DEVICE FOR THE REMOTE OPTICAL DETECTION OF GAS
    1.
    发明申请
    DEVICE FOR THE REMOTE OPTICAL DETECTION OF GAS 审中-公开
    用于远程光学检测气体的装置

    公开(公告)号:WO2008135654A3

    公开(公告)日:2008-12-31

    申请号:PCT/FR2008000365

    申请日:2008-03-19

    CPC classification number: G01N21/3504 G01N2021/1793

    Abstract: The invention relates to a device for the remote optical detection of a gas, that comprises a detection housing (30) connected to an electronic supply housing and to a man-machine interface, the detection housing including an infrared lens (46) for forming an image on a detector (50) with a micro-bolometres non-cooled matrix, a camera (64) of the CCD or CMOS type for observing in the visible spectrum the area observed, a set of electronic means (68) for driving the detector and for the acquisition and digitalisation of the infrared signals, and a processor (82) for processing the signals for detecting a gas in the area observed and for determining the concentration thereof.

    Abstract translation: 用于远程光学检测气体的装置技术领域本发明涉及一种用于气体的远程光学检测的装置,其包括连接到电子供应外壳和人机界面的检测外壳(30),检测外壳包括红外透镜(46),用于形成 在具有微型粒子非冷却矩阵的检测器(50)上的图像,CCD或CMOS类型的照相机(64),用于在可见光谱中观察所观察的区域,一组电子装置(68),用于驱动检测器 并用于红外信号的采集和数字化;以及处理器(82),用于处理用于检测所观察区域中的气体并确定其浓度的信号。

    DISPOSITIF DE FILTRAGE OPTIQUE POUR LA DETECTION DE GAZ

    公开(公告)号:CA2970369A1

    公开(公告)日:2016-06-16

    申请号:CA2970369

    申请日:2015-12-11

    Abstract: L'invention concerne un dispositif de filtrage optique (10), en particulier pour la détection de gaz à distance, comprenant un organe (22, 24, 26) comportant un passage tubulaire logeant une pluralité de structures réfléchissantes (34a, 34b, 34c, 34d) aptes à réfléchir des longueurs d'ondes infrarouge, lesdites structures (34a, 34b, 34c, 34d) étant allongées suivant l'axe du passage tubulaire et disposées autour de cet axe. Selon l'invention, les structures réfléchissantes (34a, 34b, 34c, 34d) comprennent des moyens de filtrage par absorption de bandes de longueurs d'ondes différentes situées dans la bande spectrale infrarouge.

    DEVICE FOR THE REMOTE OPTICAL DETECTION OF GAS

    公开(公告)号:CA2892406C

    公开(公告)日:2021-11-23

    申请号:CA2892406

    申请日:2013-11-20

    Abstract: Known gas detection devices do not allow precise measurement of gas concentrations. The invention relates to a detector device for optically detecting a gas in a zone of space under observation, the device comprising a camera and means for continuously detecting at least one gas in the observed zone by analyzing absorbance in a plurality of different spectral bands. The device further comprises a matrix of micromirrors that are individually steerable between at least two positions, in a first of which they reflect the radiant flux coming from the observed zone to the camera for detecting gas in said spectral bands, and in a second of which they reflect the radiant flux coming from the observed zone to a Fourier transform infrared spectroscope.

    Dispositivo de detección óptica de gas a distancia

    公开(公告)号:ES2869391T3

    公开(公告)日:2021-10-25

    申请号:ES13803164

    申请日:2013-11-20

    Abstract: Dispositivo de detección óptica de un gas, por ejemplo un contaminante, en una zona observada del espacio (20), que comprende una cámara (22), un espectroscopio de infrarrojos de transformada de Fourier y medios para la detección continua de al menos un gas en la zona observada sobre a partir de un análisis de absorbancia en una pluralidad de bandas espectrales diferentes, caracterizado porque comprende un conjunto de microespejos (14) orientables individualmente entre al menos dos posiciones en una primera de las cuales devuelven el flujo radiativo (16) procedente de la zona observada a la cámara (22) para la detección de gases en dichas bandas espectrales y una segunda posición en la que devuelven el flujo radiativo (16) procedente de la zona observada a dicho espectroscopio de infrarrojos de transformada de Fourier (24) y en el que la cámara comprende un sistema óptico (26) para tomar imágenes, filtros (28) y al menos un elemento sensible (30) sobre el que el sistema óptico (26) forma la imagen devuelta por el conjunto de microespejos (14) para realizar el análisis de absorbancia, siendo dicha cámara una cámara de infrarrojos o un generador de imágenes de infrarrojos.

    DISPOSITIF DE DETECTION OPTIQUE DE GAZ A DISTANCE

    公开(公告)号:FR2998371A1

    公开(公告)日:2014-05-23

    申请号:FR1261138

    申请日:2012-11-22

    Abstract: L'invention concerne un dispositif de détection optique d'un gaz dans une zone d'espace observée (20), comprenant une caméra (22) et des moyens de détection en continu d'au moins un gaz dans la zone observée à partir d'une analyse d'absorbance dans une pluralité de bandes spectrales différentes. Le dispositif comprend en outre une matrice de micromiroirs (14) individuellement orientables entre au moins deux positions dans une première desquelles ils renvoient le flux radiatif (16) en provenance de la zone observée vers la caméra (22) pour la détection de gaz dans lesdites bandes spectrales et une deuxième position dans laquelle ils renvoient le flux radiatif (16) en provenance de la zone observée vers un spectroscope infrarouge à transformée de Fourier (24).

    DISPOSITIF DE FILTRAGE OPTIQUE POUR LA DETECTION DE GAZ

    公开(公告)号:FR3030041A1

    公开(公告)日:2016-06-17

    申请号:FR1462391

    申请日:2014-12-12

    Abstract: L'invention concerne un dispositif de filtrage optique (10), en particulier pour la détection de gaz à distance, comprenant un organe (22, 24, 26) comportant un passage tubulaire logeant une pluralité de structures réfléchissantes (34a, 34b, 34c, 34d) aptes à réfléchir des longueurs d'ondes infrarouge, lesdites structures (34a, 34b, 34c, 34d) étant allongées suivant l'axe du passage tubulaire et disposées autour de cet axe. Selon l'invention, les structures réfléchissantes (34a, 34b, 34c, 34d) comprennent des moyens de filtrage par absorption de bandes de longueurs d'ondes différentes situées dans la bande spectrale infrarouge.

    DISPOSITIF DE DETECTION OPTIQUE DE GAZ A DISTANCE

    公开(公告)号:CA2892406A1

    公开(公告)日:2014-05-30

    申请号:CA2892406

    申请日:2013-11-20

    Abstract: L'invention concerne un dispositif de détection optique d'un gaz dans une zone d'espace observée (20), comprenant une caméra (22) et des moyens de détection en continu d'au moins un gaz dans la zone observée à partir d'une analyse d'absorbance dans une pluralité de bandes spectrales différentes. Le dispositif comprend en outre une matrice de micromiroirs (14) individuellement orientables entre au moins deux positions dans une première desquelles ils renvoient le flux radiatif (16) en provenance de la zone observée vers la caméra (22) pour la détection de gaz dans lesdites bandes spectrales et une deuxième position dans laquelle ils renvoient le flux radiatif (16) en provenance de la zone observée vers un spectroscope infrarouge à transformée de Fourier (24).

    8.
    发明专利
    未知

    公开(公告)号:FR2832799B1

    公开(公告)日:2006-11-03

    申请号:FR0115220

    申请日:2001-11-23

    Abstract: A measurement scale independent of temperature is determined in the calculating window from the ratio of differences in flow through the two filters. The gas concentration can be calculated from this scale by weighting the ratio using the mean flow in the calculating window or as a function of the difference between a preset temperature and the ground temperatures during the calculating window Optical gas detection system by observation at a distance of an area using a measurement filter with a transmission band comprising a specific absorption ray for the gas being sought and a reference filter with a transmission band corresponding to that of the measurement filter but not including the specific absorption ray for the gas. The process involves detecting the presence of the gas by determining the difference in flow through the gas (22) and coming from points at different temperatures in a calculation window, and of the ratio of the flow differences seen through the measurement filter and through the reference filter. The scale is equal to ( eta . phi p)/K, where eta is the ratio, phi the mean flow in the calculating window, p a parameter depending on the measuring and reference filters and K a normalization parameter equal to phi p for a preset temperature in the calculating window, e.g. 20 deg C. The values of the derivative with respect to the temperature of the spectral luminescence of a black body at a given mean temperature are calculated for difference ground temperatures to deduce the derivative with respect to the temperature of a ratio for the same mean temperature in the absence of gas. The values are recorded and the measured ratios weighted as a function of the difference between the ground temperatures and the preset mean temperature. For the detection of several gases, a filter assembly (F1, F2, F3) is used, with the transmission bands determined relative to each other as a function of the absorption rays of the gases (G1, G2, G3). Thus, a filter (F2) can be used as a reference filter for a gas (G1) and as a measuring filter for another gas (G2,G3), or vice versa, connecting the filters in pairs, each pair detecting one or more gases. An identification matrix is formed where the rows correspond to the pairs of filters and the columns to the gases to be detected. The matrix is formed by calibrating the various filters and is used to detect the presence and concentration of the gases. A series of filters with stepped transmission bands are used.

    9.
    发明专利
    未知

    公开(公告)号:NO20033308D0

    公开(公告)日:2003-07-22

    申请号:NO20033308

    申请日:2003-07-22

    Abstract: A measurement scale independent of temperature is determined in the calculating window from the ratio of differences in flow through the two filters. The gas concentration can be calculated from this scale by weighting the ratio using the mean flow in the calculating window or as a function of the difference between a preset temperature and the ground temperatures during the calculating window Optical gas detection system by observation at a distance of an area using a measurement filter with a transmission band comprising a specific absorption ray for the gas being sought and a reference filter with a transmission band corresponding to that of the measurement filter but not including the specific absorption ray for the gas. The process involves detecting the presence of the gas by determining the difference in flow through the gas (22) and coming from points at different temperatures in a calculation window, and of the ratio of the flow differences seen through the measurement filter and through the reference filter. The scale is equal to ( eta . phi p)/K, where eta is the ratio, phi the mean flow in the calculating window, p a parameter depending on the measuring and reference filters and K a normalization parameter equal to phi p for a preset temperature in the calculating window, e.g. 20 deg C. The values of the derivative with respect to the temperature of the spectral luminescence of a black body at a given mean temperature are calculated for difference ground temperatures to deduce the derivative with respect to the temperature of a ratio for the same mean temperature in the absence of gas. The values are recorded and the measured ratios weighted as a function of the difference between the ground temperatures and the preset mean temperature. For the detection of several gases, a filter assembly (F1, F2, F3) is used, with the transmission bands determined relative to each other as a function of the absorption rays of the gases (G1, G2, G3). Thus, a filter (F2) can be used as a reference filter for a gas (G1) and as a measuring filter for another gas (G2,G3), or vice versa, connecting the filters in pairs, each pair detecting one or more gases. An identification matrix is formed where the rows correspond to the pairs of filters and the columns to the gases to be detected. The matrix is formed by calibrating the various filters and is used to detect the presence and concentration of the gases. A series of filters with stepped transmission bands are used.

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