WO1998000736A1 - Optical flow meter - Google Patents

Optical flow meter Download PDF

Info

Publication number
WO1998000736A1
WO1998000736A1 PCT/DK1997/000285 DK9700285W WO9800736A1 WO 1998000736 A1 WO1998000736 A1 WO 1998000736A1 DK 9700285 W DK9700285 W DK 9700285W WO 9800736 A1 WO9800736 A1 WO 9800736A1
Authority
WO
WIPO (PCT)
Prior art keywords
optical
drop
receiving means
calculation
optical receiving
Prior art date
Application number
PCT/DK1997/000285
Other languages
English (en)
French (fr)
Inventor
Jan Kikkenborg Larsen
Original Assignee
Alka Electronic Aps
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 Alka Electronic Aps filed Critical Alka Electronic Aps
Priority to AU32546/97A priority Critical patent/AU3254697A/en
Publication of WO1998000736A1 publication Critical patent/WO1998000736A1/en

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F3/00Measuring the volume flow of fluids or fluent solid material wherein the fluid passes through the meter in successive and more or less isolated quantities, the meter being driven by the flow
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01FMEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
    • G01F1/00Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow
    • G01F1/66Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by measuring frequency, phase shift or propagation time of electromagnetic or other waves, e.g. using ultrasonic flowmeters
    • G01F1/661Measuring the volume flow or mass flow of fluid or fluent solid material wherein the fluid passes through a meter in a continuous flow by measuring frequency, phase shift or propagation time of electromagnetic or other waves, e.g. using ultrasonic flowmeters using light
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01WMETEOROLOGY
    • G01W1/00Meteorology
    • G01W1/14Rainfall or precipitation gauges

Definitions

  • the invention According to the invention it is possible to obtain a reliable and reproducible measurement and minimal power consumption, as the convex shape of a drop focuses the light from the optical transmitter (s) , whereby the intensity of light at the optical receiver (s) is increased, when the light is transmitted through the drops .
  • the measure object e.g. each drop
  • the measure object works as a kind of optical amplifier, because of the reducing of the natural spreading of the light.
  • the increased intensity at the receiver provides a possibility to decrease the transmitter power at the transmitter, thus, reducing the necessary supply of power to the- optical transmitter or transmitters.
  • the method can advantageously be used in battery applications because of the fact, that the battery life time can be extended significantly. The method is therefore advantageous in transportable and relatively cheap hardware.
  • the method has important advantages over the use of various electrical short circuiting-electrodcs as well as the method according to the invention introduces no inaccuracy or bias in dependence of diverging conductivity of the water resulted by purity or pollution .
  • the invention also provides the possibility for a relatively simple electrical dimensioning of the necessary hardware. This is for example the fact when choosing the necessary voltage level of the optical system, as this level under usual conditions desirable should be as low as possible.
  • a further advantageous embodiment of the invention can be achieved when the optical signals emitted by the transmitter (s) forms a pulse train, as it is thus possible to reduce the overall power or current consumption even more, and at the same time achieve a satisfactory and applicable level of light intensity by the receiver or the receivers.
  • the duty cycle of the pulse train surprisingly can be significantly reduced, as the invention can be utilised at relatively low voltage levels and a low current-/power- consumption.
  • the duty cycle can be reduced to less than 1°, which in relation to battery applications provides a further significantly increasing of battery life time combined with a reproducible measurement.
  • the measuring unit converts the counts of detected drops to a measure of rain over a certain interval of time, which subsequently may be shown at a monitoring unit e.g. a display.
  • the measuring unit may export the count measurement to a memory unit, as the measurement is moreover connected to a time of registration. Conseguently the time of reading the unit becomes less critical, in the sense that all data can be collected and evaluated subsequently.
  • Another very important advantage of the invention is the fact that only a positive registration of a rain drop pulse is possible, as the physical properties of the drop is necessary to obtain a registration. An impurity, an insect or the like would thus not trig an impulse, as no focusing and increased intensity at the receiver is provided.
  • the invention is therefore particularly advantageous under conditions where there is a need for accurate measurements.
  • a control unit initiates a registration of a passing drop in the optical path(s) when the electrical signal exceeds a predetermined tnreshold value, a method of measuring with improved precision is obtained.
  • a further aspect of the invention is, that the improved precision is obtained at the same time as a significantly decreased energy consumption. 'J he decreased energy consumption s caused by the fact that the necessary supplied electrical power to the optical transmitting means can be reduced significantly, as the system in "idle-mode", i.e. no drop is detected, has no need for supplied energy causing a registration threshold value to be exceeded at the optical receiving means.
  • the invention generically takes advantage of the optical refraction properties of a drop.
  • a drop in the optical path between the optical transmitting means and receiving means will act as a kind of optical amplifier, increasing tne intensity of the received optical power at the optical receiving means causing the said threshold value to be exceeded.
  • the invention as such from a technical point of view does not amplify the light guided to the optical receiving means, but rather perform a focusing of a part of the spread light from the optical transmitting means, thus causing a reduction of the spreading of the light when seen from the optical receiving means.
  • the understanding of the term fluid output is that the water from there can be guided to a container or directly out of the measuring apparatus.
  • control unit increments a drop count register when the electrical signal exceeds a predetermined threshold value an advantageous embodiment of the invention is obtained, as each drop is registered completely on the front edge or the rear edge of the drop .
  • the optical signals emitted by the optical transmitting means are pulses, a particularly advantageous embodiment of the invention is obtained, as the electrical power consumption of the optical transmitting means can be further reduced.
  • the means for calculation is arranged to initialise a registration of a passed drop m the measuring zone, when the electrical signal or a corresponding digital representation from the optical receiving means, exceeds a threshold stored m the means for calculation, a rain gauge having an improved accuracy is obtained
  • the means for calculation increments a drop count register when the electrical signal or a corresponding digital representation from the optical receiving means exceeds a threshold value stored in the said means, an advantageous embodiment of the invention is obtained, which, in its generic form, is capable to register a drop on its front edge only without further detection and processing.
  • the optical transmitting means 2 is arranged to emit pulse formed optical signals, a particular advantageous embodiment of the invention is obtained, as it has shown that a periodic activation of the optical transmitting means at a suitable dimensioning of the electrical and optical system can be implemented .
  • the pulses can have different kinds of shapes within the scope of the invention. Moreover it should be noted that the necessary number of light pulses depends on the kind of application, as the number of pulses per time unit should be chosen so that it is ensured that no drops will be overlooked as a consequence that no pulse appeared when the drop passed the optical path between the optical transmitting and receiving means.
  • each pulse can likewise be adapted suitably from application to application.
  • the pulse can be maintained until the drop has passed the optical path, thus ensuring that the drop will be illuminated during the passage of the optical path.
  • it will be possible unambiguously to register the rear edge of the drop, when the front edge of the drop has been detected.
  • the frequency and duration of the pulses can be adjusted.
  • Another example of how a pulse can be "caught" in the drop counter can be effected when increasing the frequency of the pulses as a result of an exceeding of the threshold value. In some applications this way of operation can be advantageously if the rear edge of the drop has to be registered m a simple manner.
  • the optical transmitting means is arranged to emit optical pulse formed signals having a constant period and duty cycle, said duty cycle being a measure for the optical omission time related to the total period time, a particular simple and easily applicable method according to the invention has been obtained, as the timer interrupts etc. can be performed by means of relatively simple and clear routines.
  • the duty cycle of the pulse train approximately is 1° and the period time of the pulse is approximately 32 ms
  • a further advantageous embodiment according to the invention has been achieved, which, when considering the electrical and mechanical properties of an application, can obtain a very current consumption combined with a very accurate registration.
  • the ram gauge comprises a signal interface for transmission of data to an external unit connected to the means for calculation, said data being wholly or partly comprised of representations of the calculated drop flow or derived data thereof, a further advantageous embodiment according to the invention has been achieved, which can be applicable in e.g. measuring units of a more professional character, as the data in a certain measuring period, e.g. a week, can be transferred by a memory dump to an external calculation unit, e.g. a portable computer.
  • the above mentioned signal interface could for instance be a simple RS 232-mterface .
  • the means for calculation converts the number of registered drops to a measure for the precipitation which subsequently is displayed on a display unit, an advantageous and user friendly application has been achieved.
  • the distance between the optical transmitting means and the optical receiving means approximately is 10 mm at a drop size of approximately 5/100 ml
  • a further advantageous embodiment of the invention has been obtained, when dimensioned under consideration to the degree of the focusing provided by a drop at the optical receiving means.
  • this dimensioning moreover could be supplied with an adjustment of the means, which converts the rain into a drop flow of uniform drops.
  • This adjustment could e.g. be done by adjustment of the diameter of the drop nozzle.
  • the means for calculation is arranged to initialise a registration of a passed drop in the measuring zone, when the electrical signal or a corresponding digital representation from the optical receiving means exceeds a threshold stored in the means for calculation, a further advantageous embodiment of the invention has been obtained.
  • the invention in its generic form can thus be utilised for many different types of fluid flow, volume or mass measurements, when the fluid is sufficiently transparent to guide light through the drop when the drop is passing the optical path and thereby causing an increased intensity at the optical receiving means .
  • the counting technique can be utilised for automatically regulated dosing.
  • control unit increments a drop count register when the electrical signal exceeds a predetermined threshold value, an advantageous embodiment of the invention has been obtained, which m its most simple form is capable of registering a drop on the front edge without further detection's or calculations .
  • the optical signals emitted by the optical transmitting means are pulses, a particular advantageous embodiment of the invention has been obtained, as t has proved that a periodic activation of the optical transmitting means can be utilised without "overlooking” drops, when dimensioning the electrical an optical system suitably.
  • fig. 3 shows a more detailed timing chart of the trigger operation according the invention, and where
  • fig. 4 shows the electrical implementing of the optical system in an embodiment according to the invention.
  • the preferred embodiment Fig. 1 shows the principles of an embodiment according to the invention.
  • a drop collector 4 is arranged above an optical arrangement in such a way that a drop 1, when it is guided from the drop collector 4, is a part of the optical path between an optical transmitter 2 and an optical receiver 3 constituting the optical system in this example.
  • the drop collector 4 can be dimensioned mechanically in many different ways as long as the fluid flow is guided away from the drop collector shaped as drops.
  • the optical arrangement comprises in the considered example as a LED and a photo electrical receiver, or a usual optocoupler.
  • the distance between the LED and the receiver is in the considered embodiment approximately 10 mm.
  • Fig.l shows how a given amount of water is converted to a drop 1.
  • Fig. 2 shows the same arrangement, the drop 1 now released from the drop collector” and guided into the optical arrangement, hereby collecting or focusing the light from the LED by passage. This focusing increases the light intensity at the receiver 3, resulting in an exceeding over the threshold of the receiver 3. This results in an emitted pulse from the receiver 3 which will be registered and converted to an appropriate measuring unit, preferable mm or inches, in the measuring unit (not shown)
  • Fig. 3 shows another example of an introduced threshold value V ⁇ , which may be used for detection of a passing drop.
  • V is not exceeded when there is no drop, as the "idle" light intensity emitted from the optical emitter is not sufficient to exceed the threshold value V ⁇ .
  • the appearance of the drop causes the light intensity to be focused at the optical receiver in such a way, that it exceeds to a level above the threshold value.
  • Fig. 3 shows a timing chart for the overall system, when it is trigged by a down falling drop.
  • the periods A to F show the timing between the electrical signals, and the physical measurement of a drop collected by and guided away from a drop collector.
  • the simultaneous operation of transmitter LED showing when the light/the transmitting diode is turned on, SET, showing the registration history and being used for the drop counting when inverting the reference level, and IN, showing the level of the received light in the form of a corresponding electrical signal .
  • the period time is 32.35 ms and the time when LED is high is 0.35 s giving a duty cycle of approximately 1 ° 0 .
  • SET will be set high of the system, when LED is set high, and will be maintained high, if the drop has shaded the receiver (upper trigger threshold exceeded on IN) .
  • SET will be maintained high in the following measuring periods until the drop focuses enough light that IN reaches the low threshold voltage.
  • the electrical components coupled to IN may be dimensioned suitably such that the trigger or threshold on IN corresponds to the logical threshold value of the input gate.
  • an A/D gate may be suitably used.
  • the time of each measuring period should be chosen carefully in such a way that no drop would be overlooked. This dimensioning depends in technical respect of the physical properties of the drop flow and depends in economical respect of the best possible minimising of current consumption.
  • circuit shown at fig. 3 utilises a combined shading and focusing recognition, as a shade and a focusing in practice can be said to act in opposite phase in the shown example.
  • Software routines can likewise be supplemented with internal filters, as it e.g. can be advisable to use an extra count register, which implemented in software will secure that the system not registers a pulse the next five readings after registering of a drop or a drop-like pulse. This corresponds mechanically to a dimensioning of the system so that the drop collector and nozzle provides a maximum drop flow of approximately five per second.
  • An example of a further routine could be to add a requirement for two positive registrations on the same drop before it is accepted as a real drop and the drop count register is incremented.
  • Fig. 4 shows an example of how the optical system (the optocoupler) is wired and connected to a microprocessor.
  • a microprocessor 10 comprising an output 20, OUT SET, is electrically connected to a transmitter of an optocoupler 13 via a adapter resistor 15 and a grounded 17 capacitor 14. Moreover, the transmitter of the optocoupler is connected to ground 17.
  • the receiver of the optocoupler 13 is paralleled with a capacitor 12 to ground 17.
  • Two resistors 11 and 16 connects the parallel coupling to respectively an output 21, OUT SET, and an input 22, IN, on the microprocessor 10.
  • OUT SET 21 is subsequently high until the drop in the optocoupler 13 focuses the light so much, that the receiver of the optocoupler begins to conduct and the capacitor 12 is short circuited to ground 17. This procedure appears from the third period C of fig. 3.
  • the capacitor 12 may thus be dimensioned when bearing m mind, that the resistor the photo diode of the optocoupler within a period shall be able to pull the capacitor 1? low.
  • an increased quality of measurement and a low current consumption is achieved.
  • a battery life time of two years or more m a standard application when using a battery of 1.5V (900mAh), thus illustrating the advantages gained by using the drop flow itself to focus the light on the receiver, and thereby decreasing the necessary transmitting intensity.
  • the low current consumption is further decreased as the measuring time is
  • the structure of the shown activation of the LED has form of a pulse tra having a constant period and a constant duration of the activation. It should nevertheless be noted that the shape of activation is not crucial. It is therefore within the scope of the invention possible to change the period or the time duration of activation dynamically as a function of currently applicable criteria's, as e.g. the state of the system can form the basis of the mentioned changes. As an example the system could be adapted to transmit bursts of pulse trains, if no drop flow has been detected over a given period of t me and then return to a constant pulse tram at the first indication of a fluid flow.

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  • Physics & Mathematics (AREA)
  • Fluid Mechanics (AREA)
  • Environmental & Geological Engineering (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Atmospheric Sciences (AREA)
  • Biodiversity & Conservation Biology (AREA)
  • Ecology (AREA)
  • Environmental Sciences (AREA)
  • Hydrology & Water Resources (AREA)
  • Electromagnetism (AREA)
  • Measuring Volume Flow (AREA)
PCT/DK1997/000285 1996-07-02 1997-06-30 Optical flow meter WO1998000736A1 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
AU32546/97A AU3254697A (en) 1996-07-02 1997-06-30 Optical flow meter

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
DK72796A DK72796A (da) 1996-07-02 1996-07-02 Optisk væskeflowmeter
DK0727/96 1996-07-02

Publications (1)

Publication Number Publication Date
WO1998000736A1 true WO1998000736A1 (en) 1998-01-08

Family

ID=8096856

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/DK1997/000285 WO1998000736A1 (en) 1996-07-02 1997-06-30 Optical flow meter

Country Status (3)

Country Link
AU (1) AU3254697A (da)
DK (1) DK72796A (da)
WO (1) WO1998000736A1 (da)

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2003027719A1 (en) * 2001-09-24 2003-04-03 Vaisala Oyj Precipitation sensor and method for precipitation rate measurement
US6617079B1 (en) 2000-06-19 2003-09-09 Mykrolis Corporation Process and system for determining acceptibility of a fluid dispense
WO2005003819A1 (en) * 2003-07-01 2005-01-13 Vaisala Oyj Method and device for hydrometeor detection
CN102156306A (zh) * 2011-03-09 2011-08-17 华南农业大学 基于误码检测机制的红外光电式雨水检测方法及装置
JP2013094611A (ja) * 2011-11-07 2013-05-20 Seiko Epson Corp 液滴検出装置
JP2013102914A (ja) * 2011-11-14 2013-05-30 Seiko Epson Corp 液滴検出装置
RU2617033C1 (ru) * 2016-03-09 2017-04-19 Федеральное государственное бюджетное учреждение науки Институт мониторинга климатических и экологических систем Сибирского отделения Российской академии наук (ИМКЭС СО РАН) Способ калибровки оптического измерителя осадков

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2293718A1 (fr) * 1974-12-06 1976-07-02 Donnadieu Georges Perfectionnements aux appareils de mesures et de statistiques pluviometriques a detecteurs photoelectriques
GB2080555A (en) * 1980-07-09 1982-02-03 Illingworth Anthony John A device to measure the sizes and concentration of solid or liquid particles as they move through a fluid
US4314484A (en) * 1979-10-09 1982-02-09 University Of Utah Research Foundation Self-compensating optical drop count apparatus for measuring volumetric fluid flow
US4680977A (en) * 1985-03-06 1987-07-21 Ivac Corporation Optical flow sensor
US4720636A (en) * 1984-08-06 1988-01-19 Abbott Laboratories Drop detecting system which operates under different ambient light conditions
GB2204683A (en) * 1987-05-11 1988-11-16 Scientific Technology Precipitation gauge
DE3926228C2 (da) * 1988-08-11 1992-04-23 Fujitsu Ten Ltd., Kobe, Hyogo, Jp

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2293718A1 (fr) * 1974-12-06 1976-07-02 Donnadieu Georges Perfectionnements aux appareils de mesures et de statistiques pluviometriques a detecteurs photoelectriques
US4314484A (en) * 1979-10-09 1982-02-09 University Of Utah Research Foundation Self-compensating optical drop count apparatus for measuring volumetric fluid flow
GB2080555A (en) * 1980-07-09 1982-02-03 Illingworth Anthony John A device to measure the sizes and concentration of solid or liquid particles as they move through a fluid
US4720636A (en) * 1984-08-06 1988-01-19 Abbott Laboratories Drop detecting system which operates under different ambient light conditions
US4680977A (en) * 1985-03-06 1987-07-21 Ivac Corporation Optical flow sensor
GB2204683A (en) * 1987-05-11 1988-11-16 Scientific Technology Precipitation gauge
DE3926228C2 (da) * 1988-08-11 1992-04-23 Fujitsu Ten Ltd., Kobe, Hyogo, Jp

Cited By (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6617079B1 (en) 2000-06-19 2003-09-09 Mykrolis Corporation Process and system for determining acceptibility of a fluid dispense
WO2003027719A1 (en) * 2001-09-24 2003-04-03 Vaisala Oyj Precipitation sensor and method for precipitation rate measurement
WO2005003819A1 (en) * 2003-07-01 2005-01-13 Vaisala Oyj Method and device for hydrometeor detection
US7286935B2 (en) 2003-07-01 2007-10-23 Vaisala Oyj Method and device for hydrometeor detection
CN102156306A (zh) * 2011-03-09 2011-08-17 华南农业大学 基于误码检测机制的红外光电式雨水检测方法及装置
JP2013094611A (ja) * 2011-11-07 2013-05-20 Seiko Epson Corp 液滴検出装置
JP2013102914A (ja) * 2011-11-14 2013-05-30 Seiko Epson Corp 液滴検出装置
RU2617033C1 (ru) * 2016-03-09 2017-04-19 Федеральное государственное бюджетное учреждение науки Институт мониторинга климатических и экологических систем Сибирского отделения Российской академии наук (ИМКЭС СО РАН) Способ калибровки оптического измерителя осадков

Also Published As

Publication number Publication date
AU3254697A (en) 1998-01-21
DK72796A (da) 1998-01-03

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