WO1996004607A1 - Self-calibration of an ndir gas sensor - Google Patents
Self-calibration of an ndir gas sensor Download PDFInfo
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- WO1996004607A1 WO1996004607A1 PCT/US1994/008780 US9408780W WO9604607A1 WO 1996004607 A1 WO1996004607 A1 WO 1996004607A1 US 9408780 W US9408780 W US 9408780W WO 9604607 A1 WO9604607 A1 WO 9604607A1
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- Prior art keywords
- value
- cycle
- determining
- sensor
- drift
- Prior art date
Links
- 238000000034 method Methods 0.000 claims abstract description 22
- 238000012886 linear function Methods 0.000 claims 10
- 238000005070 sampling Methods 0.000 claims 2
- 230000007774 longterm Effects 0.000 abstract description 6
- 125000004122 cyclic group Chemical group 0.000 abstract 1
- CURLTUGMZLYLDI-UHFFFAOYSA-N Carbon dioxide Chemical compound O=C=O CURLTUGMZLYLDI-UHFFFAOYSA-N 0.000 description 40
- 229910002092 carbon dioxide Inorganic materials 0.000 description 20
- 239000001569 carbon dioxide Substances 0.000 description 20
- 238000005259 measurement Methods 0.000 description 8
- 230000015654 memory Effects 0.000 description 6
- 239000007789 gas Substances 0.000 description 5
- XLYOFNOQVPJJNP-UHFFFAOYSA-N water Chemical compound O XLYOFNOQVPJJNP-UHFFFAOYSA-N 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 230000002035 prolonged effect Effects 0.000 description 3
- 230000015556 catabolic process Effects 0.000 description 2
- 230000007423 decrease Effects 0.000 description 2
- 238000006731 degradation reaction Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- VNWKTOKETHGBQD-UHFFFAOYSA-N methane Chemical compound C VNWKTOKETHGBQD-UHFFFAOYSA-N 0.000 description 2
- 238000009423 ventilation Methods 0.000 description 2
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 238000004364 calculation method Methods 0.000 description 1
- 238000002485 combustion reaction Methods 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
- 239000000428 dust Substances 0.000 description 1
- 230000007613 environmental effect Effects 0.000 description 1
- 238000012544 monitoring process Methods 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 239000000779 smoke Substances 0.000 description 1
- 238000007619 statistical method Methods 0.000 description 1
- 239000000126 substance Substances 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
- G01N21/27—Colour; Spectral properties, i.e. comparison of effect of material on the light at two or more different wavelengths or wavelength bands using photo-electric detection ; circuits for computing concentration
- G01N21/274—Calibration, base line adjustment, drift correction
-
- 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
-
- 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
- G01N21/59—Transmissivity
- G01N21/61—Non-dispersive gas analysers
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2201/00—Features of devices classified in G01N21/00
- G01N2201/12—Circuits of general importance; Signal processing
- G01N2201/127—Calibration; base line adjustment; drift compensation
- G01N2201/12746—Calibration values determination
- G01N2201/12753—Calibration values determination and storage
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2201/00—Features of devices classified in G01N21/00
- G01N2201/12—Circuits of general importance; Signal processing
- G01N2201/127—Calibration; base line adjustment; drift compensation
- G01N2201/12746—Calibration values determination
- G01N2201/12784—Base line obtained from computation, histogram
Definitions
- the present invention is in the field of measuring instruments, and specifically relates to a method for correcting the measurements made by a nondispersive infrared (NDIR) gas sensor for the effects of long-term drift.
- NDIR nondispersive infrared
- the method will be illustrated by an actual example in which a carbon dioxide sensor is used to determine the concentration of carbon dioxide gas in a building.
- the application of the method to the detection of other gases by the use of NDIR gas sensors is straightforward.
- the present invention grew out of prolonged observation of the carbon dioxide level in an office building. It has been discovered that the carbon dioxide level decreases when the people leave the building and exhibits a prolonged quiescent period thereafter. During this quiescent period, the carbon dioxide level approximates that found outdoors, typically 500 parts per million in a city. As the people return to work in the morning, the carbon dioxide level rises again in a predictable manner.
- the self-calibration technique of the present invention is based on this daily cycle. First, the quiescent portion of the daily cycle is identified. The carbon dioxide level is measured at least once during the quiescent interval, and the measured values from successive days are stored. Each day a best-fitting straight line is determined by statistical methods. The slope of the straight line reflects the long-term drift rate.
- the best fitting straight line is extrapolated forward through the next day, and is used to compensate the values measured throughout the next day.
- Calculation of the best-fitting straight line is repeated each day on a moving basis.
- Figure 1 is a chart illustrating typical variations in carbon dioxide concentration in a building over a period of several days
- Figure 2 is a graph showing a trend in measurements taken during the quiescent portion of successive days
- Figure 3 is a block diagram showing a preferred embodiment of the present invention
- Figure 4 is a flow chart showing a sequence of operations executed by the apparatus of Figure 3 in a first preferred embodiment
- Figure 5 is a flow chart showing a sequence of operations executed by the apparatus of Figure 3 in a second preferred embodiment
- Figure 6 is a flow chart showing a sequence of operations executed by the apparatus of Figure 3 in a third preferred embodiment
- Figure 7 is a flow chart showing a sequence of operations executed by the apparatus of Figure 3 in a fourth preferred embodiment.
- Figure 8 is a flow chart showing a sequence of operations executed by the apparatus of Figure 3 in each of the preferred embodiments.
- Figure 1 shows how the measured concentration of carbon dioxide varies during the daytime in a building, in a typical situation.
- the carbon dioxide level increases, and reaches a peak at some time during the day.
- the carbon dioxide level decreases, and after working hours, the carbon dioxide concentration stabilizes at a relatively low level referred to herein as a quiescent value.
- the concentration of carbon dioxide is typically in the range of 300 to 500 parts per million.
- the effect illustrated in Figure 1 is based on actual data observed in a number of office and business buildings.
- Figure 2 shows the effect of sensor drift; the vertical scale is greatly magnified compared to Figure 1.
- the data points in Figure 2 are hypothetical readings taken by an imperfect drifting sensor during the quiescent interval on successive days. If the measuring instrument were drift-free, the data points would lie rather close to a horizontal line representing the average level of carbon dioxide during the quiescent intervals. Unfortunately, because of the drift present in a real sensor, the data points best fit a straight line having a small slope. This slope is the drift of the sensor; and in general, the drift may be upward or downward. It is the purpose of the present invention to compensate the sensor for this observed drift.
- Figure 3 shows the apparatus used in implementing a preferred embodiment of the present invention
- Figures 4 through 8 are flow charts showing successive operations performed by the apparatus of Figure 3.
- the senor 10 produces an output signal x(t) that is sampled periodically by the sample and hold circuit 12 that is enabled by the clock 14.
- the sample and hold circuit 12 captures a sample every half hour. Each captured sample, in turn, is converted to a digital form X(t s ) by the digitizer 16. These successive digitized data are fed to the computer 18.
- the computer 18 operates on the incoming X(tj) to compensate them for drift of the sensor 10, producing the corresponding drift-compensated x c (t).
- the drift-compensated variable x,.(t) is then applied to a threshold circuit 20. When the threshold is exceeded, an alarm signal is produced on the line 22, and that signal is applied to operate an alarm 24 in the preferred embodiment. In an alternative embodiment, the alarm signal on the line 22 may be used to start an electric fan motor.
- the memories 26 and 28 are associated with the computer 18. How the computer 18 goes about compensating for drift of the sensor is shown in the flow diagrams of Figures 4 through 8 in which it is assumed, for illustrative purposes, that the variable x(t) is sampled every half hour, i.e., 48 times per day.
- the drift-compensating action of the present invention would normally be kept in operation at all times, and therefore the drift that accumulates in any particular day is small relative to the range of values that defines the quiescent interval. Accordingly, the measured values (including the drift component) can reasonably be expected to fall, during part of each day, within the range of values X L to X H that defines the quiescent interval.
- the incoming digitized samples X(t ( ) are first tested to determine whether they lie within the range of values that characterize the quiescent interval, as indicated at box 30 in Figure 4.
- a number of the samples X(t;) that have been determined to lie within the range are stored briefly in the memory Mj 26. After a number of such samples have been stored, their average value is calculated at boxes 34 of Figure 4, and stored in the memory M 2 28, as the estimate, for that day, of the quiescent value (as shown in box 36 of Fig. 4). In an alternative embodiment, only one sample is taken and it is stored immediately in the memory M 2 28 as the estimate, for that day, of the quiescent value.
- variable being measured cannot become less than or greater than some known value. For example, oxygen is not likely to exceed 21%, by weight, of the air. Likewise, water vapor is not likely to exceed a relative humidity of 100%.
- the flow chart of Figure 5 is applicable to situations where a maximum or minimum is to be found each day.
- the value of a variable may be known at a particular hour of each day; for example, a starting value or an initial concentra ⁇ tion. In this case, drift of the NDIR sensor can be determined from successive daily measurements of the variable at the particular time, in accordance with the method of the present invention, as shown in Figure 6.
- the total amount of gas produced each day is a constant. For example, if a known quantity of methane is burned each day in a thermostat-controlled furnance, then the total amount of water vapor produced is necesssarily limited and determinable, even though the furnance is turned OFF and ON several times during the day. In this situation, the water vapor concentration measurements taken throughout the day would be totaled or averaged, as shown in Figure 7.
- the common thread that connects these examples is the idea that each day the NDIR sensor measurements are used to produce, through the computer 18, an estimate of a variable whose true value is known, at least approximately, by some other means.
- the estimates found from the sensor measurements each day are stored in the memory M 2 28 day by day until a selected maximum number H of the daily estimates have been stored. Thereafter, each time a new estimate is stored, the oldest one is discarded from the memory M 2 28.
- the maximum number H is chosen, based on well-known statistical theory, to yield a desired degree of accuracy in estimating the drift.
- the straight line that best fits the stored estimates is calculated and its slope is estimated, as indicated at box 38 of Fig. 8. Since the variable is presumed to have the same value each day at the time the sample is taken, the slope of the best-fitting straight line is ascribed to drift of the instrument. Using the slope thus estimated, the raw measurements taken throughout the day are corrected for the drift, as shown at boxes 40 and 42 of Fig. 8.
- the drift-corrected measurements that are the output of the computer 18 are applied to the threshold circuit 20, and if the threshold is exceeded, an alarm signal is generated that is used to produce an audible or visible alarm.
- the "alarm" signal is applied to enable the operation of a fan or blower.
- Sensors of all types can be compensated for drift by use of the described method, provided the sensed variable is known to return periodically to a particular value. Compensation for drift is most valuable in sensors that are required to operate for long periods of time without attention, such as fire detectors and environmental monitoring sensors.
Abstract
Some cyclic variables include within each cycle a value that can be determined extrinsically. In such case, the sensed value may differ from the known value by an amount that is a combination of long-term drift of the sensor and random measuring error. The drift component can be evaluated and eliminated by the following method. Once each cycle, for a number of cycles, the sensor measures the variable at a time when its value should equal the extrinsically-known value. The differences are plotted versus time, and a best-fitting straight line is determined (38), which indicates the drift. Throughout the next cycle as the variable is continuously sensed, the drift determined (40) from the best-fitting straight line is continuously applied (42) to correct the sensed value.
Description
INTERNATIONAL APPLICATION
UNDER THE
PATENTCOOPERATIONTREATY
FOR
SELF-CALIBRATION OF AN NDIR GAS SENSOR
DESCRIPTION Technical Field
The present invention is in the field of measuring instruments, and specifically relates to a method for correcting the measurements made by a nondispersive infrared (NDIR) gas sensor for the effects of long-term drift.
Background Art
Many kinds of sensors experience long-term drift. Depending on the sensor, this drift may result from various causes, including: gradual chemical changes; a slow build-up of foreign matter, such as might result from exposure to water vapor, smoke, dust, etc.; and, variations in the electrical power supply, including battery degradation over time.
The classic approach to this problem is to provide within the sensor a reference channel that specifically measures the degradation caused by the aforementioned factors. However, provision of this reference channel increases the cost and complexity of the sensor. The problem of uncompensated drift is especially serious in NDIR sensors in general and especially in carbon dioxide sensors that are used in fire detectors and in ventilation monitors, because these devices are expected to operate for long periods of time, perhaps even years, without attention. These uses require long-term stability to avert excessive false alarm rates and erratic ventilation. Fortunately, under some conditions that are not uncommon, the situation is not hopeless. Using the method and apparatus described below, a sensor can
be made to calibrate itself, and to compensate itself for long-term drift.
The method will be illustrated by an actual example in which a carbon dioxide sensor is used to determine the concentration of carbon dioxide gas in a building. The application of the method to the detection of other gases by the use of NDIR gas sensors is straightforward.
Disclosure of Invention
The lowest naturally-occurring concentration of carbon dioxide is found outdoors in rural areas; the concentration there is in the range of 300-500 parts per million. Inside an office building or a residence, the presence of combustion and of people contribute to the amount of carbon dioxide in the air, so that indoor levels are usually higher than 500 parts per million.
The present invention grew out of prolonged observation of the carbon dioxide level in an office building. It has been discovered that the carbon dioxide level decreases when the people leave the building and exhibits a prolonged quiescent period thereafter. During this quiescent period, the carbon dioxide level approximates that found outdoors, typically 500 parts per million in a city. As the people return to work in the morning, the carbon dioxide level rises again in a predictable manner. The self-calibration technique of the present invention is based on this daily cycle. First, the quiescent portion of the daily cycle is identified. The carbon dioxide level is measured at least once during the quiescent interval, and the measured values from successive days are stored. Each day a best-fitting straight line is determined by statistical methods. The slope of the straight line reflects the long-term drift rate.
The best fitting straight line is extrapolated forward through the next day, and is used to compensate the values measured throughout the next day.
Calculation of the best-fitting straight line is repeated each day on a moving basis.
Decisions involving the concentration of carbon dioxide are based on the compensated values determined by the above-described process.
A preferred example of the method will be described in detail below with
the aid of the accompanying drawings which are provided for purposes of illustration and explanation, and not by way of limitation.
Brief Description of the Drawings
Figure 1 is a chart illustrating typical variations in carbon dioxide concentration in a building over a period of several days;
Figure 2 is a graph showing a trend in measurements taken during the quiescent portion of successive days;
Figure 3 is a block diagram showing a preferred embodiment of the present invention; Figure 4 is a flow chart showing a sequence of operations executed by the apparatus of Figure 3 in a first preferred embodiment;
Figure 5 is a flow chart showing a sequence of operations executed by the apparatus of Figure 3 in a second preferred embodiment;
Figure 6 is a flow chart showing a sequence of operations executed by the apparatus of Figure 3 in a third preferred embodiment;
Figure 7 is a flow chart showing a sequence of operations executed by the apparatus of Figure 3 in a fourth preferred embodiment; and,
Figure 8 is a flow chart showing a sequence of operations executed by the apparatus of Figure 3 in each of the preferred embodiments.
Best Mode for Carrying Out the Invention
Figure 1 shows how the measured concentration of carbon dioxide varies during the daytime in a building, in a typical situation. Early in the morning, as the workers begin to arrive, the carbon dioxide level increases, and reaches a peak at some time during the day. Thereafter, as the workers leave the office building, the carbon dioxide level decreases, and after working hours, the carbon dioxide concentration stabilizes at a relatively low level referred to herein as a quiescent value. During the quiescent interval, the concentration of carbon dioxide is typically in the range of 300 to 500 parts per million. The effect illustrated in Figure 1 is based on actual data observed in a number of office and business buildings.
Figure 2 shows the effect of sensor drift; the vertical scale is greatly magnified compared to Figure 1. The data points in Figure 2 are hypothetical readings taken by an imperfect drifting sensor during the quiescent interval on successive days. If the measuring instrument were drift-free, the data points would lie rather close to a horizontal line representing the average level of carbon dioxide during the quiescent intervals. Unfortunately, because of the drift present in a real sensor, the data points best fit a straight line having a small slope. This slope is the drift of the sensor; and in general, the drift may be upward or downward. It is the purpose of the present invention to compensate the sensor for this observed drift.
Figure 3 shows the apparatus used in implementing a preferred embodiment of the present invention, and Figures 4 through 8 are flow charts showing successive operations performed by the apparatus of Figure 3.
A digital implementation is used in the preferred embodiment of Figure 3 because it is believed that that approach is the simplest; however, an analog implementation is used in an alternative embodiment.
In the preferred embodiment shown in Figure 3, the sensor 10 produces an output signal x(t) that is sampled periodically by the sample and hold circuit 12 that is enabled by the clock 14. In the preferred embodiment, the sample and hold circuit 12 captures a sample every half hour. Each captured sample, in turn, is converted to a digital form X(ts) by the digitizer 16. These successive digitized data are fed to the computer 18.
The computer 18 operates on the incoming X(tj) to compensate them for drift of the sensor 10, producing the corresponding drift-compensated xc(t). The drift-compensated variable x,.(t) is then applied to a threshold circuit 20. When the threshold is exceeded, an alarm signal is produced on the line 22, and that signal is applied to operate an alarm 24 in the preferred embodiment. In an alternative embodiment, the alarm signal on the line 22 may be used to start an electric fan motor. The memories 26 and 28 are associated with the computer 18. How the computer 18 goes about compensating for drift of the sensor is shown in the flow diagrams of Figures 4 through 8 in which it is assumed, for illustrative purposes, that the variable x(t) is sampled every half hour, i.e., 48 times
per day.
The drift-compensating action of the present invention would normally be kept in operation at all times, and therefore the drift that accumulates in any particular day is small relative to the range of values that defines the quiescent interval. Accordingly, the measured values (including the drift component) can reasonably be expected to fall, during part of each day, within the range of values XL to XH that defines the quiescent interval.
Thus, in the preferred embodiment, the incoming digitized samples X(t() are first tested to determine whether they lie within the range of values that characterize the quiescent interval, as indicated at box 30 in Figure 4.
In the preferred embodiment, a number of the samples X(t;) that have been determined to lie within the range are stored briefly in the memory Mj 26. After a number of such samples have been stored, their average value is calculated at boxes 34 of Figure 4, and stored in the memory M2 28, as the estimate, for that day, of the quiescent value (as shown in box 36 of Fig. 4). In an alternative embodiment, only one sample is taken and it is stored immediately in the memory M2 28 as the estimate, for that day, of the quiescent value.
The existence of a quiescent time and corresponding range of values for the carbon dioxide concentration in an office building has been verified experimentally. For variables other than carbon dioxide under a wide range of situations, a prolonged quiescent interval may not exist. Such situations are not intractable and NDIR sensors can be rendered self-calibrating in more situations than was previously thought possible.
In some situations, it may be known in advance that the variable being measured cannot become less than or greater than some known value. For example, oxygen is not likely to exceed 21%, by weight, of the air. Likewise, water vapor is not likely to exceed a relative humidity of 100%. The flow chart of Figure 5 is applicable to situations where a maximum or minimum is to be found each day. In still other situations, the value of a variable may be known at a particular hour of each day; for example, a starting value or an initial concentra¬ tion. In this case, drift of the NDIR sensor can be determined from successive
daily measurements of the variable at the particular time, in accordance with the method of the present invention, as shown in Figure 6.
In yet other situations it may be clear from physical considerations that the total amount of gas produced each day is a constant. For example, if a known quantity of methane is burned each day in a thermostat-controlled furnance, then the total amount of water vapor produced is necesssarily limited and determinable, even though the furnance is turned OFF and ON several times during the day. In this situation, the water vapor concentration measurements taken throughout the day would be totaled or averaged, as shown in Figure 7. The common thread that connects these examples is the idea that each day the NDIR sensor measurements are used to produce, through the computer 18, an estimate of a variable whose true value is known, at least approximately, by some other means.
The estimates found from the sensor measurements each day are stored in the memory M228 day by day until a selected maximum number H of the daily estimates have been stored. Thereafter, each time a new estimate is stored, the oldest one is discarded from the memory M2 28. The maximum number H is chosen, based on well-known statistical theory, to yield a desired degree of accuracy in estimating the drift. At the beginning of each day, starting with the third day, the straight line that best fits the stored estimates, is calculated and its slope is estimated, as indicated at box 38 of Fig. 8. Since the variable is presumed to have the same value each day at the time the sample is taken, the slope of the best-fitting straight line is ascribed to drift of the instrument. Using the slope thus estimated, the raw measurements taken throughout the day are corrected for the drift, as shown at boxes 40 and 42 of Fig. 8.
The drift-corrected measurements that are the output of the computer 18 are applied to the threshold circuit 20, and if the threshold is exceeded, an alarm signal is generated that is used to produce an audible or visible alarm. In another embodiment the "alarm" signal is applied to enable the operation of a fan or blower.
Thus, there has been described apparatus and a method for autonomous
self-calibration of a sensor so as to increase its stability over time by correcting the raw output x(t) of the sensor to compensate for drift of the sensor. The technique is predicated on the daily or cyclical recurrence of a known value of the variable being sensed. The foregoing detailed description is illustrative of several embodiments of the invention, and it is to be understood that additional embodiments thereof will be obvious to those skilled in the art. The embodiments described herein together with those additional embodiments are considered to be within the scope of the invention.
Industrial Applicability
Sensors of all types can be compensated for drift by use of the described method, provided the sensed variable is known to return periodically to a particular value. Compensation for drift is most valuable in sensors that are required to operate for long periods of time without attention, such as fire detectors and environmental monitoring sensors.
Claims
1. A method for drift compensation of a sensor used for measuring a cyclical variable X that is known to lie within a known range extending from a low value XL to a high value XH during a part of each cycle, said sensor producing an electrical signal x(t) representative of the instantaneous value of X at time t, said method characterized by the steps of: a) determining when x(t) is between xL and xH where xL and xH denote the values of x(t) corresponding to XL and XH respectively; b) sampling x(t) during each cycle when x(t) is between xL and xH and storing a representative quiescent value of x(t) for each cycle; c) determining a linear function E(t) that best fits the representative quiescent values of x(t) that were stored in a number of successive cycles; d) extrapolating the linear function E(t) to the present time to, thereby obtaining E(to) ; and, e) determining a corrected value xc(t0) for the signal x(t) at the present time to which is compensated for sensor drift.
2. A method for drift compensation of a sensor used for measuring a cyclical variable X that is known to attain a constant maximum value XMAX during each cycle, said sensor producing an electrical signal x(t) representative of the instantaneous value of X at time t, said method characterized by the steps of: a) determining for each cycle the maximum value x AX corresponding
b) storing the maximum values determined in successive cycles; c) determining a linear function E(t) that best fits the maximum values stored in a number of successive cycles; d) extrapolating the linear function E(t) to the present time to, thereby obtaining E(to); and, e) determining a corrected value x-(to) for the signal x(t) at the present time t0 which is compensated for sensor drift.
3. A method for drift compensation of a sensor used for measuring a cyclical variable X that is known to attain a constant minimum value XMιN during each cycle, said sensor producing an electrical signal x(t) representative of the instantaneous value of X at time t, said method characterized by the steps of: a) determining for each cycle the minimum value XMIN corresponding
b) storing the minimum values determined in successive cycles; c) determining a linear function E(t) that best fits the minimum values stored in a number of successive cycles; d) extrapolating the linear function E(t) to the present time to, thereby obtaining E(to); and, e) determining a corrected value Xc(to) for the signal x(t) at the present time t0 which is compensated for sensor drift.
4. A method for drift compensation of a sensor used for measuring a cyclical variable X that is known to attain a known particular value Xκ at some known phase of each cycle, said sensor producing an electrical signal x(t) representative of the instantaneous value of X at time t, said method characterized by the steps of: a) sampling the value of x(t) once in each cycle at said known phase of each cycle; b) storing the values sampled in successive cycles; c) determining a linear function E(t) that best fits the values stored in a number of successive cycles; d) extrapolating the linear function E(t) to the present time t0, thereby obtaining E(to); and, e) determining a corrected value xc(t0) for the signal x(t) at the present time to which is compensated for sensor drift.
5. A method for drift compensation of a sensor used for measuring a cyclical variable X that is known to have the same known average value X for each cycle, said sensor producing an electrical signal x(t) representative of the instantaneous value of X at time t, said method characterized by the steps of: a) determining the average value x of x for each cycle; b) storing the average values determined in step a) for each cycle; c) determining a linear function E(t) that best fits the average values stored in a number of successive cycles; d) extrapolating the linear function E(t) to the present time to, thereby obtaining E(to); and, e) determining a corrected value x,.(t0) for the signal x(t) at the present time to which is compensated for sensor drift.
Priority Applications (7)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US07/762,396 US5347474A (en) | 1991-09-19 | 1991-09-19 | Self-calibration of an NDIR gas sensor |
DK94925177T DK0738405T3 (en) | 1994-08-02 | 1994-08-02 | Self-calibrating NDIR gas sensor |
DE69435188T DE69435188D1 (en) | 1994-08-02 | 1994-08-02 | AUTO CALIBRATION OF AN NDIR GAS SENSOR |
PCT/US1994/008780 WO1996004607A1 (en) | 1991-09-19 | 1994-08-02 | Self-calibration of an ndir gas sensor |
AT94925177T ATE423305T1 (en) | 1994-08-02 | 1994-08-02 | AUTO CALIBRATION OF A NDIR GAS SENSOR |
EP94925177A EP0738405B1 (en) | 1994-08-02 | 1994-08-02 | Self-calibration of a ndir gas sensor |
AU75196/94A AU7519694A (en) | 1991-09-19 | 1994-08-02 | Self-calibration of an ndir gas sensor |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US07/762,396 US5347474A (en) | 1991-09-19 | 1991-09-19 | Self-calibration of an NDIR gas sensor |
PCT/US1994/008780 WO1996004607A1 (en) | 1991-09-19 | 1994-08-02 | Self-calibration of an ndir gas sensor |
Publications (1)
Publication Number | Publication Date |
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WO1996004607A1 true WO1996004607A1 (en) | 1996-02-15 |
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Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
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PCT/US1994/008780 WO1996004607A1 (en) | 1991-09-19 | 1994-08-02 | Self-calibration of an ndir gas sensor |
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WO (1) | WO1996004607A1 (en) |
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EP1350116A1 (en) * | 2000-12-29 | 2003-10-08 | Edwards Systems Technology, Incorporated | Method of compensating for drift in gas sensing equipment |
WO2011101525A1 (en) * | 2010-02-19 | 2011-08-25 | Vaisala Oyj | Method for calibration of a co2 concentration sensor and a measuring device |
DE10255698B4 (en) * | 2002-11-29 | 2021-06-24 | Abb Ag | Method for operating a flow measuring device |
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EP1350116A1 (en) * | 2000-12-29 | 2003-10-08 | Edwards Systems Technology, Incorporated | Method of compensating for drift in gas sensing equipment |
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DE10255698B4 (en) * | 2002-11-29 | 2021-06-24 | Abb Ag | Method for operating a flow measuring device |
WO2011101525A1 (en) * | 2010-02-19 | 2011-08-25 | Vaisala Oyj | Method for calibration of a co2 concentration sensor and a measuring device |
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