LIQUID QUANTITY MEASUREMENT

Abstract: Apparatus for the ratiometric measurement of a quantity of liquid in a tank includes first and second capacitors (6,8) disposed in a tank and responsive to an AC excitation signal (2). The output signal from the first capacitor (6) corresponds to the quantity of liquid in the tank, while the output signal of the second capacitor (8) corresponds to an empty tank condition. First and second rectifier units (D1,D2; and D3,D4) are respectively coupled to the first and second capacitors (6,8). A first current-to-voltage converter (14) is coupled to both the first and second rectifier units (D1,D2; and D3,D4) and provides a first voltage signal corresponding to the first and second rectified signals. A second current-to-voltage converter (18) is coupled to the second rectifier unit (D3 and D4) and provides a second voltage signal corresponding to the second rectified signal. A ratio device (20) is coupled to the outputs of both voltage-to-converter means (14 and 18) and forms a ratio of the first and second voltage signals to provide an output signal indicative of the quantity of liquid in the tank. This output signal is insensitive to diode characteristics and variations in the excitation voltage and frequency, and produces a true zero output when the sensed quantity of liquid in a tank is zero.

Description: The invention relates to apparatus for measuring the quantity of a liquid in a tank, comprising: first capacitance means in the tank and positioned to be variably immersed by the liquid according to the amount of liquid in the tank, and having a first capacitance value which has a minimum value when the proportion of the effective height dimension of the capacitance means immersed by the liquid is a minimum proportion and which varies above this minimum value in dependence on the variation of the said proportion above the minimum proportion; second capacitance means in the tank and having a predetermined second capacitance value which is a reference value; an excitation source connected to energise the first and second capacitance means with an AC excitation signal whereby the first capacitance means produces a first measurement signal dependent on the first capacitance value and the second capacitance means produces a second measurement signal dependent on the second capacitance value; a first pair of oppositely poled diodes connected to receive in parallel the first measurement signal and to split it into two oppositely flowing currents; a second pair of oppositely poled diodes connected to receive in parallel the second measurement signal and to split it into two oppositely flowing currents; and current to voltage converting means connected to respond to the currents and to produce therefrom an indication of the quantity of liquid in the tank. Such apparatus is known from US-A-4 259 865. In this apparatus, the signal produced by the second capacitance means is used to control the excitation signal, while the signal produced by the first capacitive means is used to produce the liquid quantity indicating signal. The aim is to render the liquid quantity indicating signal independent of variations in the excitation signal and of other variations. The invention provides an arrangement in which the liquid level indicating signal is produced as a ratio of signals respectively produced by the two capacitance means, thus avoiding the need for control or adjustment of the excitation signal. Accordingly, such apparatus is characterised in that the second capacitance value is a predetermined value equal to the value of the first capacitance means under empty tank conditions; and the current to voltage converting means comprises (a) a first current to voltage converter connected to respond to the algebraic sum of one of the currents produced by the first diode pair and the oppositely flowing one of the currents produced by the second diode pair whereby to produce a first voltage output which is dependent on the magnitude of the excitation signal and on the amount by which the first capacitance value exceeds the minimum value thereof; and (b) a second current to voltage converter connected to respond to the other current produced by the second diode pair whereby to produce a second voltage output dependent on the magnitude of the excitation signal and on the second capacitance value; such that the ratio of the first and second voltage outputs provides a liquid quantity indicating signal indicative of the quantity of liquid in the tank and independent of variations in the excitation signal. Liquid quantity measuring apparatus embodying the invention will now be described by way of example only, with reference to the accompanying drawing, the single Figure of which is a schematic circuit diagram of the apparatus. The apparatus uses DC fuel tank measuring units and provides the benefits of immunity to variations in excitation voltage and frequency, insensitivity to temperature variations and DC diode characteristics even at low excitation voltages, and provides a true zero output when no fuel is sensed in the tank. In brief, the apparatus consists of a tank measuring unit including a first, variable, capacitor and a second, fixed capacitor. The first capacitor has a capacitance value which varies in accordance with the quantity of fuel in the tanks. The second capacitor has a fixed capacitance value which is predetermined in accordance with an empty tank condition. Both capacitors are driven by an AC generator. A diode pair is coupled to each capacitor with the diodes of each pair being of opposite polarity. The capacitance of the fixed capacitor is predetermined to be equal to the empty capacitance of the tank unit. This may be accomplished at the factory by connecting each diode coupled to the variable capacitor to the oppositely poled one of the diodes coupled to the fixed capacitor. The fixed capacitor is then adjusted (by selection, trimmer, etc.) until the total current from the assembly is zero when excited by a sine wave at, for example, 6 KHz. The factory calibrated probe assembly is then installed into a fuel tank using three wires and two DC amplifiers. The "positive" diode of the variable capacitor (i.e. the diode whose anode is connected to that capacitor) and the "negative diode" of the fixed capacitor (i.e. the diode whose cathode is connected to that capacitor) are connected to one DC amplifier. The negative diode of the variable capacitor is connected to the DC amplifier ground reference. The positive diode of the fixed capacitor is coupled to the second DC amplifier. Naturally, all diodes may be reversed to change polarity of the signal, if desired. The ratio of the outputs of the two DC amplifiers is now proportional to the added capacitance of the tank unit and accurately provides an output of the fluid volume within the tank. Since the signal is a ratio, it is independent of the excitation voltage and frequency and independent of diode thermal effects. Since diode characteristics no longer adversely effect the output, a much lower excitation voltage may be used. The Figure depicts the apparatus. Signal generator 2 provides an AC, sine wave signal at a predetermined frequency. For example, a 6 KHz signal may be used. Signal generator 2 may be a sine wave oscillator or any other known or convenient means for generating the sine wave excitation voltage. Within the tank unit assembly (T/U assembly) 4, is disposed a variable capacitor 6 having a capacitance value C T . Also disposed within T/U assembly 4 is fixed capacitor 8 which has a capacitance value of C F . One plate of each of capacitors 6 and 8 is provided with the excitation voltage from signal generator 2. The second plate of capacitor 6 is coupled to first rectifying means D1,D2, while the second plate of capacitor 8 is coupled to second rectifying means D3,D4. In general, the current through a capacitive sensor excited by a sine wave of angular frequency w is as follows: I = EwC (1) where E is the peak voltage of the excitation source, and C is the capacitance of the sensor. If a diode is inserted in series with this current, only positive or negative half cycles of the current will flow dependent upon the orientation of the diode. A positive and a negative diode are used in a pair to preserve AC current flow through the capacitive sensor. However, the diodes are used to steer positive current pulses to one return point, and the negative current pulses to another (or the same) return point. If the current out of one diode is returned to the summing node of an operational amplifier with low pass filter characteristics and a feedback resistor of value R, then only the DC component of the current remains and the rectified output voltage will be DC and as follows: V DC = E wCR/pi (2) The above-stated relationships are well known by those versed in the art. In general, the concept and advantages of a capacitive sensor with diodes is well-known. The benefits include simple signal conditioning and the elimination of a shielded cable for the output signal. However, such known systems are still sensitive to the value of the excitation voltages and to changes in the diode characteristics, and produce an output even when the sensed quantity of fuel is zero. The apparatus therefore uses the steering ability of the diodes to produce a capacitive sensor system which is insensitive to diode characteristics, excitation voltage and frequency, and which produces a true zero output when the sensed quantity is zero. The capacitance value of capacitor 6 may be quantified as follows: C T = alpha(K-1)C at +C et (3) where: alpha is the height of the sensed dielectric material (e.g., the fuel), K is the dielectric constant of the material (e.g., the fuel dielectric constant), C at is the active capacitance of the sensor and is a constant, and C et is the sensor capacitance in air which is also a constant. As described above, when the sensor assembly is built, diodes D1 and D4 are tied together and diodes D2 and D3 are also tied together. The sensor is then excited by a sine wave source and the capacitance value of capacitor 8 is adjusted such that the total output current of each diode pair is zero. Therefore, the following relationship holds: C F = C et (4) The output current from the capacitor 6 through diode D1 is as follows: DC current D1 = EwC T /pi (5) Likewise, the DC current from capacitor 8 through diode D4 is as follows: DC current D4 = EwC F /pi (6) The output currents through diodes D1 and D4 are summed at node 10 and directed to the summing junction 12 of operational amplifier 14. The output of operational amplifier 14 is a voltage signal E1. Since the inverting input of operational amplifier 14 receives DC current from both diodes D1 and D4, the output voltage E1 of operational amplifier 14 may be calculated as follows: E₁ = (C T - C F )(EwR1)/pi (7) where R1 = the resistance value of resistor R1 in the feedback path of operational amplifier 14. Since C F - C et (see equation (4)), and since equation (3) may be restated as follows: C et = C T - alpha (K-1)C at (8) then, the output voltage E₁ of operational amplifier 14 may be stated as follows: E₁ = alpha (K-1)C at (EwR1)/pi (9) In a like manner, the DC current through diode D3 may be stated as follows: DC current D₃ - EwC F /pi (10) Since C F - C et (see equation (4)), DC current through diode D3 may be stated as follows: DC current D3 = EwC et /pi (11) The DC current from diode D3 is provided to the summing node 16 of operational amplifier 18. Thus, the inverting input of operational amplifier 18 receives the DC current from diode D3. Operational amplifier 18 includes a feedback path having a resistor R2 of resistance value R2. The non-inverting input of operational amplifier 18 is coupled to ground. Thus, the output of operational amplifier 18 is a voltage signal E₂. This voltage signal E₂ may be calculated as follows: E₂ = EwC et R2/pi (12) Thus, equations (9) and (12) provide output voltage signals reflecting the level of quantity of fuel in the tank and a fixed capacitance predetermined base on an empty tank. By forming a ratio of the voltage signals from each operational amplifier, the disadvantageous effects of diode characteristics and excitation voltage variations may be eliminated. The ratio of the first voltage signal E₁ to the second voltage signal E₂ may be calculated as follows: Since C et and C at are known constants, and if R1 and R2 are a known ratio (ratio-matched resistors are well known), then the resulting value is independent of excitation voltage E, excitation frequency w, and diode variations (which appear as excitation voltage changes), and produces an output of zero when the measured parameter is in fact zero. In fact, if R1 and R2 are selected to be accurate and stable resistors, then the ratio output signal is only dependent on the desired measured parameter which is the product alpha(K-1). Needless to say, it is ratio device 20 which performs the necessary ratio calculations and provides the appropriate output signal. Since both sets of diodes are in the same thermal environment, diode effects are also cancelled in the ratio signal. Since the diode characteristics no longer affect the output, much lower excitation voltages may be used without compromising system accuracy. Thus, what has been described is a simplified, streamlined structure for providing a very accurate output signal indicative of the level of fuel within a tank. The output signal is immune to variations in excitation voltage and frequency and, diode characteristics, and produces a true zero output signal when no fuel is in the tank. Ratio device 20, may, for example, be a display unit, a microprocessor, or any known and convenient device for performing the ratio operations and providing the appropriate output signal.

Claims: Apparatus for measuring the quantity of a liquid in a tank, comprising: first capacitance means (6) in the tank and positioned to be variably immersed by the liquid according to the amount of liquid in the tank, and having a first capacitance value which has a minimum value when the proportion of the effective height dimension of the capacitance means (6) immersed by the liquid is a minimum proportion and which varies above this minimum value in dependence on the variation of the said proportion above the minimum proportion; second capacitance means (8) in the tank and having a predetermined second capacitance value which is a reference value; an excitation source (2) connected to energise the first and second capacitance means (6,8) with an AC excitation signal whereby the first capacitance means (6) produces a first measurement signal dependent on the first capacitance value and the second capacitance means (8) produces a second measurement signal dependent on the second capacitance value; a first pair of oppositely poled diodes (D1,D2) connected to receive in parallel the first measurement signal and to split it into two oppositely flowing currents; a second pair of oppositely poled diodes (D3,D4) connected to receive in parallel the second measurement signal and to split it into two oppositely flowing currents; and current to voltage converting means (14,18) connected to respond to the currents and to produce therefrom an indication of the quantity of liquid in the tank; characterised in that the second capacitance value is a predetermined value equal to the value of the first capacitance means under empty tank conditions; and the current to voltage converting means (14,18) comprises (a) a first current to voltage converter (14) connected to respond to the algebraic sum of one of the currents produced by the first diode pair (D1,D2) and the oppositely flowing one of the currents produced by the second diode pair (D3,D4), whereby to produce a first voltage output which is dependent on the magnitude of the excitation signal and on the amount by which the first capacitance value exceeds the minimum value thereof; and (b) a second current to voltage converter (18) connected to respond to the other current produced by the second diode pair (D3,D4) whereby to produce a second output voltage output dependent on the magnitude of the excitation signal and on the second capacitance value; such that the ratio of the first and second voltage outputs provides a liquid quantity indicating signal indicative of the quantity of liquid in the tank and independent of variations in the excitation signal. Apparatus according to claim 1, characterised by a ratio device (20) receiving the first and second voltage output signals and measuring their ratio to produce the said liquid quantity indicating signal. Apparatus according to claim 1 or 2, characterised in that each current to voltage converter comprises a respective operational amplifier (14,18). Apparatus according to claim 3, characterised in that the operational amplifier (14) comprised by the first current to voltage converter has its inverting input connected to one (D1) of the diodes of the first pair (D1,D2) and to the oppositely poled one (D4) of the diodes of the second pair (D3,D4) so as to receive the said algebraic current sum. Apparatus according to claim 3 or 4, characterised in that the operational amplifier (18) comprised by the second current to voltage converter has its inverting input connected to the other diode (D3) of the second pair of diodes (D3,D4). Apparatus according to any one of claims 3 to 5, characterised in that the non-inverting input of each operational amplifier (14,18) is connected to ground. Apparatus according to any one of claims 3 to 6, characterised in that each operational amplifier (14,18) has a feedback path including respective resistor means (R1,R2) whose values have a predetermined ratio. Apparatus according to any preceding claim, characterised in that the said second capacitance means (8) is positioned in the tank.

Inventors: MAIER, LAWRENCE CARL
Applicants: SIMMONDS PRECISION PRODUCTS INC.
Application year: 1988
Main classification: G01F23
IPC codes: G01F23