GB2180639A - Determining atmospheric materials using lidar - Google Patents

Determining atmospheric materials using lidar Download PDF

Info

Publication number
GB2180639A
GB2180639A GB08518554A GB8518554A GB2180639A GB 2180639 A GB2180639 A GB 2180639A GB 08518554 A GB08518554 A GB 08518554A GB 8518554 A GB8518554 A GB 8518554A GB 2180639 A GB2180639 A GB 2180639A
Authority
GB
United Kingdom
Prior art keywords
constituent
radiation
atmosphere
spectrum
lidar
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
GB08518554A
Other versions
GB8518554D0 (en
GB2180639B (en
Inventor
Dr Arthur Maitland
Dr Roger Bradley Millington
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Teledyne UK Ltd
Original Assignee
English Electric Valve Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by English Electric Valve Co Ltd filed Critical English Electric Valve Co Ltd
Priority to GB8518554A priority Critical patent/GB2180639B/en
Publication of GB8518554D0 publication Critical patent/GB8518554D0/en
Publication of GB2180639A publication Critical patent/GB2180639A/en
Application granted granted Critical
Publication of GB2180639B publication Critical patent/GB2180639B/en
Expired legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/25Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
    • G01N21/31Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
    • G01N21/39Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using tunable lasers
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/25Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
    • G01N21/31Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
    • G01N21/35Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
    • G01N21/3504Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light for analysing gases, e.g. multi-gas analysis
    • G01N2021/3513Open path with an instrumental source
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/25Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
    • G01N21/31Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
    • G01N21/39Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using tunable lasers
    • G01N2021/392Measuring reradiation, e.g. fluorescence, backscatter
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/25Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
    • G01N21/31Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
    • G01N21/35Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
    • G01N21/3504Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light for analysing gases, e.g. multi-gas analysis
    • G01N21/3518Devices using gas filter correlation techniques; Devices using gas pressure modulation techniques

Landscapes

  • Physics & Mathematics (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Analytical Chemistry (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Optics & Photonics (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Optical Radar Systems And Details Thereof (AREA)
  • Investigating Or Analysing Materials By Optical Means (AREA)

Abstract

A lidar arrangement includes a laser 1 located between two mirrors 2 and 3, one of which 2 is partially transmissive to permit laser radiation to pass through it to form the transmitted beam of the lidar. A cell 4 contains an absorbing material is be moved into and out of the path of the laser radiation to produce two spectra. The absorbing material is a constituent which it is wished to monitor in the atmosphere. The transmitted lidar beam is scattered from the atmosphere and by observing the amplitude of the received scattered radiation for both spectra the amount of constituent in the atmosphere, and its location, may be ascertained. <IMAGE>

Description

SPECIFICATION Lidars This invention relates to lidars and more particularly to apparatus fortuning the spectrum in a differential lidarsystem. Lidarisan acronym for light detection and ranging. A lidaris a device for detecting and observing such things as cloud patterns or pollution in the atmosphere by directing a laser beam in the desired direction and observing the returned spectrum.
A differential lidar is one which transmitstwo signals at different distribution of wavelengths and by comparing the responses is able to detect a particular constituent of the atmosphere, for example, by using a differential lidar it is possible to detect whether or not sulphur dioxide is present in smoke.
Previously, the required distributions have been selected by means of a diffraction grating or a prism within the laser cavity. However, in wavelength selection by these methods, alignment is critical and the apparatus is difficult to maintain in the aligned state necessary for its successful operation.
This invention seeks to provide an improved lidar apparatus.
According to this invention there is provided lidar apparatus comprising meansformoving avolumeof absorbing material into and out ofthe path of laser radiation thereby producing a first spectrum which includes a certain wavelength distribution and a second spectrum in which the wavelength distribution has been modified by absorption bytheabsorb- ing material, the wavelength distribution being such as to interact with a constituent of an atmosphere, whereby the constituent can be monitored. Thus lidar apparatus in accordance with the invention may be made more robust and insensitive to misalignmentthan previously known apparatus. The interaction ofthe radiation at the chosen wavelength distribution with the constituent ofthe atmosphere is by absorption.Preferably,the absorbing material includes the constituent of the atmosphere to be monitored, thus enabling the desired first and second spectra to be easily and quickly produced, and advantageously the absorbing material is the constituent.
The invention is now further described by way of example with reference to the accompanying drawings in which: Figure 1 schematically illustrates lidar apparatus in accordance with the invention; and Figures2a, 2b, 3a and 3á illustrate the operation of the apparatus of Figure 1.
With reference to Figure 1, a lidar arrangement includes a xenon chloride laser 1 which is located between two mirrors 2 and 3, one of which 2 is partially transmissive to permit laser radiation to pass through itto form the transmitted beam of the lidar.
Acell 4 containing sulphurdioxide gas is also inclu- ded in the arrangement and is movable into and out ofthe path of the laser radiation as indicated by arrow5 to modify the wavelength distribution of the transmitted beam.
When the cell 4 is in the position shown in full lines the spectrum ofthe transmitted laser beam is that shown diagramatically in Figure 2a and includes radiation distributed about a peak at the wavelength X1.
When the cell 4 is in the position indicated by the broken lines such that it is interposed in the path of the laser radiation the spectrum of the radiation transmitted isthatshown in Figure2b.Thesulphur dioxide contained in the cell 4 absorbs radiation distributed about the wavelength X1.
To observe, say, whether sulphur dioxide is present in smoke emanating froma chimney, the output laser radiation is transmitted in the appropriate direction and scattering from the atmosphere is obse rved using a telescope (not shown) aligned along- sidethe laser 1. The amplitude ofthe signal received at the telescope when the spectrum of Figure 2a is transmitted is shown in Figure 3a, and thatforthe spectrum of Figure 2b is shown in Figure 3b. The cell 4is moved between its two positions a numberof times to obtain average responses for both ofthe output spectra, shown in Figures 2a and 2b.
The response shown in Figure 3b includes a peak6, received at a time t1 afterthe transmission of a pulse of laser radiation, which is dueto the presence of smoke in the atmosphere which returns a relatively large amount ofthe radiation. The received radiation is unaffected by the amount of sulphur dioxide present, since radiation at X1 has been removed by the cell4.
The response shown in Figure 3a includes a component 7 which is scattered from the smoke, as in Figure 3b, but also includes an additional component which has an amplitude which is dependent on the amount of sulphur dioxide present. If a small amount is present the peak8 is largerthan if a larger amount exists, when the peak 9 is reduced because of absorption by the sulphur dioxide.
Thus by normalising the responses shown in Figures 3a and 3b and substracting one from the other the amount of sulphur dioxide present may be monitored, and also its location.
If it is desired to monitor another constituent of the atmosphere, the cell 4 is arranged to contain that constituent to alter the spectra of the transmitted laser beam as desired.
1. Lidarapparatuscomprising means for moving avolume ofabsorbing material into and outofthe path of laser radiation thereby producing a first spectrum which includes a certain wavelength distribution and a second spectrum in which the wave- length distribution has been modified by absorption by absorbing material, the wavelength distribution being such as to interact with a constituent of an atmosphere whereby the constituent can be monitored.
2. Lidarapparatus as claimed in claim 1,and wherein the absorbing material includes the constituent.
3. Lidar apparatus as claimed in claim 2 and wherein the absorbing matsrie! it, the cnstituent.
**WARNING** end of DESC field may overlap start of CLMS **.

Claims (4)

**WARNING** start of CLMS field may overlap end of DESC **. SPECIFICATION Lidars This invention relates to lidars and more particularly to apparatus fortuning the spectrum in a differential lidarsystem. Lidarisan acronym for light detection and ranging. A lidaris a device for detecting and observing such things as cloud patterns or pollution in the atmosphere by directing a laser beam in the desired direction and observing the returned spectrum. A differential lidar is one which transmitstwo signals at different distribution of wavelengths and by comparing the responses is able to detect a particular constituent of the atmosphere, for example, by using a differential lidar it is possible to detect whether or not sulphur dioxide is present in smoke. Previously, the required distributions have been selected by means of a diffraction grating or a prism within the laser cavity. However, in wavelength selection by these methods, alignment is critical and the apparatus is difficult to maintain in the aligned state necessary for its successful operation. This invention seeks to provide an improved lidar apparatus. According to this invention there is provided lidar apparatus comprising meansformoving avolumeof absorbing material into and out ofthe path of laser radiation thereby producing a first spectrum which includes a certain wavelength distribution and a second spectrum in which the wavelength distribution has been modified by absorption bytheabsorb- ing material, the wavelength distribution being such as to interact with a constituent of an atmosphere, whereby the constituent can be monitored. Thus lidar apparatus in accordance with the invention may be made more robust and insensitive to misalignmentthan previously known apparatus. The interaction ofthe radiation at the chosen wavelength distribution with the constituent ofthe atmosphere is by absorption.Preferably,the absorbing material includes the constituent of the atmosphere to be monitored, thus enabling the desired first and second spectra to be easily and quickly produced, and advantageously the absorbing material is the constituent. The invention is now further described by way of example with reference to the accompanying drawings in which: Figure 1 schematically illustrates lidar apparatus in accordance with the invention; and Figures2a, 2b, 3a and 3á illustrate the operation of the apparatus of Figure 1. With reference to Figure 1, a lidar arrangement includes a xenon chloride laser 1 which is located between two mirrors 2 and 3, one of which 2 is partially transmissive to permit laser radiation to pass through itto form the transmitted beam of the lidar. Acell 4 containing sulphurdioxide gas is also inclu- ded in the arrangement and is movable into and out ofthe path of the laser radiation as indicated by arrow5 to modify the wavelength distribution of the transmitted beam. When the cell 4 is in the position shown in full lines the spectrum ofthe transmitted laser beam is that shown diagramatically in Figure 2a and includes radiation distributed about a peak at the wavelength X1. When the cell 4 is in the position indicated by the broken lines such that it is interposed in the path of the laser radiation the spectrum of the radiation transmitted isthatshown in Figure2b.Thesulphur dioxide contained in the cell 4 absorbs radiation distributed about the wavelength X1. To observe, say, whether sulphur dioxide is present in smoke emanating froma chimney, the output laser radiation is transmitted in the appropriate direction and scattering from the atmosphere is obse rved using a telescope (not shown) aligned along- sidethe laser 1. The amplitude ofthe signal received at the telescope when the spectrum of Figure 2a is transmitted is shown in Figure 3a, and thatforthe spectrum of Figure 2b is shown in Figure 3b. The cell 4is moved between its two positions a numberof times to obtain average responses for both ofthe output spectra, shown in Figures 2a and 2b. The response shown in Figure 3b includes a peak6, received at a time t1 afterthe transmission of a pulse of laser radiation, which is dueto the presence of smoke in the atmosphere which returns a relatively large amount ofthe radiation. The received radiation is unaffected by the amount of sulphur dioxide present, since radiation at X1 has been removed by the cell4. The response shown in Figure 3a includes a component 7 which is scattered from the smoke, as in Figure 3b, but also includes an additional component which has an amplitude which is dependent on the amount of sulphur dioxide present. If a small amount is present the peak8 is largerthan if a larger amount exists, when the peak 9 is reduced because of absorption by the sulphur dioxide. Thus by normalising the responses shown in Figures 3a and 3b and substracting one from the other the amount of sulphur dioxide present may be monitored, and also its location. If it is desired to monitor another constituent of the atmosphere, the cell 4 is arranged to contain that constituent to alter the spectra of the transmitted laser beam as desired. CLAIMS
1. Lidarapparatuscomprising means for moving avolume ofabsorbing material into and outofthe path of laser radiation thereby producing a first spectrum which includes a certain wavelength distribution and a second spectrum in which the wave- length distribution has been modified by absorption by absorbing material, the wavelength distribution being such as to interact with a constituent of an atmosphere whereby the constituent can be monitored.
2. Lidarapparatus as claimed in claim 1,and wherein the absorbing material includes the constituent.
3. Lidar apparatus as claimed in claim 2 and wherein the absorbing matsrie! it, the cnstituent.
4. Lidar apparatus substantially as illustrated in and described with reference to the accompanying drawings.
GB8518554A 1985-07-23 1985-07-23 Lidars Expired GB2180639B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
GB8518554A GB2180639B (en) 1985-07-23 1985-07-23 Lidars

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
GB8518554A GB2180639B (en) 1985-07-23 1985-07-23 Lidars

Publications (3)

Publication Number Publication Date
GB8518554D0 GB8518554D0 (en) 1985-08-29
GB2180639A true GB2180639A (en) 1987-04-01
GB2180639B GB2180639B (en) 1989-08-09

Family

ID=10582703

Family Applications (1)

Application Number Title Priority Date Filing Date
GB8518554A Expired GB2180639B (en) 1985-07-23 1985-07-23 Lidars

Country Status (1)

Country Link
GB (1) GB2180639B (en)

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3788742A (en) * 1971-06-24 1974-01-29 Westinghouse Electric Corp Gas monitoring system
US3998557A (en) * 1974-06-03 1976-12-21 Massachusetts Institute Of Technology Gas detector
GB2060873A (en) * 1979-10-01 1981-05-07 Hartmann & Braun Ag Photoelectric gas analysis device
US4425503A (en) * 1980-08-05 1984-01-10 The United States Of America As Represented By The Secretary Of The Army Method for detecting the presence of a gas in an atmosphere

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3788742A (en) * 1971-06-24 1974-01-29 Westinghouse Electric Corp Gas monitoring system
US3998557A (en) * 1974-06-03 1976-12-21 Massachusetts Institute Of Technology Gas detector
GB2060873A (en) * 1979-10-01 1981-05-07 Hartmann & Braun Ag Photoelectric gas analysis device
US4425503A (en) * 1980-08-05 1984-01-10 The United States Of America As Represented By The Secretary Of The Army Method for detecting the presence of a gas in an atmosphere

Also Published As

Publication number Publication date
GB8518554D0 (en) 1985-08-29
GB2180639B (en) 1989-08-09

Similar Documents

Publication Publication Date Title
US2930893A (en) Long path infrared detection of atmospheric contaminants
US7397568B2 (en) Coherent differential absorption lidar (dial)
US4871916A (en) Sensing of methane
EP0738899A1 (en) Distance measuring device
AU1732588A (en) Scrap detector
GB1475910A (en) Gas detection apparatus using radiation detector-s-
EP0018458A3 (en) Optical particle analyser
US20030089854A1 (en) Apparatus and method for remotely sensing hydrocarbons and other pollutants in vehicle emissions
KR20220025811A (en) Sensor arrangement for characterizing particles
CN106645082B (en) Gated fiber Raman spectrometer based on automatic focusing of laser ranging
US7184143B2 (en) Method for remote sensing of pollutant molecules in a transparent medium using ultra-short intense lasers
GB2180639A (en) Determining atmospheric materials using lidar
SE8901554L (en) Laser Detector
Gregor et al. 20-Hz eyesafe laser rangefinder for air defense
RU2540451C1 (en) Laser location system
DE69925899T2 (en) SENSOR SYSTEM
GB1010277A (en) Improvements in and relating to optical interforometers
US7426028B2 (en) Spectroscopic feedback for high density data storage and micromachining
CN104181545A (en) Coaxial aerosol laser radar system of human-eye safe wavelength
JP2581016B2 (en) Microscopic infrared spectrophotometer
Immler et al. A new LIDAR system for the detection of Cloud and aerosol backscatter, depolarization, extinction, and fluorescence
JPH05288681A (en) Apparatus for coherent anti-stokes&#39; raman scattering spectroscopy
Agroskin et al. Multifrequency sounding with DF-laser-based lidar system: preliminary results
Alcock et al. Frequency broadening in laser-induced sparks
Kawamura et al. Attenuation characteristics of a high‐power CO2 laser by an air discharge plasma column

Legal Events

Date Code Title Description
PCNP Patent ceased through non-payment of renewal fee