Detecting a disturbance in the propagation of light in an optical waveguide
View Patent ↗An optical time domain reflectometry apparatus has a laser and light modulator for producing coherent light pulses, each having two sections of higher intensity separated by a gap of lower or substantially zero intensity. As the light pulses propagate along the optical fibre, light is continuously Rayleigh backscattered by inhomogeneities of the optical fibre. A photodetector generates backscatter signals representing the intensity of light Rayleigh backscattered in the optical fibre as each light pulse travels along the optical fibre. The PC uses these backscatter signals to derive a difference signal representing a change dI in intensity between signals generated from two successive pulses. The PC then calculates the Root Mean Square (RMS) of the difference signal averaged over the interval between the two sections of the light pulses. Next, the PC averages the backscatter signal generated from the first of the pulses over the same interval and normalises the RMS difference signal using the averaged signal to obtain a compensated difference signal that depends only on differences in the rate of change of phase of light of the light pulses as they travelled along the waveguide. This is repeated at different wavelengths to allow the compensated difference signal to be adjusted to represent the magnitude of the differences.
1. An apparatus for detecting a disturbance in the propagation of light in an optical waveguide comprising:
a light source for sending a light pulse along the waveguide, the light pulse being substantially coherent and varying in intensity over its duration to provide two sections of higher intensity separated from one another by a section of lower or substantially zero intensity;
a photodetector for generating a signal representing a time distributed intensity of light backscattered in the waveguide as the light pulse travels along the waveguide; and
a processor in communication with the photodetector,
wherein the light source sends two such light pulses along the waveguide,
wherein the photodetector generates first and second such signals, one for each of the light pulses, and
wherein the processor derives a difference signal indicative of differences between the first and second signals.
2. The apparatus of claim 1 , further comprising means for selecting sensitivity to the disturbance by varying the length of the section of lower or substantially zero intensity.
3. The apparatus of claim 1 , wherein the intensity of the light pulse varies with a substantially square waveform.
4. The apparatus of claim 1 , wherein the photodetector has a response time approximately equal to the duration of either of the two sections of higher intensity of the light pulse.
5. The apparatus of claim 1 , wherein the processor further performs the steps of:
averaging the first signal over a period approximately equal to the duration of the light pulses;
calculating a root mean square of the difference signal and averaging this over a period approximately the same as the period of averaging of the first signal; and
normalising the averaged root mean square of the difference signal using the averaged first signal to derive a compensated difference signal indicative of a change in the propagation of light in the waveguide.
6. The apparatus of claim 1 , wherein the light source sends light pulses having different wavelengths along the waveguide.
7. The apparatus of claim 1 , wherein the light source sends a further two such light pulses along the waveguide having a different wavelength from the two such light pulses and the photodetector generates further first and second such signals, one for each of the further light pulses.
8. The apparatus of claim 7 , having processing means for deriving a further difference signal indicative of differences between the further first and second signals.
9. The apparatus of claim 8 , wherein the processor further executes the steps of:
averaging the further first signal over a period approximately equal the duration of the further two such light pulses;
calculating a root mean square of the further difference signal and averaging this over a period approximately the same as the period of averaging of the further first signal;
normalising the averaged root mean square of the further difference signal using the averaged further first signal to derive a further compensated difference signal indicative of a change in the propagation of light in the waveguide; and
comparing the compensated difference signals at the two wavelengths to generate an adjusted compensated difference signal indicative of the magnitude of the change in the propagation of light in the waveguide.
10. The apparatus of claim 7 , wherein the processor further executes the step of comparing the difference signals to derive an adjusted difference signal indicating the magnitude of the change in the propagation of light in the waveguide.
11. An apparatus for optical time domain reflectometry comprising the apparatus of claim 1 .
12. An apparatus for detecting a change in the effective refractive index or optical path length of an optical waveguide comprising the apparatus of claim 1 .
13. The apparatus of claim 1 , wherein at least one of the light pulses is sufficiently coherent that light backscattered as it travels along the waveguide has at least a component of intensity detectable by the photodetector arising from interference between light backscattered from each of the two sections of higher intensity of the light pulse.
14. A method of detecting a disturbance in the propagation of light in an optical waveguide, comprising the steps of:
sending at least first and second light pulses along the waveguide, each light pulse being substantially coherent and each varying in intensity over its duration to provide two sections of higher intensity separated from one another by a section of lower or substantially zero intensity;
generating first and second signals representing time distributed intensity of light backscattered in the waveguide as the respective first and second light pulses travel along the waveguide; and
deriving a difference signal indicative of differences between the first and second signals.
15. The method of claim 14 , further comprising selecting sensitivity to the disturbance by varying the length of the section of lower or substantially zero intensity.
16. The method of claim 14 , wherein the intensity of the light pulse varies with a substantially square waveform.
17. The method of claim 14 , wherein a signal is generated with a response time approximately equal to the duration of each of the sections of higher intensity of the light pulse.
18. The method of claim 14 , further comprising:
averaging the first signal over a period approximately equal to the duration of the light pulses;
calculating a root mean square of the difference signal and averaging this over a period approximately the same as the period of averaging of the first signal; and
normalising the averaged root mean square of the difference signal using the averaged first signal to derive a compensated difference signal indicative of a change in the propagation of light in the waveguide.
19. The method of claim 14 , further comprising sending light pulses having different wavelengths along the waveguide.
20. The method of claim 14 , further comprising sending a further two such light pulses along the waveguide having a different wavelength to the prior two such light pulses and generating further first and second such signals, one for each of the further light pulses.
21. The method of claim 20 , comprising deriving a further difference signal indicative of differences between the further first and second signals.
22. The method of claim 21 , comprising comparing the difference signals to derive an adjusted difference signal indicating the magnitude of the change in the propagation of light in the waveguide.
23. The method of claim 21 , comprising:
averaging the further first signal over a period approximately equal the duration of the further two such light pulses;
calculating a root mean square of the further difference signal over a period approximately the same as the period of averaging of the further first signal;
normalising the averaged root mean square of the further difference signal using the averaged further first signal to derive a difference signal indicative of a change in the propagation of light in the waveguide; and
comparing the difference signals at the two wavelengths to indicate the magnitude of the change in the propagation of light in the waveguide.
24. A method of optical time domain reflectometry comprising the method of claim 14 .
25. A method of detecting a change in the effective refractive index or optical path length of an optical waveguide comprising the method of claim 14 .
26. The method of claim 14 , wherein each of the first and the second light pulses is sufficiently coherent that light backscattered as it travels along the waveguide has at least a component of intensity detectable by the photodetector arising from interference between light backscattered from each of the two sections of higher intensity of the light pulse.