Optical Blade Clearance Probe

• US 20120182563A1
• Filed: 01/10/2012
• Published: 07/19/2012
• Est. Priority Date: 01/14/2011
• Status: Active Grant

• Current Assignee: Prime Photonics, LC (Halliburton Company)
• Original Assignee: Prime Photonics, LC (Halliburton Company)
• Inventors: Kominsky, Daniel
• Granted Patent: US 8,553,237 B2
• Time in Patent Office: Days
• US Class Current: 356/625
• CPC Class Codes: G01B 11/026 by measuring distance between sensor and object G01B11/0608 takes precedence
• CPC Class Codes: G01B 11/14 for measuring distance or clearance between spaced objects or spaced apertures G01B11/26 takes precedence; rangefinders G01C3/00

Abstract

The sensor comprises a beam of electromagnetic radiation projecting across a gap between the stationary member and the translating member, a reference detector having a reference FOV and a signal detector having a signal FOV. The sensor is to be mounted on the stationary member. The electromagnetic radiation beam, the reference FOV and the signal FOV intersect in a volume including the gap, and the gap is calculated from the reflected electromagnetic radiation received by the reference and signal detectors. The gap can be determined from a ratio between a rise time in the signal pulse and a rise time in the reference pulse, or a ratio between a fall time in the signal pulse and a fall time in the reference pulse, or a ratio between a delay time in the signal pulse and a delay time in the reference pulse, among other features.

Claims

1. A sensor comprising:

a source of electromagnetic radiation to be mounted on a stationary member to project an electromagnetic radiation beam across a gap toward at least one translating member;

a reference detector having a reference field of view (FOV) and a signal detector having a signal FOV to be mounted on the stationary member,

wherein the electromagnetic radiation beam, the reference FOV and the signal FOV intersect in a volume including said gap,

wherein a feature of the translating member is measured from the reflected electromagnetic radiation received by the reference detector and by the signal detector.

2. The sensor of claim 1, wherein said feature comprises the gap between the translating member and the stationary member.

3. The sensor of claim 1, wherein said feature comprises a time period at which said translating member passes said volume.

4. The sensor of claim 1, wherein said feature comprises a profile of the intensity of the electromagnetic radiation reflected by the passing of said translating member through said volume.

5. The sensor of claim 1 further comprising an optical element to direct the electromagnetic radiation beam across said gap and to direct reflected electromagnetic radiation toward the reference detector and signal detector.

6. The sensor of claim 5, wherein the optical element comprises a lens, a window with at least one angle surface, a mirror or a prism.

7. The sensor of claim 1, wherein said stationary member comprises a window that is transparent to the electromagnetic radiation.

8. The sensor of claim 5, wherein the optical element comprises a lens and a spacer is disposed between the lens and an end of the source of electromagnetic radiation.

9. The sensor of claim 1, wherein the source of electromagnetic radiation, the reference detector and the signal detector each comprises an optical fiber or waveguide.

10. The sensor of claim 9, wherein at least one of the optical fibers or waveguides comprises an angled end.

11. The sensor of claim 9, wherein at least one of the optical fibers or waveguides is retained in a slotted ferrule.

12. The sensor of claim 2, wherein the gap is proportional to intervals between time markers on pulses produced by the reflected electromagnetic radiation received by the reference detector and the signal detector, or ratios of said intervals.

13. A method for measuring a gap between a stationary member and at least one translating member comprising the steps of:

i. projecting a beam of electromagnetic radiation across said gap;

ii. providing a reference field of view (FOV) and a signal FOV across said gap;

wherein the beam of electromagnetic radiation, the reference FOV and the signal FOV intersect in a volume that includes said gap;

iii. receiving reflected electromagnetic radiation through the reference FOV and the signal FOV as the translating member moves through the beam of electromagnetic radiation;

iv. calculating said gap from time markers on pulses derived from at least one of a signal pulse received from the signal FOV and a reference pulse received from the reference FOV.

14. The method of claim 13, wherein the time markers comprises at least one time marker from the signal pulse and at least one corresponding time marker on the reference pulse.

15. The method of claim 14, wherein step (iv) comprises a step of determining a ratio between a rise time in the signal pulse and a rise time in the reference pulse.

16. The method of claim 14, wherein step (iv) comprises a step of determining a ratio between a fall time in the signal pulse and a fall time in the reference pulse.

17. The method of claim 14, wherein step (iv) comprises a step of determining a ratio between a delay time in the signal pulse and a delay time in the reference pulse.

18. The method of claim 13, wherein the time markers comprises at least one time marker from the signal pulse and at least one dissimilar time marker on the reference pulse.

19. The method of claim 18, wherein step (iv) comprises a step of determining a ratio between signal rise time and rise time delay.

20. The method of claim 13 further comprising the step of providing an optical element to direct the electromagnetic radiation beam across said gap and to direct reflected electromagnetic radiation toward the reference detector and the signal detector.

21. The method of claim 20 further comprising the step of minimizing a reflection of said electromagnetic radiation from said optical element back to the reference detector and the signal detector.

22. The method of claim 20, further comprising the step of varying the optical power of the optical element by varying the distance from the end of the electromagnetic radiation beam and the FOVs to the optical element.