,428 B2
• Filed: 01/23/2004
• Issued: 10/03/2006
• Est. Priority Date: 09/25/2002
• Status: Active Grant

• Current Assignee: SMS MEER GmbH (Bernhard-Weiss-Stiftung)
• Original Assignee: SMS MEER GmbH (Bernhard-Weiss-Stiftung)
• Inventors: Sauerland, Martin, Deppe, Gerd-Joachim
• Primary Examiner(s): Lauchman, Layla G.
• Assistant Examiner(s): ANDERSON, DENISE BROWN
• Application Number:
  US10/764,144
• Publication Number:
  US 20050162662A1
• Time in Patent Office: 984 Days
• Field of Search: 356/502, 356/503, 735/03, 736/55
• US Class Current: 356/502
• CPC Class Codes: G01B 11/0691 of objects while moving G01B11/0616 takes precedence
• CPC Class Codes: G01B 17/02 for measuring thickness
• CPC Class Codes: G01B 2290/25 Fabry-Perot in interferometer, e.g. etalon, cavity
• CPC Class Codes: G01B 9/02023 Indirect probing of object, e.g. via influence on cavity or fibre
• CPC Class Codes: G01B 9/02052 Protecting, e.g. shock absorbing, arrangements
• CPC Class Codes: G01B 9/02067 by electronic control systems, i.e. using feedback acting on optics or light
• CPC Class Codes: G01B 9/02068 Auto-alignment of optical elements

Abstract

A method and device for measuring the wall thickness of a pipe in a pipe-rolling mill wherein a Fabry-Pérot interfero-meter has its mirror spacing set by providing an input to a linear activity for one of the mirrors from a controller receiving an input from a photodiode at the output side of the interferometer. A second control circuit regulates the amplification of that photodiode with at least one parameter derived from the rolling system, for example, the input optical signal to the interferometer or a disturbance value representing for example the temperature of the rolled product and obtained through an optical pyrometer. The incoming optical signal may be tapped to another photodiode also with a variable amplification amplifier and both amplifiers may be controlled by a second controller.

Claims

1. A method of measuring a wall thickness of a pipe in a pipe rolling line, comprising the steps of:

(a) launching an ultrasonic pulse into a wall of a pipe whereby an ultrasonic wave is transmitted across a thickness of said wall and an ultrasonic echo is returned to a surface of the pipe;

(b) training a laser beam from an illuminating laser onto said surface whereby a laser-light reflection from said surface is modulated by said echo;

(c) collecting laser light reflected from said surface and modulated by said echo as an input optical signal and feeding said input optical signal to a Fabry-Pé

rot interferometer having two mirrors spaced apart by a predeterminable distance (a), said Fabry-Pé

rot interferometer having an output optical signal;

(d) passing said output optical signal to a first photodiode and converting said output optical signal into an electrical signal and evaluating said electrical signal to determine transit time for echoes spanning the thickness of said pipe and, from said transit time and a speed of sound in material of the pipe, said wall thickness;

(e) at least one of the steps of;

(e₁) deriving a photodiode-measurement control signal from said electrical signal,

(e₂) deriving a input-measurement control signal from said input optical signal, and

(e₃) deriving a rolling-line control signal representing a fabrication process variable;

(f) controlling a linear actuator determining a position of at least one of said mirrors directly or indirectly through a controller for said linear actuator with at least one of said control signals;

(g) regulating said photodiode with the output from a variable amplification amplifier; and

(h) during steps (e), (f), and (g)

(h₁) varying a signal measured by said first photodiode as a function of the input optical signal as measured by a second photodiode and feeding the varied signal to said controller, each of said first and second photodiodes having respective amplifiers for amplifying the signals measured thereby, and

(h₂) controlling the amplifiers in a respective control circuit based upon at least one predeterminable command variable.

2. The method defined in claim 1 wherein the amplification of said amplifiers is controlled in dependence upon a signal from said second photodiode in said respective control circuit in response to one of said command variables.

3. The method defined in claim 1 wherein a signal from said first photodiode is varied in dependence upon a measured temperature of said pipe before it is fed to said controller.

4. The method defined in claim 1 wherein the amplification of at least one of said amplifiers is controlled in dependence upon a disturbance variable (z) applied to at least one of said amplifiers through at least one adder.

5. The method defined in claim 4 wherein said disturbance variable (z) is a measured temperature (T) of said pipe.

6. The method defined in claim 3 wherein pipe temperature is measured with a pyrometer.

7. The method defined in claim 1 wherein said controller is a high-dynamic regulator acting upon said linear actuator.

8. The method defined in claim 1 wherein said controller is a regulator applying PID control to said linear actuator.

9. The method defined in claim 1 wherein the control circuits for said amplifiers are operated with high dynamic controllers.

10. The method defined in claim 1, further comprising applying PID control to at least one of said amplifiers.

11. The method defined in claim 1, further comprising applying PI control to at least one of said amplifiers.

12. The method defined in claim 1, further comprising the step of defining at least one of said command variables by stepwise scanning of a course of functional response of the respective control circuit prior to use thereof in a wall thickness determination of a rolled pipe.

13. A device for measuring a wall thickness of a pipe in a pipe rolling line, the device comprising:

a laser ultrasonic measuring unit having an excitation laser trained on a surface of a pipe for launching an ultrasonic pulse into a wall of the pipe whereby an ultrasonic wave is transmitted across a thickness of said wall and an ultrasonic echo is returned to the surface of the pipe, an illuminating laser directing a laser beam onto said surface whereby a laser-light reflection from said surface is modulated by said echo, and an interferometer receiving laser light reflected from said surface and modulated by said echo as an input optical signal and having two mirrors spaced apart by a predeterminable distance (a), said interferometer having an output optical signal evaluatable to determine transit time for echoes spanning the thickness of said pipe and, from said transit time and a speed of sound in material of the pipe, said wall thickness, said interferometer having a linear actuator for relatively displacing said mirrors to adjust said distance; and

a control system acting upon said linear actuator and including;

a first photodiode receiving said output optical signal,

a controller responsive to a signal obtained from said first photodiode and controlling said linear actuator, and

a second photodiode receiving said input optical signal,

respective amplifiers connected to said photodiodes for amplifying respective signals measured thereby, and

a control circuit including a further controller for regulating amplifications of said amplifiers to predetermined values.

14. The device defined in claim 13 wherein at least one of said amplifiers is connected to an adder for introducing a disturbance parameter as a control factor for the respective amplifier.

15. The device defined in claim 13, further comprising a pyrometer for measuring the temperature of said pipe and providing an input to at least one of said controllers.

16. The device defined in claim 13 wherein at least one of said amplifiers has a logarithmic characteristic.

17. The device defined in claim 13 wherein said circuit includes a tolerance former for determining a difference between the measured signal of said first photodiode and the measured signal of said second photodiode and feeding a difference signal to the controller responsive to the signal obtained from said first photodiode.

18. The device defined in claim 13, further comprising a vibration-damped support for said interferometer.

19. The device defined in claim 18 wherein said support has vibration-absorbing feet on a bottom side thereof.

20. The device defined in claim 19 wherein said support has an enclosure for said interferometer enclosing said interferometer from all sides.

21. The device defined in claim 20 wherein said enclosure is composed of wood.

22. The device defined in claim 20 wherein said support is provided on inner sides with plate-shaped damping elements.

23. The device defined in claim 22 wherein said damping elements are fibers of medium density.

24. The device defined in claim 22, further comprising a foam between said plate-shaped damping elements and inner sides of said support.