WO2005068977A1 - Sulphur dioxide detection method - Google Patents
Sulphur dioxide detection method Download PDFInfo
- Publication number
- WO2005068977A1 WO2005068977A1 PCT/AU2005/000035 AU2005000035W WO2005068977A1 WO 2005068977 A1 WO2005068977 A1 WO 2005068977A1 AU 2005000035 W AU2005000035 W AU 2005000035W WO 2005068977 A1 WO2005068977 A1 WO 2005068977A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- radiation
- wavelengths
- sulphur dioxide
- water vapour
- subsidiary
- Prior art date
Links
- RAHZWNYVWXNFOC-UHFFFAOYSA-N Sulphur dioxide Chemical compound O=S=O RAHZWNYVWXNFOC-UHFFFAOYSA-N 0.000 title claims abstract description 122
- 235000010269 sulphur dioxide Nutrition 0.000 title claims abstract description 37
- 239000004291 sulphur dioxide Substances 0.000 title claims abstract description 37
- 238000001514 detection method Methods 0.000 title claims description 23
- 230000005855 radiation Effects 0.000 claims abstract description 63
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Substances O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 claims abstract description 46
- 238000000034 method Methods 0.000 claims abstract description 24
- 238000005259 measurement Methods 0.000 claims description 5
- 238000012545 processing Methods 0.000 claims description 5
- 239000006096 absorbing agent Substances 0.000 description 9
- 238000010521 absorption reaction Methods 0.000 description 9
- 230000000694 effects Effects 0.000 description 6
- 238000004088 simulation Methods 0.000 description 5
- VIKNJXKGJWUCNN-XGXHKTLJSA-N norethisterone Chemical compound O=C1CC[C@@H]2[C@H]3CC[C@](C)([C@](CC4)(O)C#C)[C@@H]4[C@@H]3CCC2=C1 VIKNJXKGJWUCNN-XGXHKTLJSA-N 0.000 description 4
- 206010037844 rash Diseases 0.000 description 4
- 238000010586 diagram Methods 0.000 description 3
- 230000006870 function Effects 0.000 description 3
- 239000007789 gas Substances 0.000 description 3
- 239000002245 particle Substances 0.000 description 3
- 238000011160 research Methods 0.000 description 3
- 238000012360 testing method Methods 0.000 description 3
- QAOWNCQODCNURD-UHFFFAOYSA-N Sulfuric acid Chemical compound OS(O)(=O)=O QAOWNCQODCNURD-UHFFFAOYSA-N 0.000 description 2
- 238000005316 response function Methods 0.000 description 2
- 235000011149 sulphuric acid Nutrition 0.000 description 2
- 239000001117 sulphuric acid Substances 0.000 description 2
- 230000005457 Black-body radiation Effects 0.000 description 1
- NINIDFKCEFEMDL-UHFFFAOYSA-N Sulfur Chemical compound [S] NINIDFKCEFEMDL-UHFFFAOYSA-N 0.000 description 1
- 239000005864 Sulphur Substances 0.000 description 1
- 230000002547 anomalous effect Effects 0.000 description 1
- 230000003466 anti-cipated effect Effects 0.000 description 1
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 239000000203 mixture Substances 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
- 230000004044 response Effects 0.000 description 1
- QPILZZVXGUNELN-UHFFFAOYSA-N sodium;4-amino-5-hydroxynaphthalene-2,7-disulfonic acid Chemical compound [Na+].OS(=O)(=O)C1=CC(O)=C2C(N)=CC(S(O)(=O)=O)=CC2=C1 QPILZZVXGUNELN-UHFFFAOYSA-N 0.000 description 1
- CCEKAJIANROZEO-UHFFFAOYSA-N sulfluramid Chemical group CCNS(=O)(=O)C(F)(F)C(F)(F)C(F)(F)C(F)(F)C(F)(F)C(F)(F)C(F)(F)C(F)(F)F CCEKAJIANROZEO-UHFFFAOYSA-N 0.000 description 1
- 238000012546 transfer Methods 0.000 description 1
- 230000000007 visual effect Effects 0.000 description 1
- 238000011179 visual inspection Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
- G01N21/25—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands
- G01N21/31—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry
- G01N21/35—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
- G01N21/3504—Investigating 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
Definitions
- the invention relates to a sulphur dioxide detection method and apparatus.
- Volcanic ash and sulphur dioxide clouds constitute a serious hazard to aircraft even after the clouds have moved from the site of a volcanic eruption.
- the clouds include gases such as S0 2 which after a few days oxidises and hydrolises to form sulphuric acid droplets, either as an ash-acid mixture or as a coating over ash particles.
- gases such as S0 2 which after a few days oxidises and hydrolises to form sulphuric acid droplets, either as an ash-acid mixture or as a coating over ash particles.
- Both the ash particles and the sulphuric acid droplets of volcanic ash clouds are capable of causing significant damage to and possible 5 loss of an aircraft which encounters an ash cloud.
- the present invention relates to a method of detecting sulphur dioxide clouds comprising: measuring infrared radiation at a viewing elevation at or above the horizon and at a key wavelength at which there is a sulphur dioxide feature and in the vicinity of which there is a region where the amount of infrared radiation from water vapour in the atmosphere varies in accordance with a predetermined relationship; measuring radiation at two or more subsidiary wavelengths in said region; determining the amount of radiation from water vapour at the key wavelength from the measured radiation at the subsidiary wavelengths using the predetermined relationship; and determining whether a sulphur dioxide cloud is present from the measured infrared radiation at the key wavelength and the determined amount of radiation from water vapour.
- said subsidiary wavelengths are located either side of said key wavelength.
- the inventor has determined that the key wavelength should be one of 7.3 ⁇ m and 8.6 ⁇ m and that 7.3 ⁇ m is the preferred key wavelength.
- the key wavelength is 7.3 ⁇ m
- subsidiary wavelengths at ⁇ 0.5 ⁇ m are used.
- the inventor has established that for the region of these wavelengths the predetermined relationship is that radiation from water vapour varies in a substantially linear manner. Accordingly, the radiation from water vapour at the key wavelength can be interpolated from the radiation at the subsidiary wavelengths on the basis of this predetermined relationship.
- the inventor has also established that there is substantially less S0 2 absorption at this wavelength.
- the method may also involve compensating for background S0 2 in the atmosphere.
- the invention also provides a detection apparatus for detecting a sulphur dioxide cloud comprising: measurement means that measures infrared radiation at a viewing elevation at just below, or above the horizon and at a key wavelength at which there is a sulphur dioxide feature and in the vicinity of which there is a region where the amount of infrared radiation from water vapour in the atmosphere varies in accordance with a predetermined relationship, said measurement means also measuring infrared radiation at two or more subsidiary wavelengths in said region; and processing means for determining the amount of radiation from water vapour at the key wavelength from the measured radiation at the subsidiary wavelengths using the predetermined relationship and determining whether a sulphur dioxide cloud is present from the measured infrared radiation at the key wavelength and the determined amount of radiation from water vapour; and output means for generating an output signal indicative of the presence of a sulphur dioxide cloud when a sulphur dioxide cloud is present.
- the inventor has also determined that the method and apparatus of the present invention can be used to detect sulphur dioxide clouds from the ground or from an aircraft.
- Figure 1 illustrates the S0 2 absorption feature in the region 1200cm "1 to 1500cm "1 and the preferred measurement wavelengths of the invention
- Figure 2 is a schematic diagram of a S0 2 detection apparatus of the preferred embodiment
- Figure 3 illustrates two modes of operation of the apparatus
- Figure 4 is a schematic diagram of apparatus to be used from an aircraft
- Figures 5a - 5c represent normal climatic conditions
- Figures 6a and 6b represent variations on normal conditions to allow testing of the invention
- Figure 7 represents variations in S0 2 for testing
- Figure 8 shows variation in temperature with S0 2 concentration
- Figure 9 shows temperature plotted as a function of absorber amount.
- the term "key wavelength” is used to refer to a wavelength at which there is an appropriate S0 2 feature.
- a “wavelength” in the context of this specification does not imply a single wavelength but rather encompasses a band of radiation. Typically the width of the band will depend on the filter used to observe/measure light at the wavelength of interest.
- the numerical figures given in this specification are used to denote, in general terms, the centre of such bands, however, it will be appreciated by persons skilled in the art that some variation of the centre wavelength is possible.
- the term "subsidiary wavelength” is used to refer to a wavelength in a region in the vicinity of the key wavelength where a relationship can be established between radiation from water vapour at two or more subsidiary wavelengths and radiation from water vapour at the key wavelength.
- the preferred embodiment provides a method and apparatus that allows identification of sulphur dioxide clouds in the free atmosphere.
- the apparatus of the preferred embodiment uses an infrared detector, interference filters and focussing optics.
- the filters divide radiation within the band between 6.8 and 8.1 ⁇ m into three narrow bands .
- the central band corresponds to a strong S0 2 absorption feature caused by the antisymmetric stretch of the S0 2 molecule at 7.3 ⁇ m.
- the other bands are above and below this feature.
- the central band B c is sensitive to S0 2 concentrations.
- the lower band, Bj and higher band B h are used to account for the effects of water vapour on the absorption in band B c .
- B c is the key wavelength and Bi and B h are the subsidiary wavelengths in the preferred embodiment.
- Figure 1 illustrates the absorption feature due to S0 2 for the infrared region extending from 1200 cm “1 (8.33 ⁇ ) to 1500 cm “1 (6.67 ⁇ m) .
- B h (7.633-8.065 ⁇ m)
- B c (7.143-7.57 ⁇ m)
- Bi (6.897-7.042 ⁇ m
- the response functions are normalised to unity and scaled appropriately for plotting.
- the central wavenumber for the S0 2 absorption is 1363 cm -1 and the band extends from about 1320 cm “1 to about 1390 cm “1 .
- a filter covering this region responds to all the radiation from this band; whether the S0 2 feature be due to absorption or emission.
- water vapour and clouds also absorb and emit radiation in the region 7-8 ⁇ m.
- the inventor has realised that the two bands positioned either side of the central band can be used to eliminate the effects of water vapour.
- Water vapour absorbs and emits radiation throughout the region 7-8 ⁇ m.
- the amount of radiation absorbed or emitted depends on the amount of water vapour and on its location in the atmospheric column. Water vapour near the boundary of the earth's surface is generally warm and abundant. Water vapour near the tropopause (i.e. at jet aircraft cruising altitudes) is cold and sparse.
- the central band B c of the S0 2 detector of the preferred embodiment responds to radiation due to both S0 2 and water vapour.
- the lower and higher bands B c , B h of the detector are only sensitive to water vapour.
- the inventor has determined that the radiation from water vapour in the region surrounding B c behaves in a sufficiently linear manner to enable it to eliminate the effects of water vapour on the central band sufficiently for the purpose of detecting a sulphur dioxide cloud.
- the Planck blackbody radiation from Bi and Bh are linearly interpolated to estimate the radiation detected in B c due to water vapour only. This radiation amount is subtracted from the radiation actually measured by B c . The residual amount is due to S0 2 .
- the preferred embodiment utilises a predetermined relationship that water vapour behaves in a linear manner. Persons skilled in the art will appreciate that other predetermined relationships could be used, for example, relationships that are approximately linear.
- the detection apparatus 6 consists of four major components:
- Fore-optics 1 that focus a beam of incoming infrared radiation onto a detector.
- a filter wheel 2 consisting of at least three narrow band interference filters that isolate radiation into the bands: B 2 , B c and B h .
- An infrared detector array 3 sensitive to radiation in the 7-8 ⁇ m region.
- Processing means 4 for processing the detector signal to determine whether S0 2 and hence a sulphur dioxide cloud is present.
- Figure 3 is a schematic diagram illustrating two modes of operation of a detection apparatus 6 that senses infrared radiation in order to detect S0 2 clouds.
- a first mode assumes that the detection apparatus 6 is on board an aircraft 7 and views the S0 2 cloud ahead at a small angle to the horizontal.
- the second mode assumes that the detection apparatus 6 is based on the ground and views the cloud at a large angle to the horizontal (e.g. zenith viewing) .
- the detection apparatus of the preferred embodiment may be operated from the ground viewing the sky above or from an aircraft viewing forwards at just below or above the horizon.
- the principal mode of operation is anticipated to be from an aircraft with the instrument having an unobstructed view of the atmosphere ahead of the aircraft as the inventor has established that the method works best when water vapour path amount is less than lg cm "2 .
- water vapour path is defined as the integral of the water vapour concentration with distance along the line of sight between instrument and target.
- the view should be horizontal or a few degrees (3-5°) above the horizon, so that the background radiation is cold.
- the processor 4 can be configured to account for changes in viewing zenith angle, making the technique insensitive to the viewing direction. For the case of a detection apparatus 6 viewing ahead of an aircraft at a zenith angle of Z degrees, the detection apparatus 6 provides three signals to the processor 4. A synthetic signal corresponding to the amount of radiation from water vapour is determined through linear interpolation of the signals from Bj and B h . This signal labeled B c is compared to the signal from B c .
- the processor 4 then computes the S0 2 amount at the key wavelength B c using B c and the original signal B c .
- the processor 4 uses pre-defined look-up tables that account for standard atmospheric conditions (tropical, mid-latitude, and polar) and the viewing geometry to compensate for background S0 2 .
- the detector array 3 provides an image of the S0 2 amount with a spatial resolution that depends on the exact number of detector elements in the array (320x240 is recommended) and the distance to the S0 2 cloud. Distance information is supplied by the detection apparatus 6, however, the S0 2 anomaly will be detected at distances of up to several 100 kms depending on the cruising altitude and clarity of the atmosphere ahead.
- the detection apparatus 6 produces an output 5, for example in the form of an amount of S0 2 or an alarm signal indicating the presence of sufficient S0 2 to pose a problem.
- the alarm signal may cause an audible or visual alarm in an aircraft.
- Figure 4 illustrates how the apparatus works in the case of being mounted in an aircraft.
- the processor 4 In addition to signals from the detector 3 the processor 4 also receives aircraft altitude information 8 from the aircraft and standard atmosphere information 9 from a memory associated with the processor.
- a sophisticated radiative transfer model-MODTRAN (Berk, et al., 1989) is used to model the response expected from a single-element detector viewing arealistic atmosphere.
- the viewing geometry is varied in the simulations to account for viewing from below the S0 2 cloud, viewing from above, and viewing at a small angle along a nearly horizontal path.
- the amount of S0 2 is varied, as is the main other gaseous absorber in the region-water vapour. We refer to the amount of S0 2 as the cloud thickness.
- the temperature profile is shown in Figure 6a. Varying the profile has little effect on the retrieval and detection algorithm because the algorithm uses differences in temperatures. No further simulations were performed on this parameter because of its insensitivity.
- model simulations have been performed for the case of horizontal viewing from a platform (e.g. an aircraft) directly ahead and towards an S0 2 cloud.
- the cloud thickness (as measured in the viewing direction) is varied from 10 km to 500 km and the concentration within the cloud is varied from background levels to «0.1 ppmV. This range of concentration covers the smallest eruptions (that are likely to reach these heights, e.g. Hekla-style eruptions) to the largest observed this century (e.g. Pinatubo-style eruptions) .
- the results of these model simulations are summarised in two figures.
- Figure 8 shows the variation of the temperature anomaly (the temperature difference between the synthetic signal and the measured signal as a function of cloud thickness) .
- the family of curves 20-27 generated from the modelling are lines of constant concentration for S0 2 concentration varying from 0.0136 ppmV 20 to 0.1083 pp V 27.
- the points that lie on vertical lines correspond to lines of constant cloud thickness.
- the temperature anomaly increases towards a limiting value (AT « -2 K) .
- the opaque limit is reached either by increasing concentration or increasing cloud thickness, since both quantities increase optical depth and hence absorption. Beyond a thickness of 500 km, the cloud is essentially opaque and the radiative process changes from absorption to emission.
- Figure 9 provides an alternate way of understanding the physical processes involved in S0 2 detection.
- the temperature anomaly is plotted as a function of absorber amount.
- the plot indicates that for a given anomaly, several values of absorber amount are possible, depending on the cloud thickness and concentration. Thus, it is not possible to uniquely quantify the absorber amount from the temperature anomaly without knowing either the concentration or the cloud thickness . In practice it is not necessary to know these quantities, as the purpose of the invention is to detect the presence of S0 2 gas in the free atmosphere, rather than quantify the amount.
- the modelling does give an indication of the limits within which detection of S0 2 is possible. At the lower end, for cloud thicknesses of 10 km or less, the S0 2 concentration must be larger than «0.06 ppmV.
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- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Analytical Chemistry (AREA)
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- General Health & Medical Sciences (AREA)
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Abstract
Description
Claims
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
EP05700067A EP1706726A4 (en) | 2004-01-16 | 2005-01-14 | Sulphur dioxide detection method |
AU2005205610A AU2005205610A1 (en) | 2004-01-16 | 2005-01-14 | Sulphur dioxide detection method |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
AU2004900213A AU2004900213A0 (en) | 2004-01-16 | Sulphur dioxide detection method | |
AU2004900213 | 2004-01-16 |
Publications (1)
Publication Number | Publication Date |
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WO2005068977A1 true WO2005068977A1 (en) | 2005-07-28 |
Family
ID=34754156
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/AU2005/000035 WO2005068977A1 (en) | 2004-01-16 | 2005-01-14 | Sulphur dioxide detection method |
Country Status (2)
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EP (1) | EP1706726A4 (en) |
WO (1) | WO2005068977A1 (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7371335B2 (en) | 2004-10-21 | 2008-05-13 | E.I. Dupont De Nemours And Company | Curable thick film compositions for use in moisture control |
WO2011135060A1 (en) | 2010-04-29 | 2011-11-03 | Norsk Institutt For Luftforskning | System and method for detecting adverse atmospheric conditions ahead of an aircraft |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3805074A (en) * | 1973-01-02 | 1974-04-16 | Texas Instruments Inc | Spectral scan air monitor |
EP0087077A2 (en) * | 1982-02-23 | 1983-08-31 | Siemens Aktiengesellschaft | Measuring device for optical gas analysis |
US5654700A (en) * | 1990-04-09 | 1997-08-05 | Commonwealth Scientific And Industrial Research Organization | Detection system for use in an aircraft |
US6822236B1 (en) * | 2002-05-25 | 2004-11-23 | Ophir Corporation | Method of optimizing a response of a gas correlation radiometer to a trace amount of a target gas |
Family Cites Families (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS6011122A (en) * | 1983-07-01 | 1985-01-21 | Shimadzu Corp | Method for compensating interference in non-dispersive type infrared analysis |
WO2002066966A1 (en) * | 2001-01-08 | 2002-08-29 | California Analytical Instruments, Inc. | Method and apparatus for the determination of total sulfur in a gas |
-
2005
- 2005-01-14 WO PCT/AU2005/000035 patent/WO2005068977A1/en active Application Filing
- 2005-01-14 EP EP05700067A patent/EP1706726A4/en not_active Withdrawn
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3805074A (en) * | 1973-01-02 | 1974-04-16 | Texas Instruments Inc | Spectral scan air monitor |
EP0087077A2 (en) * | 1982-02-23 | 1983-08-31 | Siemens Aktiengesellschaft | Measuring device for optical gas analysis |
US5654700A (en) * | 1990-04-09 | 1997-08-05 | Commonwealth Scientific And Industrial Research Organization | Detection system for use in an aircraft |
US6822236B1 (en) * | 2002-05-25 | 2004-11-23 | Ophir Corporation | Method of optimizing a response of a gas correlation radiometer to a trace amount of a target gas |
Non-Patent Citations (6)
Title |
---|
ALAN ROBOCK. ET AL.: "Volcanism and the earth's atmosphere.", 2003, GEOPHYSICAL MONOGRAPH., article PRATA J. ET AL: "Global, long term sulphur dioxide measurements from TOVS data: A new tool for study explosive volcanism and climate." * |
DATABASE WPI Week 198336, Derwent World Patents Index; Class S03, AN 1983754335 * |
PATENT ABSTRACTS OF JAPAN * |
PUGNAGHIS S. ET AL: "Estimation of SO2 abundance in the eruption plume of Mt. Etna using two MIVIS thermal infrared channels: a cade study from the Sicily-1997 Campaing.", BULL VOLCANO., vol. 64, 2002, pages 328 - 337 * |
See also references of EP1706726A4 * |
WATSON I.M. ET AL: "Thermal infrared remote sensing of volcanic emissions using the moderate resolution imaging spectroradiometer.", JOURNAL OF VOLCANOLOGY AND GEOTHERMAL RESEARCH., vol. 135, 2004, pages 75 - 89 * |
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7371335B2 (en) | 2004-10-21 | 2008-05-13 | E.I. Dupont De Nemours And Company | Curable thick film compositions for use in moisture control |
WO2011135060A1 (en) | 2010-04-29 | 2011-11-03 | Norsk Institutt For Luftforskning | System and method for detecting adverse atmospheric conditions ahead of an aircraft |
DE212011100091U1 (en) | 2010-04-29 | 2013-02-22 | Norsk Institutt For Luftforskning | A system for detecting adverse atmospheric conditions in front of an aircraft |
US10063794B2 (en) | 2010-04-29 | 2018-08-28 | Nicarnica Aviation As | System and method for detecting adverse atmospheric conditions ahead of an aircraft |
US10440291B2 (en) | 2010-04-29 | 2019-10-08 | Nicarnica Aviation As | System and method for detecting adverse atmospheric conditions ahead of an aircraft |
Also Published As
Publication number | Publication date |
---|---|
EP1706726A4 (en) | 2008-03-12 |
EP1706726A1 (en) | 2006-10-04 |
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