WO2004051211A2 - Detecteur par voie optique de la presence de bulles de gaz dans un liquide - Google Patents
Detecteur par voie optique de la presence de bulles de gaz dans un liquide Download PDFInfo
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- WO2004051211A2 WO2004051211A2 PCT/FR2003/003480 FR0303480W WO2004051211A2 WO 2004051211 A2 WO2004051211 A2 WO 2004051211A2 FR 0303480 W FR0303480 W FR 0303480W WO 2004051211 A2 WO2004051211 A2 WO 2004051211A2
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- light
- liquid
- detector
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- light source
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- 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
- G01N21/47—Scattering, i.e. diffuse reflection
- G01N21/49—Scattering, i.e. diffuse reflection within a body or fluid
Definitions
- the invention relates to the field of detectors optically for the presence of gas bubbles in a liquid.
- the invention can be used not exclusively for the detection of gas bubbles in a cooling water circuit of an internal combustion engine of a motor vehicle.
- Document WO 98/55849 describes a device for detecting a gas leak in a cooling system by using means for detecting the presence of gas bubbles.
- the device implemented in document WO 98/55849 comprises a light source aligned with a light detector such that the source and the detector are optically coupled by an optical path, this being defined by the path taken by the light between its emission by the source and its reception by the detector.
- a conversion device connected to the light detector, produces an electronic signal in response to the amount of light received by the light detector from the light source.
- This device compares the electronic signal in response to the amount of light received by the light detector with a reference signal corresponding to the amount of light received by the detector when the optical path is not obstructed by the passage of a bubble. . If this difference is greater than a predetermined threshold value, then the passage of a gas bubble through the optical path is detected. This device makes it possible to detect the presence of gas bubbles in the cooling, sign of the presence of a leak in said cooling system.
- the reference value is fixed over time.
- the system exhibits optical drifts (dirt, opacification, etc.) and undergoes temperature variations such that its properties are modified over time.
- the sensitivity of the system is then altered and it is possible that after a certain time bubbles are not detected and that the corresponding alert is not therefore triggered. It is also possible that a small amount of bubbles are considered to be too large and that a false alarm is then triggered.
- An object of the invention is to provide a device for optically detecting the presence of bubbles that is simple, economical and reliable while overcoming the drawbacks of the systems described above.
- the invention proposes a method for detecting gas bubbles in a liquid suitable for a device comprising a light source, a light detector and a control and information processing unit connected to a client system. comprising the steps of acquiring successive measurements of the light intensity coming from the light source and perceived by the light detector and of calculating the variation between two successive measurements of said light intensity.
- the time difference between two successive measurements is very small compared to the time to be observed so that the sensitivity of the system is significantly altered due in particular to optical drifts and variations in temperature. So the transformations of the properties of the system during said time difference between two successive measurements cannot distort the measurement of the variation of the light intensity between two successive measurements.
- the process which is the subject of the invention is thus insensitive to temporal modifications of the properties of the system.
- the method for detecting gas bubbles in a liquid further comprises a step of comparing said variation between two successive measurements of the light intensity to a value predefined threshold S.
- the system implemented in this preferred embodiment of the invention detects the presence of a gas bubble in the liquid if the measurement of the variation between two successive measurements of the light intensity is greater than this threshold S.
- control and information processing unit further comprises an alert counter incremented by a predefined value A when the variation between two successive measurements of the light intensity perceived by the detector is greater than the threshold S and decremented by a predefined value B otherwise.
- the alert counter has, as an option, a predefined alert value C, such that if the value of said alert counter exceeds the alert value C, the client system is informed that the maximum authorized bubble rate is exceeded.
- the alert counter also has an optional predefined value D, called the end of alert value, such that the client system is constantly informed that the bubble rate is higher than the maximum authorized bubble rate only when the alert counter is less than said alert end value D.
- the method for detecting gas bubbles further comprises a step for calculating the average value of a plurality of said variations between two successive measurements of the light intensity.
- the system implemented in this second preferred embodiment of the invention then returns this average value which is representative of the rate of gas bubbles in the liquid.
- control and information processing unit further to comprise a light source control module capable of controlling the polarization value of the light source, which makes it possible to carry out a new system calibration.
- This light source control module is in particular capable of carrying out a periodic polarization of the light source. It can, as an option, have a detector for exceeding a predefined polarization threshold. With such a threshold crossing detector, it is then possible, under certain conditions related to the optical configuration adopted, to detect whether the sensor consisting of the source and the light detector is immersed in the liquid or not.
- the light source and the light detector are arranged substantially orthogonally.
- the step of acquiring successive measurements of the light intensity perceived by the light detector then makes it possible to acquire measurements of the quantity of light rays emitted by the light source which are reflected if necessary during the presence of bubbles on the surface of a gas bubble in a direction substantially orthogonal from the direction of incidence towards the light detector.
- the light source and the light detector can also be arranged substantially adjacent to each other.
- the step of acquiring successive measurements of the light intensity perceived by the light detector then makes it possible to acquire measurements of the quantity of light rays emitted by the light source which are reflected if necessary during the presence of bubbles on the surface of a gas bubble in one direction substantially parallel to the direction of incidence towards the light detector.
- a temperature measuring element and at least one switch associated with said temperature measuring element can be added to the device.
- the switch is able to change state when a gas bubble is detected.
- the control and information processing unit transmits, via an interface module, to the client system information on the temperature of the liquid and the presence of gas bubbles in the liquid.
- a high level signal of amplitude proportional to the temperature of the liquid when the presence of a bubble is not detected or of low level when the presence of a bubble is detected is then supplied to the client system on a single wire.
- an electrode system capable of measuring the resistivity of the ambient medium can also be added to the device.
- the client system is then informed that the sensor consisting of the source and the light detector is not immersed in the liquid when the electrode system identifies the ambient medium as not being the liquid.
- the switch associated with the temperature element then advantageously changes state when a gas bubble is detected and when there is no liquid.
- the client system can then be informed by a high level signal of amplitude proportional to the temperature of the liquid when the presence of a bubble is not detected and the sensor is immersed in the liquid or of low level when the presence a bubble is detected or when the sensor is not immersed in the liquid.
- the light source and the light detector are arranged substantially face to face.
- the light emission stage then makes it possible to emit light from the light source of specific wavelength such that it is strongly (reciprocally weakly) absorbed by the liquid and little (reciprocally strongly) absorbed by the gas constituting the bubbles.
- the measurement acquisition step successive of the light intensity perceived by the light detector can make it possible to acquire measurements of the quantity of light rays emitted by the light source which are deflected towards the light detector if necessary during the presence of bubbles due to the fact differences in the diffraction index between the liquid and the gas constituting the bubbles at the surface of said bubbles.
- a temperature measuring element and at least one switch associated with said temperature measuring element can be added to the device.
- the switch changes state when a gas bubble is detected.
- the control and information processing unit transmits, via an interface module, to the client system information on the temperature of the liquid and the presence of bubbles in the liquid.
- a periodic signal is supplied to the client system on a single wire and the period of said signal is formed by a first phase constituted by a constant high level signal of amplitude proportional to the temperature of the liquid and by a second phase constituted by a pulse train with modulated width, the pulse width being modulated according to the average value of the successive variations of the light intensity perceived by the light detector.
- the client system can be informed that the sensor is not immersed in the liquid when the polarization value of the light source exceeds a predefined threshold value T, called the polarization alert threshold value.
- the client system can then be informed of information on the temperature of the liquid, the presence of bubbles in the liquid and the non-immersion of the sensor in the liquid by a periodic signal whose period is formed by a first phase consisting of a constant signal of high level of amplitude proportional to the temperature of the liquid and of a second phase constituted by a train of pulses of modulated width, the width of the pulses being modulated according to the average value of the successive variations of the light intensity perceived by the detector of light and said width being maximum when the sensor is not immersed in the liquid.
- the invention also relates to a device for detecting gas bubbles in a liquid comprising means for emitting light, means for detecting light and means for controlling and processing information linked to the means for detecting light. characterized in that following the emission of light by the light emission means and the detection of light by the light detection means, the control and information processing means are capable of obtaining means detecting light successive measurements of the light intensity detected by the light detection means and calculating a variation of the light intensity between two successive measurements of the light intensity.
- FIG. 1 shows a block diagram of the device for detecting gas bubbles in a liquid according to a first arrangement of the source and the light detector.
- FIG. 2 shows a block diagram of the device for detecting gas bubbles in a liquid according to a second arrangement of the source and the light detector.
- FIG. 3 shows a block diagram of the device for detecting gas bubbles in a liquid according to a third arrangement of the source and the light detector.
- FIG. 4 shows a block diagram of an electronic control and information processing unit according to a first preferred embodiment of the invention.
- FIG. 5 shows a block diagram of an electronic control and information processing unit according to a second preferred embodiment of the invention.
- - Figure 6 shows the interfacing of the electronic control and information processing unit with a client system in the context of the first preferred embodiment of the invention.
- FIGS. 1, 2 and 3 represent a device according to the invention essentially comprising a light source 1 and a light detector 2 associated with a control and information processing unit 6.
- the device is interfaced with a client system 8 is carried out via an interface module 7.
- the light is emitted by the light source 1 in an illumination zone 4.
- the field of vision of the light detector 2 defines a vision zone 5.
- the intersection of the viewing area 5 with the lighting area 4 defines a bubble detection area 3.
- the light source 1 can be any type of source, coherent or not, of electromagnetic radiation (for example a flashlight, a light-emitting diode, etc.).
- the light detector 2 is any of the conventional light detectors (for example a photodiode, a phototransistor, a photoresistor, etc.).
- the light detector 2 generates an electrical signal 17 in response to an amount of light coming from the light source 1 and perceived by the detector 2 in the viewing area 5. This electrical signal 17 is then sent to the control unit and information processing 6 so that an associated temporal variation is measured.
- the light source 1 and the light detector 2 can also be arranged in parallel as shown in FIG. 2.
- the light detector 2 then picks up the reflected light in a direction substantially parallel to the direction of incidence of the light emitted by the light source 1.
- the light source 1 and the light detector 2 are arranged face to face so that the light emitted by the source 1 hits the detector 2 directly. 'illumination 4 and vision 5 are then substantially combined and the detection zone 3 corresponds to the path taken by the light between its emission by the light source 1 and its reception by the light detector 2.
- Different techniques can be chosen, in particular those based on the absorption of a specific wavelength or on the diffraction of light rays.
- the wavelength of the light emitted by the light source 1 towards the light detector 2 can thus be strongly absorbed by the liquid and little absorbed by the gas constituting the bubbles.
- the light emitted by the light source 1 travels its path in a liquid with a high absorption coefficient so that said light is only weakly perceived by the light detector 2.
- the light emitted by the light source 1 travels part of its path in a gas with a low absorption coefficient.
- the amount of light perceived by the light detector 2 when a bubble is present in the detection zone 3 is then greater than that perceived by the detector when no bubble is present in the detection zone 3. It it follows that the passage of a gas bubble in the detection zone 3 creates a variation of the electrical signal at the terminals of the light detector 2.
- the light rays emitted by the light source 1 towards the light detector 2 can be deflected when a gas bubble is present in the detection zone 5 due to the differences in refractive index which exist between the liquid and the gas at the bubble surface.
- the passage of a gas bubble in the detection zone then causes a variation in the light intensity perceived by the detector 2, the brightness at the level of the detector being modified due to the deflection of the light rays.
- the optical materials used can be determined to transmit a maximum of light when the sensor is in a gas and a much smaller amount when the sensor is immersed in a liquid.
- the light rays are effectively strongly curved and therefore strongly brought to the light detector 2 when the light travels its entire path in a gas.
- the light rays are slightly curved and consequently weakly brought to the light detector 2 when the light travels the whole of its path in a liquid. We can then take into account the abnormally high amount of light perceived by the light detector 2 when the sensor is immersed in an ambient medium consisting of gas in order to determine whether said sensor is immersed in the liquid or not.
- FIGS. 4 and 5 respectively represent the first and the second preferred embodiment of the invention.
- control and information processing unit 6 essentially comprises a control module 15 for the light source 1, an analog / digital conversion module 11 capable of digitizing the electrical signal 17 generated by the light detector 2 and a light intensity processing module in the bubble detection zone 3,
- the electrical signal 17 generated by the light detector 2 in response to the quantity of light which it perceives is digitized via the analog / digital conversion module 11.
- the control of the light source 1 must be active during the acquisition of the corresponding signal of the light intensity perceived by the light detector 2.
- the control of the source is carried out by the control module 15 of the light source and is either continuous or, as is the case in the description, drawn and synchronized with the acquisition via a synchronization module 14.
- the light source control module 15 is capable of periodically polarizing the light source 1 and of measuring the electrical signal 17 collected on the light detector 2.
- the polarization can be done on several levels in order to best adjust the intensity of the light emitted.
- This calibration is typically carried out by successively testing the possible polarization values of the light source and retaining the polarization value having given the best voltage of the electrical signal 17 collected on the light detector, that is to say the voltage best framed in the voltage range possible.
- This calibration is done at regular intervals to compensate for the drifts in the optical characteristics of the system (soiling, clouding, etc.) as well as those due to temperature variations.
- the time interval is typically between 10 s and 1 min. It thus appears that an advantage of the invention lies in the fact that the drifts of the system do not affect the sensitivity of the device implemented by the invention.
- the detection of the presence of a gas bubble in the detection zone 3 is done by measuring the variation in the light intensity perceived by the light detector 2.
- the time scale for measuring these variations must correspond to the average time taken by a bubble to traverse the detection zone 3, which time itself depends on the size of the detection zone and on the speed of the bubbles to be detected.
- the time constant is between a few hundred microseconds and a few milliseconds for a speed of a few meters per second.
- a temperature measuring device as already described in European patent application EP 1 231 463 to which one can refer for more information.
- the incorporation of such a device makes it possible to obtain a dual-function sensor (liquid temperature / presence of gas bubbles in the liquid).
- a temperature probe is used which can be short-circuited when the device has detected the presence of bubbles.
- the medium effectively transmits much more light than normal.
- the polarization value of the light source therefore takes an abnormally low value.
- a detector 16 when a predefined polarization threshold is exceeded makes it possible to detect whether the sensor consisting of the source and the light detector is immersed in the liquid or not.
- the client system 8 is then alerted via the interface module 7 of the complete absence of liquid at the level of the sensor when the polarization value of the light source 1 is less than a predefined threshold value T and is detected as such by the overshoot detector 16 of a predefined polarization threshold.
- the module 9 for processing the light intensity comprises logic comparison means 12 capable of detecting a significant variation in the light intensity between two successive measurements as well as means for statistical processing 21 of said variation capable of providing information on whether or not the tolerated bubble limit rate has been exceeded.
- Said logic comparison module 12 consists of means 18 capable of calculating the variation of the light intensity between two successive measurements made at the level of the light detector 2 and of means 19 capable of detecting the exceeding of a predetermined threshold S.
- the variation in the light intensity is then calculated by comparing, via the means 18, the value of the electrical signal 17 to that previously obtained.
- the measurement of the variation in the light intensity between two successive measurements is then compared with a predetermined threshold S via the means 19 for detecting that the threshold is exceeded. If the difference between these two successive values is greater than the threshold S, the system considers that a bubble is present in the detection zone 3.
- the alert counter 13 of the means of statistical processing 21 of the variation between successive measurements of the light intensity is incremented by a predetermined value A. Otherwise, this same counter is decremented by a value B.
- the values A and B are such that A is greater than B and that their A / B ratio is generally between 10 and 1000.
- the alert counter 13 is bounded between two predefined values. If it exceeds an alert value C, the control and information processing unit 6 then informs the client system 8 via the interface module 7 that the bubble rate is higher than the authorized limit rate. Said value C is generally between 70% and 95% of the maximum value of the alert counter 13. To optimize the system, a hysteresis can be set up thanks to an alarm end value D which avoids transient problems between the two output states
- the values C and D are fixed so that C is greater than D.
- the A / C ratio is typically between 1/25 and 1/250 and the D / C ratio typically between 3/10 and 8/10.
- a time delay can also be added to the system in order to advantageously increase the functional approval of the detector.
- the value C is generally, but not necessarily, equal to C.
- the response time is inversely proportional to the quantity of bubbles present in the detection zone. A very large presence of bubbles is detected very quickly, while a small quantity is analyzed longer and more finely in order to be sure that the detection is founded. This avoids any false alarm.
- the module is inversely proportional to the quantity of bubbles present in the detection zone. A very large presence of bubbles is detected very quickly, while a small quantity is analyzed longer and more finely in order to be sure that the detection is founded. This avoids any false alarm.
- the module is inversely proportional to the quantity of bubbles present in the detection zone. A very large presence of bubbles is detected very quickly, while a small quantity is analyzed longer and more finely in order to be sure that the detection is founded. This avoids any false alarm.
- the module is inversely proportional to the quantity of bubbles present in the detection zone. A very large presence of bubbles is detected very quickly, while a small quantity is analyzed longer and more finely in order to be sure that the detection is founded. This avoid
- means 18 for processing the light intensity comprises means 18 capable of calculating the variation of the light intensity between two successive measurements as well as means 23 capable of extracting the average value of a plurality of said variations between two successive measurements of the light intensity.
- the variation in light intensity is calculated by comparing, via the means 18, the value of the electrical signal 17 previously digitized by the analog / digital conversion module 11 to the value previously acquired.
- the measurement of the variation of the light intensity between two successive measurements is then introduced into a low-pass digital filter characterized by its coefficients Fo and constituting suitable means 23 extracting the average value of the variations between two successive measurements of the light intensity.
- the control and information processing unit 6 then supplies the client system 8, via the interface module 7, with this average value which is representative of the bubble level in the liquid.
- This second preferred embodiment of the invention makes it possible to reactively indicate the quantity of bubbles present in the liquid. It thus offers a flexibility of use to the customer who can adjust or re-adjust the systems when he wishes, or even develop new alert strategies, for example by using pre-alert levels.
- a temperature probe is then used which can be short-circuited when the sensor has detected the presence of bubbles and / or when the sensor is not immersed in the liquid.
- thermoelectric measurement device makes it possible to obtain a tri-function sensor (liquid temperature / presence of gas bubbles in the liquid / absence of liquid) when capture techniques based on the transmission properties light in media with different optical characteristics is used.
- thermoelectric measurement device makes it possible to obtain a dual-function sensor (temperature of the liquid / presence of gas bubbles in the liquid) when capture techniques based on the properties of reflection of light on the surface of the gas bubbles are used. If, as we have seen previously, an electrode system is also incorporated, the third functionality (absence of liquid) is advantageously added to the device according to the invention.
- the interfacing with the client system 8 can advantageously be done, as illustrated by FIGS. 6 and 7, by using only one connecting wire on which the information relating to the liquid temperature, the presence of bubbles in the liquid and, according to certain configurations, the absence of liquid.
- FIG. 6 illustrates such an interface in the context of the first preferred embodiment of the invention.
- an alert signal is generated.
- This alert signal then controls the short-circuiting of the temperature sensor. So the output signal to the client system 8 is at a high level of amplitude proportional to the temperature of the liquid when the sensor is immersed in the liquid and no bubble is detected in the detection zone. Said signal takes a low level following the short circuiting of the probe when the sensor has detected the presence of bubbles or the absence of liquid.
- FIG. 7 illustrates the interfacing which can be carried out within the framework of the second preferred embodiment of the invention.
- Information on the bubble rate is sent at regular intervals in the form of a train of slots PWM (Puise Width Modulation, or in French Pulse Duration Modulation).
- PWM Pulise Width Modulation, or in French Pulse Duration Modulation
- the value of the voltage of the variable resistor forming the temperature measuring device is force periodically to the ground and supply voltages of the sensor.
- the width of the pulses is proportional to the bubble rate measured.
- An absence of liquid at the level of the sensor is considered as a maximum bubble rate and is therefore represented by a train of pulses of maximum width.
- the output signal to the client system 8 therefore consists of the periodic succession of a constant high level signal of amplitude proportional to the temperature of the liquid and a PWM signal representative of the rate of bubbles in the liquid.
- the invention applies in particular, but not exclusively, to the detection of gas bubbles in a cooling circuit of an internal combustion engine of a motor vehicle.
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Abstract
Description
Claims
Priority Applications (6)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| AU2003294079A AU2003294079A1 (en) | 2002-11-26 | 2003-11-25 | Optical detector for the presence of gas bubbles in a liquid |
| EP03789495A EP1565717A2 (fr) | 2002-11-26 | 2003-11-25 | Dispositif optique pour detecter la presence de bulles de gaz dans un liquide |
| US10/536,472 US7372063B2 (en) | 2002-11-26 | 2003-11-25 | Optical detector for the presence of gas bubbles in a liquid |
| BR0307926-0A BR0307926A (pt) | 2002-11-26 | 2003-11-25 | Detector por via óptica da presença de bolhas de gás dentro de um lìquido |
| JP2004556421A JP2006508356A (ja) | 2002-11-26 | 2003-11-25 | 液体内に存在する気泡を検出するための光検出器 |
| US12/105,938 US20080218746A1 (en) | 2002-11-26 | 2008-04-18 | Optical detector for the presence of gas bubbles in a liquid |
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| FR02/14805 | 2002-11-26 | ||
| FR0214805A FR2847670B1 (fr) | 2002-11-26 | 2002-11-26 | Detecteur par voie optique de la presence de bulles de gaz dans un liquide |
Related Child Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US12/105,938 Continuation US20080218746A1 (en) | 2002-11-26 | 2008-04-18 | Optical detector for the presence of gas bubbles in a liquid |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| WO2004051211A2 true WO2004051211A2 (fr) | 2004-06-17 |
| WO2004051211A3 WO2004051211A3 (fr) | 2005-06-09 |
Family
ID=32241613
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| PCT/FR2003/003480 Ceased WO2004051211A2 (fr) | 2002-11-26 | 2003-11-25 | Detecteur par voie optique de la presence de bulles de gaz dans un liquide |
Country Status (7)
| Country | Link |
|---|---|
| US (2) | US7372063B2 (fr) |
| EP (1) | EP1565717A2 (fr) |
| JP (1) | JP2006508356A (fr) |
| AU (1) | AU2003294079A1 (fr) |
| BR (1) | BR0307926A (fr) |
| FR (1) | FR2847670B1 (fr) |
| WO (1) | WO2004051211A2 (fr) |
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| WO2009061586A3 (fr) * | 2007-10-16 | 2009-10-15 | Zolo Technologies, Inc. | Sonde optique in situ et procédés |
| US8544279B2 (en) | 2005-11-04 | 2013-10-01 | Zolo Technologies, Inc. | Method and apparatus for spectroscopic measurements in the combustion zone of a gas turbine engine |
| CN106596623A (zh) * | 2017-01-16 | 2017-04-26 | 沧州航天科宇测试仪器有限公司 | 一种沥青软化点测定仪的自适应光电检测装置及其方法 |
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| JP4352874B2 (ja) * | 2002-12-10 | 2009-10-28 | 株式会社ニコン | 露光装置及びデバイス製造方法 |
| KR101354801B1 (ko) | 2004-08-03 | 2014-01-22 | 가부시키가이샤 니콘 | 노광 장치, 노광 방법 및 디바이스 제조 방법 |
| JP6196289B2 (ja) | 2012-04-19 | 2017-09-13 | ゾロ テクノロジーズ,インコーポレイティド | 方向可変の波長可変ダイオードレーザ吸収分光計を有する炉内再帰反射体 |
| KR101935366B1 (ko) | 2012-05-18 | 2019-01-04 | 삼성전자주식회사 | 미세 유체 소자 내의 유체를 감지 및 제어하는 장치 및 방법 |
| KR20140141879A (ko) * | 2013-05-31 | 2014-12-11 | 삼성전자주식회사 | 자동화된 핵산 분석 시스템 |
| JP2015021932A (ja) * | 2013-07-23 | 2015-02-02 | パイオニア株式会社 | 気泡検出器及び気泡検出方法 |
| US10072962B2 (en) * | 2016-07-05 | 2018-09-11 | Ecolab Usa Inc. | Liquid out-of-product alarm system and method |
| CN108896460A (zh) * | 2018-08-16 | 2018-11-27 | 钟祥博谦信息科技有限公司 | 气体检测系统、方法、设备及存储介质 |
| DE102019115603A1 (de) * | 2019-06-07 | 2020-12-10 | Endress+Hauser Conducta Gmbh+Co. Kg | Verfahren zur Korrektur eines durch einen optischen Sensor ermittelten Primärmesssignals |
| JP7475151B2 (ja) * | 2020-02-05 | 2024-04-26 | アズビル株式会社 | 測定装置、および測定方法 |
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| CN115575340B (zh) * | 2022-11-08 | 2023-03-10 | 杭州谱育科技发展有限公司 | 吸光度检测装置和方法 |
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| DE3880700D1 (de) * | 1987-02-04 | 1993-06-09 | Hoefliger Harro Verpackung | Verfahren und vorrichtung zum feststellen von fremdkoerpern in fluiden. |
| US4986659A (en) * | 1988-02-29 | 1991-01-22 | Aerometrics, Inc. | Method for measuring the size and velocity of spherical particles using the phase and intensity of scattered light |
| US4885676A (en) * | 1988-03-09 | 1989-12-05 | Storage Technology Corporation | Control loop instability detection and correction apparatus |
| JPH0390835A (ja) * | 1989-09-02 | 1991-04-16 | Murata Mach Ltd | 配管部品の漏れチェック装置 |
| US5331177A (en) * | 1993-04-26 | 1994-07-19 | Honeywell Inc. | Turbidity sensor with analog to digital conversion capability |
| US5508521A (en) * | 1994-12-05 | 1996-04-16 | Cardiovascular Diagnostics Inc. | Method and apparatus for detecting liquid presence on a reflecting surface using modulated light |
| US6315955B1 (en) * | 1995-04-06 | 2001-11-13 | Delaval International A.B. | Method and apparatus for quantitative particle determination in fluids |
| WO1998048867A1 (fr) * | 1997-04-29 | 1998-11-05 | Medtronic, Inc. | Detection et quantification optiques de bulles d'air microscopiques dans le sang |
| CA2292561A1 (fr) * | 1997-06-06 | 1998-12-10 | Texaco Development Corporation | Detection optique d'un gaz piege dans un systeme de refroidissement |
| DE19825518C2 (de) * | 1998-06-08 | 2001-10-04 | Fresenius Ag | Vorrichtung zur Messung von Parameteränderungen an lichtdurchlässigen Objekten |
| US6377341B1 (en) * | 1999-08-03 | 2002-04-23 | University Technology Corporation | Refractive index based detector system for liquid chromatography |
-
2002
- 2002-11-26 FR FR0214805A patent/FR2847670B1/fr not_active Expired - Fee Related
-
2003
- 2003-11-25 BR BR0307926-0A patent/BR0307926A/pt not_active IP Right Cessation
- 2003-11-25 JP JP2004556421A patent/JP2006508356A/ja active Pending
- 2003-11-25 AU AU2003294079A patent/AU2003294079A1/en not_active Abandoned
- 2003-11-25 US US10/536,472 patent/US7372063B2/en not_active Expired - Fee Related
- 2003-11-25 WO PCT/FR2003/003480 patent/WO2004051211A2/fr not_active Ceased
- 2003-11-25 EP EP03789495A patent/EP1565717A2/fr not_active Withdrawn
-
2008
- 2008-04-18 US US12/105,938 patent/US20080218746A1/en not_active Abandoned
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US8544279B2 (en) | 2005-11-04 | 2013-10-01 | Zolo Technologies, Inc. | Method and apparatus for spectroscopic measurements in the combustion zone of a gas turbine engine |
| WO2009061586A3 (fr) * | 2007-10-16 | 2009-10-15 | Zolo Technologies, Inc. | Sonde optique in situ et procédés |
| CN106596623A (zh) * | 2017-01-16 | 2017-04-26 | 沧州航天科宇测试仪器有限公司 | 一种沥青软化点测定仪的自适应光电检测装置及其方法 |
Also Published As
| Publication number | Publication date |
|---|---|
| FR2847670A1 (fr) | 2004-05-28 |
| US20080218746A1 (en) | 2008-09-11 |
| AU2003294079A1 (en) | 2004-06-23 |
| US20060061763A1 (en) | 2006-03-23 |
| WO2004051211A3 (fr) | 2005-06-09 |
| BR0307926A (pt) | 2005-08-23 |
| FR2847670B1 (fr) | 2005-06-10 |
| US7372063B2 (en) | 2008-05-13 |
| EP1565717A2 (fr) | 2005-08-24 |
| JP2006508356A (ja) | 2006-03-09 |
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