Variable gas volume flow measuring and control methods and apparatus

Abstract: Methods and apparatus are disclosed for measuring gas volume flow rate through a duct (23) including a variable area orifice (24), e.g. in an air conditioning system. Respective sensors (S1, S2) reference the total pressure upstream of the orifice (24) to the static pressure downstream, and a first signal representing the differential pressure is fed, with a second signal representing the open orifice area, to a control computer (31) which calculates the gas flow rate through the duct (23) on the basis of the signal values and information in a stored gas flow volume database. The database is constructed from values of the first and second signals generated at known volumes of air, preferably as a single, non-dimensional curve for all amplitudes of the differential pressure signal. The open orifice area may be controlled in dependence on conditions e.g. temperature, pollution, detected by a sensor (37) downstream of the orifice (24).

Description: The present invention relates to methods and apparatus for measuring the gas flow volume in a system of the kind in which the amount of gas flowing in a duct can vary in response to variation of the area of a variable orifice in the duct and/or in response to changes in the total pressure of the gas upstream of the orifice. The invention relates particularly to methods and apparatus for providing highly accurate measurements of gas flow at quite low gas flow volumes within the duct. The present invention has particular application as a control for the air flow in a duct of a variable air volume air conditioning system of the kind used in buildings. The invention may also have application to the measurement and to the control of gas flow for other gas flow volume systems. The present methods may, for example, be used to measure and to control the gas flow in an automotive system of the kind in which it is necessary to sense the level of a pollutant, e.g. the level of nitrogen oxide, in the exhaust gases of an internal combustion engine. Obtaining an accurate measurement of quite low air flow volume (and exerting effective control over such low air flows) can present a number of practical problems in variable air volume air conditioning systems for buildings. The overall variable air volume system for an entire building is quite large and often requires a relatively large number of control devices for measuring and for controlling the air flow to localized zones or areas, such as individual rooms or suites within the building. Because a typical system may require a large number of control devices, it is desirable that the control devices be of a class which is not too expensive. The control devices should, however, be capable of producing accurate, repeatable flow measurements at both high flow velocities (in the range of 20 m/s (4000 ft/min) in a typical 152 mm (six inch) diameter duct) and at low flow velocities (in the range of 2 m/s (400 ft/min) or less). The devices should also be capable of being easily installed in the field and should require little or no field calibration or recalibration after installation. Designing and manufacturing a control device which will meet all the requirements at high flow volumes is not too difficult. But it is difficult to manufacture a control device which is cost effective and which performs satisfactorily for accurate measurement and control of flow volumes at low flow rates (in the range of 400 feet per minute or less). Many of the existing measurement devices require an accurate sensing of the velocity pressure. The velocity pressure is a low number at low flow volumes. For example, in a conventional 152 mm (6 inch) diameter duct which produces one inch water column velocity pressure at 20 m/s (4000 ft/min) flow velocity within the duct, a flow velocity of 2 m/s (400 ft/min) produces a velocity pressure of only 0.01 inch water column. If the accuracy of the measuring device is 1 percent at the one inch water column corresponding to 20 m/s (4000 ft/min) (that is if the accuracy is plus or minus 0.01 inch water column at the high end) then the device can be off by factor of 100 percent (plus or minus 0.01 inch water column) at the 2 m/s (400 ft/min) flow velocity in the duct. There are many mechanical means to amplify, but such amplifier means are effective only at highest flow rates. The amplifiers present problems of measuring low flows. Specific prior art documents include the following: EP-A-61856 (Lucas), on which the two-part form of the present claims is based, describes measurement of air mass flow in an internal combustion engine duct having a movable throttle. Pressure drop is measured between static pressure transducers upstream and downstream of the throttle, and mass flow calculated using the pressure drop value and throttle position using a reference EPROM database. EP-A-237390 describes monitoring gas flow through a check device having an adjustable valve, by measuring pressures upstream and downstream of the valve and calculating the flow using a ratio of these together with the valve position and gas temperature. EP-A-166502 describes measuring gas flow using two fixed orifices in series, each with an upstream pressure sensor. JP-A-58/190718 describes monitoring exhaust gas flow using sensed dynamic pressure and temperature. EP-A-86259 describes measuring gas flow through a variable orifice, using the orifice size and a difference ΔP between upstream and downstream static pressures. EP-A-223300 describes microprocessor-controlled gas flow control through a multi-valve block, keeping constant the static pressure drop across the block. The general problem addressed herein is to provide new gas flow rate measuring methods and apparatus, enabling accurate measurement at low flow velocities. The solution according to the invention as defined in claims 1 and 6 involves referencing the total pressure upstream of the damper to the static pressure downstream of the damper so that the sensed pressure condition is a condition which is representative of the differential pressure between the total pressure upstream of the damper and the static pressure downstream of the damper and is a signal which generally has a high amplitude even at quite low gas flow velocities and volumes. By using this approach the invention enables a basic indication of the air flow within the duct to be obtained by sensing the damper position, the basic indication of the air flow then not being so dependent upon obtaining an accurate indication of the velocity pressure per se within the duct. A preferred object is to produce a manufactured product of consistent, predictable, reproducible geometry, using standard sensors, which can be calibrated at the factory by locating one point on a defined database, identified by using a single set of flow condition volumes generated at a known volume of air through the system. The present invention provides methods and apparatus for measuring gas flow volume, in a system of the kind in which the gas flow rate in a duct can vary in response to the variation of area of a variable area orifice in the duct formed by different damper positions and/or in response to changes of the total pressure of the gas upstream of the orifice and wherein the total pressure of the gas upstream of the orifice is referenced to the static pressure of the gas downstream of the orifice. The invention involves sensing the total pressure upstream of the orifice, sensing the static pressure downstream of the orifice, sensing a condition representative of the differential pressure between the total pressure upstream of the orifice and the static pressure downstream of the orifice, producing a first signal corresponding to said sensed condition representative of the differential pressure, producing a second signal corresponding to the area of the opening of the orifice represented by the damper position, supplying the first and second signals to a gas flow volume database which is correlated to the sensors and the orifice in the duct, and reading out from the database the gas flow volume occurring in the duct corresponding to those first and second signals. The invention also involves controlling the flow volume by positioning the damper to vary the area of the variable area orifice. This may include sensing a condition downstream of the damper and then controlling the gas flow volume in response to the sensed condition. In a preferred embodiment the database is constructed to have a single, non-dimensional curve for all amplitudes of the first and second signals. The invention may advantageously be applied in systems wherein the amount of gas flowing in the duct varies from quite low volumes of gas flowing at quite low velocities to quite large volumes of gas flowing at relatively high flow velocities, the components being such that the first signal producing means are effective to produce a first signal which is always a signal of relatively large amplitude, even at low gas flow volumes and velocities, so that highly accurate flow measurements can be obtained with sensors that do not need to be constructed for high accuracy at quite low amplitude levels of a sensed condition, such as low gas flow volumes and velocities. Features of the present invention will be apparent from the following description and claims and are illustrated in the accompanying drawings which, by way of example, show embodiments of the present invention and the principles thereof. In the drawings: Figure 1 is a side elevation view of apparatus constructed in accordance with one embodiment of the present invention for measuring and controlling gas flow volume in a system of the kind in which the amount of gas flowing in a duct can vary in response to the variation of area of a variable area orifice in the duct formed by different damper positions and/or in response to changes in the total pressure of the gas upstream of the orifice. Figures 2 through 7 are end elevation views illustrating how the area for flow of gas through the variable area orifice varies with movement of a control element (such as a movable blade damper, movable cage damper or a movable conical damper). Figure 2 shows the orifice completely closed and Figure 7 shows the orifice completely open. Figures 3-6 show a progressively increasing area of opening of the orifice as the damper moves from full closed to full open. Figure 8 is a table which correlates sensed pressures and sensed orifice area opening signals (obtained in accordance with the present invention) with the respective Figure 2 through Figure 7 showings. The chart of Figure 8 assumes the gas is air, that the density is 1.2 kg/m³ (0.075 lb/ft³), that the total pressure at S1 with reference to S2 is held at 25 mm (one inch) of water column, that the static pressure at S1 and S2 are equal in Figure 7, that the duct is the same size upstream and downstream of the orifice, and that S2 is not affected by Vena Contracta. The illustrations in Figures 2-7 and the data in Figure 8 are helpful to demonstrate a principle of the present invention, as will be described in more detail below in the specification. Figure 9 is a graphical plot of database information used to read gas flow volume occurring in the duct at specific combinations of a sensed differential pressure signal and a sensed orifice area opening signal (damper position signal). Figures 10, 11 and 12 are side elevation views showing details of different sensor constructions which can be used for sensing a condition which is representative of the differential pressure between the total pressure upstream of the orifice and the static pressure downstream of the orifice. Figures 13, 14 and 15 are plots of pressure losses along a duct when a blade damper is fully closed (Figure 13), partly open (Figure 14) and fully opened (Figure 15). In Figure 1 a gas flow volume measuring and control apparatus constructed in accordance with one embodiment of the present invention is indicated generally by the reference numeral 21. The apparatus 21 measures gas flow volume in a system of the kind in which the amount of gas flowing in a duct can vary in response to the variation of area of a variable area orifice in the duct and/or in response to changes in the total pressure of the gas upstream of the orifice. The total pressure upstream of the variable area orifice is referenced to the static pressure downstream of the orifice. The present invention, as will be described in more detail below, senses the total pressure upstream of the orifice, senses the static pressure downstream of the orifice, and senses a condition which is representative of the differential pressure between said total pressure upstream of the orifice and said static pressure downstream of the orifice. The present apparatus produces a first signal corresponding to the sensed condition representative of differential pressure, produces a second signal corresponding to the area of the opening in the orifice, and supplies the first and second signals to a gas flow volume database correlated to the sensors and the orifice in the duct. The system then reads out from the database the gas flow volume occurring in the duct at the sensed signals. The present apparatus also permits controlling the flow volume by varying the area of the variable area orifice. The control may be in response to a set point and a sensed condition. The sensed condition may, for example, be the pressure, temperature and/or humidity in a space or in the duct. By way of further example, the sensed condition may be the level of a pollutant, such as, for example nitrogen oxide in the exhaust gases of an internal combustion engine. As illustrated in Figure 1, the apparatus 21 comprises a duct 23. A blade type damper D-1 is mounted for pivoting action on a pivot shaft 25 so that the damper D-1 can move between a position (see Figure 2) in which the damper D-1 completely blocks gas flow through the duct 23 and a position (see Figure 7) in which the damper D-1 is wide open and offers minimum or no resistance to air flow through the duct. The position of the damper (the angle of rotation about the pivot 25) is controlled by a damper actuator 27 and a control line 29 from a computer/controller 31. The actuator 27 is connected to the damper D-1 through an articulated linkage 26-28. The air flows through the duct from left to right (as indicated by the legend "Air Flow" within the direction arrow shown in Figure 1). As illustrated in Figure 1, the angular position of the damper D-1 is transmitted to the computer/controller 31 by a signal line 33. The signal line 33 receives its input signal from a damper position sensor 34 associated with the pivot shaft 25 for sensing the angular position of the shaft 25 and thus the position of the damper D-1 and thus the area of the opening for the variable area orifice provided by the movable damper D-1. In a specific embodiment of the present invention the sensor 34 is a potentiometer. A potentiometer 34 of only moderate cost supplies a very accurate indication of the angle of the damper D-1. In another specific embodiment the sensor is a digital sensor which supplies a digital signal on the line 33. This embodiment is more expensive but produces a signal of very high accuracy. A stepper motor of high accuracy may be used. In accordance with the present invention a sensor DP-1 senses a condition which is representative of the differential pressure between the total pressure upstream of the variable area orifice and the static pressure downstream of the variable area orifice. A first sensor S1 senses the total pressure upstream of the orifice. A second sensor S2 senses the static pressure downstream of the orifice. The sensor DP-1 is connected to the probes S1 and S2 by conduits 36 and 38 as illustrated in Figure 1. The sensor DP-1 may have any of the constructions shown in Figs. 10-12, as described in more detail below. The sensor DP-1 produces the first signal (corresponding to the sensed condition which is representative of the differential pressure) noted above. This first signal is transmitted to the computer/controller 31 by a signal line 35. In the present invention a very accurate measurement of the gas flow volume in the duct 23 can be obtained by supplying the first signal on the line 35 and the second signal on the line 33 to a gas flow volume database which is correlated to the sensors and to the orifice in the duct. A very accurate measurement of the gas flow volume can be obtained, even at quite low gas flow volumes, because (1) the DP-1 sensor is always dealing with a large signal quantity (the total pressure involved) rather than with a small signal quantity (for example, a flow pressure signal) which can become very small at low gas flow volumes, and (2) a potentiometer 34 (as noted above) supplies a very accurate indication of the angle of the damper D-1. The gas flow volume, occurring in the duct at the sensed differential pressure and the orifice area opening, is then read out from the database. Figure 9 illustrates a database constructed in accordance with the present invention. The method of construction of the database will be described in more detail below. The database shown in Fig. 9 is used to read out a loss coefficient which is directly and readily converted to the gas flow volume occurring in the duct at the sensed signals, as will also be described in more detail below. To complete this initial summary of the structure and operation of the structure shown in Figure 1, the apparatus 21 of the present invention in most cases includes a condition sensor 37 which is connected to the computer/controller 31 by a line 39 so that the apparatus 21 can be used not only to measure the gas flow in the duct 23 but also to control the gas flow volume occurring in the duct. The condition sensor 37 is used to sense a condition (such as the pressure, temperature and/or humidity in a space or in the duct 23) downstream of the damper D-1. In other applications, the sensed condition may be a level of a pollutant, such as, for example, the level of nitrogen oxide in the exhaust gases of an internal combustion engine. The signal corresponding to the sensed condition is transmitted to the computer/controller 31 by the signal line 39. This signal is compared, in the computer 31, with a set point signal. The level of the set point signal can be varied manually or by programmed instructions. The difference between the sensed condition and the set point condition is then used by the computer to activate the damper actuator 27 to move the damper D-1 in the required direction to eliminate the difference between this condition and the set point condition or to bring the sensed condition within a certain range of the set point. With this introductory description and summary of the apparatus 21 shown in Figure 1, reference will now be made to Figures 2-8 to describe a principle of operation involved in the apparatus shown in Figure 1. For purposes of illustration the duct 23 in Figures 2-8 can be considered to be a 152 mm (6") duct of 0.018 m² (0.196 ft²) cross section, and a flow velocity of 20 m/s (4000 ft/min) through the duct produces 25 mm (one inch) of water column velocity pressure. A flow velocity of 2 m/s (400 ft/min) produces only 0.25 mm (0.01 inch) of water column velocity pressure. Multiplying 20 m/s (4,000 feet per minute) air flow velocity in the duct times the cross sectional area of the duct produces a flow volume of 0.37 m³/s (784 cubic feet per minute) going through the duct at 25 mm (1.0 inch) water column velocity pressure. The velocity pressure being referred to here is derived from the formula -- pressure total equals pressure static plus pressure velocity. The velocity pressure equals 25 mm (one inch) water column for the 20 m/s flow. To better understand the advantages of the measurement method and apparatus of the present invention, the following explanation is made, with reference to the assumptions specified above in relation to Fig. 8. The objective of this explanation of Figs. 2-8 is to demonstrate the simple principle of physics involved. Total pressure is the sum of static pressure and velocity pressure. In Figure 2 (which represents the damper D-1 in the closed position) the DP-1 sensor is measuring only a difference in static pressure across the damper D-1. In Figure 7 the DP-1 sensor is measuring all velocity pressure. In Figures 3-6 the DP-1 sensor is measuring a combination of static and velocity pressure or total pressure. The DP-1 sensor is a total pressure measuring device which measures the total pressure across the damper D-1. All that is needed to obtain a cubic feet per minute reading for the airflow within the duct is the DP-1 reading and a calibrated orifice (damper position), and the cubic feet per minute can be calculated. The definitions of total pressure as used above must be qualified. Normally total pressure is referenced to atmosphere. Here total pressure (S1) is referenced directly downstream of the orifice (the damper D-1) at S2. Although Figure 1 shows S2 as atmosphere, it is unlikely that would be the case in any real application. By referencing total pressure to S2, there is no need to be concerned about any downstream restrictions or variables (that is any restrictions or any variables downstream of the location of the S2 sensor). A major requirement for this system is a requirement to calibrate and to set up a database or lookup table for the computer/controller 31. The apparatus 21, in its production form, is a predictable device and once a data base is established requires a minimum of calibration for like geometry. To sum up some significant points with respect to the above explanation regarding Figs 2-8: the differential pressure S1 minus S2 is not affected by other pressure drops in the system; a calibrated database using a signal from the DP-1 sensor and a signal from the damper position sensor 34 can be constructed for convenient access by the computer/controller 31; the size of signal that the DP-1 sensor measures is total pressure reference to S2 and is a signal which has a large quantity (or high amplitude) even when the gas flow volume in the duct 23 is a quite low gas flow volume; and the DP-1 sensor is quite economical because the low end requirements are in 2.5 mm (0.1 inch) of water column instead of 0.25 mm (0.01 inch) of water column (the quantity required when using standard flow measurement methods). To elaborate on this last point, the DP-1 sensor is always dealing (even at low gas flow volumes) with a large signal quantity (the total pressure involved) rather than with a signal quantity (for example, a velocity pressure signal) which can become very small at low gas flow volumes. This permits the present invention to use less sensitive devices and still maintain a high degree of accuracy. This last point can perhaps be appreciated also by referring specifically to Figure 3. In the case of the very small opening of the orifice 24 shown in Figure 3, there is (as indicated in Figure 8) a small amount of air flow velocity within the duct 23 -- in this case 0.074 m³/s (156 ft³/min) [4 m/s (800 ft/min) flow velocity] as compared to 0.37 m³/s (784 ft³/min) [20 m/s (4000 ft/min) flow velocity] when the damper is completely open as shown in Figure 7. The apparatus 21 is thus producing a very low average cross sectional air velocity. Standard measurements as used in the industry would produce only a very low air velocity signal (1 mm (0.04") water column) in this condition, but the DP-1 sensor of the present invention still has a large signal quantity to measure (in this case 25 mm (1 inch) water column total pressure). This large amplitude signal enables the sensor DP-1 to produce a signal on the line 35 which has a very high degree of accuracy. As noted above, the practical application of the method and apparatus of the present invention requires that a database be constructed so that the computer/controller 31 can read out from the database the gas flow volume occurring in the duct at the sensed signals. In the construction of a database for air conditioning an air flow measurement chamber should be designed to comply with or be better than the specifications of AMCA Standard § 500-75, "Test Methods for Louvers, Dampers and Shutters", Air Movement and Control Association, Inc. adopted and revised 1974 (or a more current standard or applicable specifications). In applications other than air conditioning the air flow measurement chamber should be designed to comply with applicable specifications. The database is constructed by obtaining the data of the first and second signals as generated at known volumes of air. The database can be constructed in the form of lookup tables which would have separate curves corresponding to different respective quantities of the amplitude of the signal sensed by the DP-1 sensor. That is, the database could have one curve for a DP-1 signal of 13 mm (0.5 inch) of water column, a second curve for a DP-1 sensed signal of 25 mm (1.0 inches) of water column, a third signal for a DP-1 sensed signal of 38 mm (1.5 inches) of water column, etc.; and the flow rate within the duct could be determined by the point at which particular damper openings (for example, a 20 percent damper opening, a 40 percent damper opening, a 60 percent damper opening, etc.) sensed signal intersected each one of those curves. A database which comprises lookup tables of this kind can have some disadvantages. For example, there can be a loss of some accuracy, lookup tables of this kind can require a substantial amount of memory, and the amount of time needed to construct a database of this kind can be a significantly long period of time. A preferred way of constructing a database for use in the present invention is to construct a database which eliminates the need to store a large number of curves and which utilizes the principles of dimensional analysis to produce a single loss coefficient curve which accuractly reflects all amplitudes of signals sensed by the DP-1 sensor. This database is shown in Figure 9 and the method of constructing this database will now be described in more detail below. In obtaining the data for constructing the database curve shown in Figure 9, a number of test runs were made in which the total pressure is held at a constant amount and the damper was progressively moved between full open and full closed positions. That is, one run was made in which the pressure total was held at a constant 13 mm (half inch) total pressure and the damper was moved to different positions and appropriate measurements were made. Another run was made with the total pressure held constant at 25 mm (one inch) water column and the damper position varied, and another run was made at a constant 38 mm (1 1/2) inch water column total pressure as the damper position was moved from full open to full closed. It should be noted that in constructing a database using principles of dimensional analysis, it is not necessary to hold the total pressure at a constant level if enough points are obtained to produce an accurate curve. Once these test runs have been made for a particular damper configuration and a particular sensor configuration, then the data can be reduced to provide the data base information for that particular apparatus; and, as that particular apparatus comes through the factory on a production line, it is necessary only to calibrate that apparatus at one point; and that particular apparatus is then calibrated for all other points and does not need any field calibration. The database construction procedure used for producing the loss coefficient curve shown in Figure 9 produces a set of data specific to the damper design and geometry. For a specific damper design there is a unique calibration curve relating the air flow rate to the damper position for different DP-1 pressure difference signals, flow properties and duct diameters. To remove the large number of curves that would have to be stored in a computer (for a database in the form of a look up table which had a separate curve for each amplitude of sensed DP-1 signals), dimensional anaylsis was utilized. The dimensional parameters that could effect the sensed DP-1 sensor signal are the following: 1. the percent the damper was open, D; 2. the air flow rate, Q; 3. the upstream duct diameter, d; 4. the air density, Rho. According to the dimensional anlysis, the non-dimensional DP-1 pressure signal expressed as the loss coefficient C L should be a function of the percent damper opening, D and the flow Reynolds number Re. C L = f(D,Re) where C L = (DP-1 d⁴)/(Rho Q²) D = % damper open Re = (Rho Q d)/(Mu A d ) DP-1 = Signal sensed by DP-1 sensor d = Diameter of duct Rho = Air density in duct Mu = Viscosity Q = Volume airflow rate A d = Cross sectional area of the duct This analysis results in a family of curves of loss coefficient versus damper opening with the Reynolds number as a parameter. If the calibration is expressed in terms of these nondimensional parameters, than the number of calibration curves is reduced. The experiments showed that the Reynolds number was not an important parameter. Therefore, for each damper design, there was only one curve relating the loss coefficient to the damper opening. The curve resulting from the dimensional analysis can be approximated using a least squares fit. This fit is then written into a control algorithm used in computer/controller 31. In applying the present invention in the field a microprocessor of the computer/controller 31 uses the following algorithm: 1. Read the values of the differential pressure and the damper position sensors using an analog-to-digital sensor or an analog-to-digital converter (if required). 2. Determine the appropriate curve segment on the calibration curve for the damper position signal. 3. Substitute the damper position signal into the curve segment to obtain a loss coefficient. 4. Use the loss coefficient and the DP-1 pressure signal and solve for the airflow equation: Q = [(C L Rho)/(DP-1 d⁴)] 1/2 5. Return to the main control loop to determine the appropriate control decision based on this flow rate. This last step (step 5) assumes that the gas flow is to be controlled as well as to be measured. The single curve database thus constructed and shown in Figure 9 reduces the amount of memory required and also reduces the manipulation that has to be done of that memory data, as compared to the amount of memory required and the amount of manipulation that would be required for multicurve database. While the curve shown in Figure 1 is for a damper having a conical geometry, a similar, single, loss coefficient curve is produced for dampers having other kinds of geometries, as, for example, a blade type damper as shown in Figure 1, or a sash damper. The damper position sensor 34 does not have to be physically tied to the damper, but may instead sense the damper position by an indirect method such as, for example, an infra-red or an ultra-sonic device. It is a very important feature that the apparatus, including the variable orifice and the associated hardware, is a manufactured product of consistent, predictable reproducible geometry, using standard sensors, and is a product which can be calibrated at the factory by locating one point on the defined database, identified by using one orifice area opening signal, and one differential pressure signal generated at a known volume of air through the system. The apparatus 21 is then ready for use in the field without the need for additional calibration. Apparatus may be constructed which produces very accurate measurements with relatively low cost, rotational potentiometers and with low cost DP-1 pressure sensor constructions. Figures 10, 11 and 12 show three different constructions of DP-1 sensors which may be used in the present invention. In Figure 10 the DP-1 sensor is a sensor which has a diaphragm or piezoelectric element 41 directly exposed on opposite sides of the element 41 to the respective pressures within the conduits 36 and 38. Figure 11 shows a square edge orifice or a nozzle type sensor. In this case a square edge orifice or nozzle 43 is mounted within the flow passage way connecting the conduits 36 and 38. A conduit 45 transmits the pressure upstream of the orifice 43 to one side of the diaphragm or piezoelectric 41, and a conduit 47 conducts the pressure downstream of the orifice 43 to the other side of the element 41. In Figure 12 the sensor DP-1 is a hot wire anemometer type sensor. As illustrated in Figure 12, a hot wire anemometer 51 is disposed within a flow conduit interconnecting the conduits 36 and 38. A first heated wire 53 and a second heated wire 55 produce a signal corresponding to a condition representative of the differential pressure between the sensors S1 and S2. The airflow across the hot wire anemometer 51 cools the wire 53 more than it cools the wire 55, and this difference in the cooling causes the sensor DP-1 to produce a signal on line 35 which is an accurate indication of the total pressure across the damper. The sensor constructions shown in Figures 1-7 and 10-12 are known, commercially available sensor constructions. Other known constructions may be used. The invention resides in the way in which the sensors are used with the other features of the system to obtain a measurement of the gas flow volume in the duct. The present apparatus provides a system for making accurate measurements of gas flow volumes and is useful for obtaining accurate measurements at quite low gas volume flows. The apparatus described obtains these results while using manufactured products of consistent, predictable, reproducible geometry which can be calibrated at the factory, all as noted above. It is also possible for the flow not only to be measured but to be controlled in response to a sensed condition. As shown in Figure 1, a condition sensor 37 can be located downstream of the damper D-1 for sensing a particular condition related to the gas flowing through the duct 23. In the case of a conditioned air system, the sensed condition may be the temperature and/or humidity in a space or in the duct downstream of the damper D-1. In other applications the sensed condition may be the level of a pollutant, such as, for example, on the level of nitrogen oxide in the exhaust gases of an internal combustion engine. The signal corresponding to the sensed condition is transmitted to the computer controller 31 by the signal line 31. This signal is compared, in the computer 31, with a set point signal. The level of the set point can be varied manually or by programmed instructions. The difference between the sensed condition and the set point condition is then used by the computer to activate the damper actuator 27 to move the damper D-1 is the required direction to eliminate the difference between this condition and the set point condition or to bring the sensed condition within a certain range of the set point. Figures 13, 14 and 15 are plots of pressure losses along a duct when a blade damper is fully closed (Figure 13), partly open (Figure 14) and fully opened (Figure 15). These figures show graphically how the differential pressure DP-1 between the total pressure P T1 upstream of the damper and the static pressure P S2 downstream of the damper remains a large quantity for all positions of the damper and for all gas flow volumes and velocities including low gas flow volumes and velocities.

Claims: A method of measuring and controlling gas flow through a duct (23) having an orifice (24) of controllably variable area through which gas flows in the duct (23), under conditions in which the gas flow rate is subject to influence by variation in (a) area of the orifice (24), and/or (b) gas pressure upstream of the orifice (24), the method comprising sensing a condition representative of the differential pressure between pressures sensed upstream and downstream of the orifice (24), and producing a first signal indicative of the differential pressure; producing a second signal indicative of the area of the orifice (24), and supplying the first and second signals to control means (31) to calculate a gas flow rate from the values of the first and second signals using a predetermined gas flow database, characterised in that the differential pressure is determined between the total pressure sensed upstream of the orifice (24) and the static pressure sensed downstream of the orifice (24), the calculated gas flow rate is a volume flow rate, and in that the control means (31) controls the area of the orifice (24) in dependence on that flow rate. A method according to claim 1 wherein the database is predetermined using data for said first and second signals at known air volume flow rates. A method according to claim 2 wherein the database has a single, non-dimensional curve for all amplitudes of the first signal. A method according to any one of claims 1, 2 and 3 which comprises calibrating a system including said duct (23) and having an orifice (24) of a given geometry, sensors (S1, S2) of a particular geometry for producing the first signal and a sensor (34) of a given construction for producing the second signal, the calibrating including locating a point on the database using one first signal value and one second signal value generated at a known volume flow rate of air. A method according to any one of the preceding claims, further comprising sensing a condition downstream of the variable orifice (24) and adjusting the area of the orifice (24) in dependence on the sensed condition downstream thereof. Apparatus for measuring and controlling gas flow through a duct (23) having a variable area orifice (24) through which gas flows in the duct (23), and in which the gas flow rate can be influenced by varying (a) the area of the orifice (24), and/or (b) gas pressure upstream of the orifice (24), the apparatus comprising sensors (S1,S2) for measuring pressure upstream and downstream of the orifice (24); means (DP-1) for sensing a condition representative of the differential pressure between the upstream and downstream pressures sensed by said sensors (S1,S2) and for producing a first signal indicative of that differential pressure; means (34) for producing a second signal indicative of the area of the orifice (24), and control means (31) incorporating a gas flow database and adapted to calculate a gas flow rate in the duct (23) using said database and values of the first and second signals, characterised in that the upstream pressure (S1) is a total pressure sensor and the downstream pressure sensor (S2) is a static pressure sensor, and in that the gas flow database is a gas volume flow database and the control means (31) is adapted to calculate a gas volume flow rate, and to control the area of the variable area orifice (24) in dependence on that flow rate. Apparatus according to claim 6 in which the differential pressure sensing and first signal producing means (DP-1) comprises a diaphragm or piezoelectric element (41) exposed on one side to the upstream total pressure and on another side to the downstream static pressure. Apparatus according to claim 6 in which the differential pressure sensing and first signal producing means (DP-1) comprises a square edge orifice sensing device (43,45,47) exposed on one side to the upstream total pressure and on another side to the downstream static pressure. Apparatus according to claim 6 in which the differential pressure sensing and first signal producing means (DP-1) comprises a hot wire anemometer (51,53,55) exposed on one side to the upstream total pressure and on another side to the downstream static pressure. Apparatus according to claim 6 or claim 7, comprising a further sensor (37) for sensing a condition in the duct (23) downstream of the orifice (24), and control means for adjusting the area of the orifice (24) in dependence on the sensed downstream condition. Apparatus according to claim 8 wherein the further sensor (37) is adapted to sense temperature, or the level of a pollutant, in the gas flow downstream of the opening (24).

Inventors: GINN LEROY DRY, GINN LEROYCE SLOE, SCHNEIDER KAREN B, GINN, LEROY DRY, GINN, LEROYCE SLOE, SCHNEIDER, KAREN B.
Applicants: GINN LEROY D, GINN LEROYCE S, GINN, LEROY DRY, GINN, LEROYCE SLOE
Application year: 1988
Main classification: G01F1
IPC codes: G01F1, G05D7