Temperature measuring arrangements using optical fibre sensor

Claim 2

A temperature measuring arrangement comprising a relatively long optical fibre temperature sensor doped along its length with material that absorbs light in dependence upon temperature, means for launching into one end of the temperature sensor fibre two contemporaneous light pulses, each having a different wavelength, and means for comparing variations of levels of back-scattered light of the two different wavelengths returned along the sensor fibre, with respect to the time of return of said back-scattered light, in order to provide an indication of the temperature distribution along the fibre, the two wavelengths correspond to different absorption wavelengths within the absorption band of the doped material.

Claim 3

A temperature measuring arrangement as claimed in claim 1, in which the light pulses of two different wavelengths are derived from respective lasers which are pulsed simultaneously by electric pulses produced by pulse generating means.

Claim 4

A temperature measuring arrangement as claimed in claim 2, in which the light pulse outputs from the two lasers are fed into power combining means which launches the pulses simultaneously into the sensor fibre.

Claim 5

A temperature measuring arrangement as claimed in claim 1, in which the back-scattered light of the two different wavelengths returned along the sensor fibre is fed into wavelength separation means which produces respective outputs at the two different wavelengths which are then applied to respective opto-electric detectors for the generation of electrical outputs arranged to be fed to comparator means to determine the ratio between the detected outputs and to provide an indication of temperature distribution along the sensor fibre.

Claim 6

A temperature measuring arrangement as claimed in claim 1, in which the dopant material is neodymium or europium.

Claim 7

A temperature measuring arrangement comprising a relatively long optical fibre temperture sensor doped along its length with material that fluoresces in response to the absorption of light in dependence upon temperature, means for launching light pulses into one end of the sensor fibre and means for detecting, at said one end, variations in the levels of fluorescent light which is emitted by the doped material in response to the light pulses and which returns to the launch end of the sensor fibre wherein the time of return of said fluorescent light and the instantaneous level thereof are indicative of the temperature distribution along the fibre.

Claim 8

A temperature measuring arrangement comprising a relatively long optical fibre temperture sensor doped along its length with material that fluoresces in response to the absorption of light in dependence upon temperature, means for launching light pulses into one end of the sensor fibre and means for detecting, at said one end, variations in the levels of fluorescent light which is emitted by the doped material in response to the light pulses and which returns to the launch end of the sensor fibre wherein the time of return of said fluorescent light and the instantaneous level thereof are indicative of the temperature distribution along the fibre.

Claim 9

A temperature measuring arrangement as claimed in claim 6, in which the dopant material of the sensor fibre effectively produces radiant re-emission of the absorbed light energy at a longer wavelength than that of the light pulses launched into the sensor fibre, the wavelength of these light pulses and the dopant material being chosen so that the light content of the light pulses as the latter reach the end of the sensor fibre remote from the launch end will still be at a reasonable level even after absorption of the light by the dopant material of the sensor fibre.

Claim 10

A temperature measuring arrangement as claimed in claim 6, in which the fluorescent light returned to the launch end of the sensor fibre is arranged to be measured in a single narrow wavelength region.

Claim 11

A temperature measuring arrangement as claimed in claim 6, in which the bandwidth of the fluorescent light is separated into two wavelengths or into specific wavelength regions and each wavelength or region is measured simultaneously in order to compensate for any variations in dopant material concentration along the sensor fibre, the variations in the ratio of levels of returned fluorescent light being used to deduce temperature distribution.

Claim 12

A temperature measuring arrangement as claimed in claim 9, in which the fluorescent light returned to the launch end of the sensor fibre is applied to filter means to provide light outputs at two different wavelengths and in which these outputs are applied to respective opto-electric detectors to produce electrical outputs which are then compared by means of a ratiometer to provide an indication of variations of temperature with time along the sensor fibre.

Claim 13

A temperature measuring arrangement as claimed in claim 6, in which light pulses of one wavelength are produced by a pulsed laser and launched into the sensor fibre.

Claim 14

A temperature measuring arrangement comprising a relatively long optical fibre temperature sensor doped along its length with material that absorbs light in dependence upon temperature, means for launching into one end of the temperature sensor fibre two contemporaneous light pulses, each having a different wavelength, from respective lasers fed into a combining means and means for comparing, at said one end, variations of levels of back-scattered light of the two different wavelengths returned along the sensor fibre, with respect to the time of return of said back-scattered light, in order to provide an indication of the temperature distribution along the fibre, the two wavelengths correspond to different absorption wavelengths within the absorption band of the doped material.

Claim 15

A temperature measuring arrangement comprising a relatively long optical fibre temperature sensor doped along its length with material that absorbs light in dependence upon temperature, means for launching into one end of the temperature sensor fibre two contemporaneous light pulses, each having a different wavelength, from respective lasers fed into a combining means and means for comparing, at said one end, variations of levels of back-scattered light of the two different wavelengths returned along the sensor fibre, with respect to the time of return of said back-scattered light, in order to provide an indication of the temperature distribution along the fibre, the two wavelengths correspond to different absorption wavelengths within the absorption band of the doped material.

Claim 16

A temperature measuring arrangement comprising a relatively long optical fibre temperature sensor doped along its length with material that absorbs light in dependence upon temperature, means for launching into one end of the temperature sensor fibre two contemporaneous light pulses, each having a different wavelength, and means for comparing, located at said one end, variations of levels of back-scattered light from the two different wavelengths returned along the sensor fibre, with respect to the return time thereof, in order to provide an indication of the temperature distribution along the fibre, the two wavelengths correspond to different absorption wavelengths within the absorption band of the doped material, wherein the back-scattered light of the two different wavelengths returned along the sensor fibre is fed into wavelength separation means which produces respective outputs at the two different wavelengths which are then applied to respective opto-electric detectors for the generation of electrical outputs arranged to be fed to comparator means to determine the ratio between the detected outputs and to provide an indication of temperature distribution along the sensor fibre.

Claim 17

A temperature measuring arrangement comprising a relatively long optical fibre temperature sensor doped along its length with material that absorbs light in dependence upon temperature, means for launching into one end of the temperature sensor fibre two contemporaneous light pulses, each having a different wavelength, and means for comparing, located at said one end, variations of levels of back-scattered light from the two different wavelengths returned along the sensor fibre, with respect to the return time thereof, in order to provide an indication of the temperature distribution along the fibre, the two wavelengths correspond to different absorption wavelengths within the absorption band of the doped material, wherein the back-scattered light of the two different wavelengths returned along the sensor fibre is fed into wavelength separation means which produces respective outputs at the two different wavelengths which are then applied to respective opto-electric detectors for the generation of electrical outputs arranged to be fed to comparator means to determine the ratio between the detected outputs and to provide an indication of temperature distribution along the sensor fibre.