1. Field of the Invention
The present invention relates to electrical potentiometric devices, and to electronic ratiometric devices, more specifically, to electronic devices developed for the purpose of replacing or simulating the electrical characteristics of a potentiometric device. Further, the present invention relates to sensors having a potentiometric electrical connection, or ratiometric output signal.
2. Description of the Prior Art
A Prior Art potentiometric device, also called a potentiometer, is a three-terminal electrically resistive device. See
A power source is connected to the potentiometer such that a power supply voltage appears across first and third terminals 6, 8, of
The resistive element 1, typically comprises a substrate of ceramic or other mechanically suitable electrically insulative material, having at least one surface that is coated with a thin layer of electrically resistive material. Typical power supply voltages for a potentiometer are 5, 10 or 24 volts DC, but other voltages may be used. It is uncommon for the power supply voltage to be above 30 volts DC. Typical resistances of the resistive element are one or two thousand ohms when used with a five volt power supply, five thousand ohms when used with a ten volt power supply, or ten thousand ohms when used with a twenty four volt power supply. It is not desirable to use a lower resistance element, such as one thousand ohms, with a higher power supply voltage, such as 10 or 24 volts, due to the higher current that would be drawn from the power source, and the resulting increase in power dissipation of the potentiometer.
As shown in
The main advantage of using a potentiometer as a means for providing a variable voltage is its simplicity. The major disadvantage of a potentiometer is that mechanical contact between the wiper and the resistive element constitutes a mechanism for wear. Wear resulting from repeated mechanical motion of the wiper normally limits the lifetime of a potentiometer. End of service life of a potentiometer typically occurs when wearing of the surface of the resistive element causes erratic voltages to appear on its output (represented here as second terminal 7), due to several factors, including buildup of particles that have been scraped from the resistive element by the wiper movement, partially bare spots where the coating of the resistive element has been removed from the underlying substrate, as well as changing the contact properties of the surface of the resistive element.
It is common in the prior art for other types of electronic devices to be developed in attempts to simulate the simplicity of wiring that is inherent with a potentiometer, but having other undesirable attributes which limit such an electronic device from being directly interchangeable with a potentiometer. Some of the undesirable attributes of such prior art electronic devices include a higher current draw from the power source, a more narrow range of allowable power supply voltage, and a more narrow range of output voltage available. Many such prior art electronic devices require a power supply voltage in the narrow range of 5.0 volts +/−0.5 volts, and provide an output voltage range of 10% to 90% of the power supply voltage for indications of zero and full scale, respectively. Such prior art electronic devices typically draw from 10 to 150 milliamperes of current from the power source.
A potentiometer is commonly employed to provide a variable output voltage in response to a physical parameter being measured (that is, in response to a parameter). Such a potentiometer is often configured as a position-measuring sensor, but potentiometric devices can be used to sense other parameters such as pressure, flow, etc. when coupled to a mechanical system that provides a mechanical motion proportional to the parameter.
The physical parameter can be mechanically coupled to the potentiometer directly, or transduced from one form of mechanical energy or motion into another as appropriate for the given parameter. For example, a diaphragm or bellows can be used to transduce a pressure measurand into a linear motion. The linear motion can be coupled to a linear potentiometer. Such a potentiometric device or combination of potentiometer and transducer can be called a potentiometric sensor.
A potentiometric sensor with a wiper that contacts and rubs along a surface of the resistive element is called a “contact-type” sensor, that is, the wiper makes mechanical contact with the resistive element. Because the typical potentiometer has only three wires, it is relatively simple to connect into an electrical system, and is also easily understood.
Various electronic devices, and especially sensors, have been developed which simulate the function of a potentiometric device to some extent. The output of such a device or sensor is typically called ratiometric. In a device having a ratiometric output, an output voltage is developed that is similar to an output voltage developed in a potentiometric sensor, in that the output voltage is a percentage of an applied power supply voltage. Many ratiometric electronic sensors have an advantage over an actual potentiometric contact-type sensor, because they can utilize capacitive, inductive, or magnetic sensing, for example, and thereby make their measurement without physical contact among moving and non-moving members comprising the device or sensor. This type of sensor arrangement is called a non-contact ratiometric sensor. This eliminates mechanical wear, and can provide an increase in the service lifetime of the sensor.
By virtue of having a three-wire electrical connection, a non-contact ratiometric sensor as described above can sometimes be used as a replacement for a potentiometric contact-type sensor. A typical sensor of this type uses an electronic circuit that requires an input voltage of 4.5 to 5.5 volts DC at a current level of between 10 mA and 150 mA, and produces an output voltage in the range of 10% to 90% of the power supply voltage in response to a 0% to 100% range of a measurand. For example, with a 0 to 1 inch linear position sensor having a power supply voltage of 5.0 volts DC, an output voltage range would typically be 0.5 to 4.5 volts DC for positions from 0 inches to 1 inch. Although this can be accommodated by some types of receiving electronics with appropriate adjustments, it is not serviceable as a direct replacement of a potentiometric contact-type sensor in many applications.
To the contrary, the present invention teaches an apparatus which can directly replace a potentiometric contact-type sensor in virtually all applications, while preserving its desirable performance characteristics and simplicity of wiring.
The present invention teaches a method and apparatus for providing a direct replacement of a potentiometer by an electronic circuit, and in some cases, a sensing element, while retaining the simple connection scheme and electrical performance of a potentiometer. This is accomplished by using a novel mix of digital and analog circuit techniques, providing output voltages very close to the voltages of the power supply, for example, 0 and 10 volts DC, while also accommodating a power supply voltage over a wide range of voltages (including for example, 5, 10, and 24 volts DC), and with a very low power supply current (for example, less than 5.0 milliamperes). The analog circuits provide compatibility with a potentiometer application, while the digital circuits maintain accuracy that could otherwise be lost with a primarily analog circuit. The digital circuit techniques include using standard logic levels while the input signal is in the form of a frequency or a duty cycle, and using the voltage potential across the simulated potentiometer as special logic levels during translation to the analog circuitry. An analog circuit technique converts the duty cycle representation of the signal into an output voltage that is centered on the power supply voltage, and so that the output voltage has a range extending to the power supply rails. In some cases, extended power supply voltages are developed.
For further understanding of the nature and objects of the present invention, reference is made to the following figures in which like parts are given like reference numerals and wherein:
Unless otherwise stated, a power source to the various circuits described here will be assumed to be from a power supply having a voltage in the range of 5 to 30 volts DC. Except for actual contact-type potentiometers, Prior Art has not disclosed an electronic potentiometric or ratiometric device having such a wide range of power supply voltage. If using mainly analog techniques, it has been difficult to maintain accuracy over such a range. If using mainly digital techniques, transition from logic levels to a wide voltage range has been difficult. But to the contrary, the present invention uses a novel mix of analog and digital techniques to circumvent such difficulties.
In this description of some preferred embodiments of the present invention, the positive terminal of a power source will be called power supply, and the negative terminal of a power source will be called common. This is a configuration that is often used with industrial applications in the field of the invention.
Vout =(Vref−Vsig)*(1+R33/R31) (1)
Frequency input 13 is an alternating current (AC) voltage having a frequency indicative of a parameter which is desired to be represented on output voltage terminal 11 as a DC voltage, in the form of a percentage of the voltage difference between first terminal 10 and third terminal 12. This frequency operates a monostable multivibrator, also called a one-shot. The output of one-shot 15, is normally at a logic level zero when it receives no input transitions, but changes to a logic level one for a fixed period of time with each low-going transition of the frequency input. There is one low-going transition for each cycle of the frequency input. After that fixed period, the one-shot output returns approximately to the voltage of common, which is logic level zero. Logic level one is a regulated positive voltage, with respect to third terminal 12. While at logic level one, the one-shot period operates transistor 26, turning it on, through current limiting resistor 20, so that the collector of transistor 26 goes approximately to the same voltage as common while the transistor is turned on. First terminal 10, second terminal 11, and third terminal 12 of the present invention according to
Using digital circuitry as described, that is, logic levels rather than analog voltages, allows the signal to be represented accurately, without any degradation as would be evident with analog voltages.
When the output of one-shot 15 goes back to logic level zero, transistor 26 turns off, and its collector voltage becomes approximately equal to the voltage of first terminal 10.
So, when considering the waveform of the collector voltage of transistor 26 over several cycles of the input frequency, the collector voltage goes to a positive voltage and to common with a duty cycle proportionate with the input frequency. Low pass filter 30 filters the waveform of transistor 26 collector, thereby presenting a variable DC voltage to the non-inverting input of amplifier 32. As stated above, the voltage appearing at the non-inverting input of amplifier 32 is called Vsig.
Inverter 14 drives a positive charge pump circuit comprising capacitors 16, 21, and diodes 22, 23 to provide an extended positive supply voltage, V++, to amplifier 32, which is more positive than the voltage at first terminal 10. Inverter 14 also drives a negative charge pump circuit comprising capacitors 17, 25, and diodes 18, 19 to provide an extended negative supply voltage, V−−, to amplifier 32, which is more negative than the voltage at third terminal 12. Powering amplifier 32 in this way allows the output of amplifier 32 to range up to the voltage of first terminal 10 and down to the voltage of third terminal 12, even though amplifier 32 may not be able to produce outputs equal to the extents of its power supply voltage. Even so-called rail-to-rail output operational amplifiers are not able to produce outputs equal to their power supply rails, and even less-so when having a load resistance connected.
Assuming some typical values, in which resistors 27, and 28 each have a resistance of 49.9 k ohms (k representing a factor of 1,000), the resistance of resistor 31 being 100 k ohms, the voltage at first terminal 10 equal to 10 volts DC, the voltage at third terminal 12 at zero volts DC, and the one-shot period being listed as P1s, the table of
In
Period is the reciprocal value of Fin, and is in microseconds. P1s is the on-time of one-shot 15 after it is triggered. Power supply voltage, Vps, is a voltage applied across first terminal 10 and third terminal 12. Vsig is derived as:
Vsig=Vps*P1s/Period (2)
Gain is derived as:
G=(2/Fsens)−1 (3)
The value of resistor 33, which is R33 in the table, is derived as:
R33=(G−1)*R31 (4)
and R31 had a value of 100 k ohms for generation of the table.
Vref is one half of the power supply voltage. Vout is derived according to formula (1), with R31 being 100 k.
The frequency input 13, shown in
A first sensing terminal 45, and a second sensing terminal 46, are to be connected to a resonant circuit, such that the resonant frequency is representative of a parameter. If the parameter is that of a rotational angle or arc, then sensing apparatus such as shown pictorially in
Voltage regulator 40, in
First sensing terminal 45 in
Target 51 is made of an electrically conductive material, and is shown in view A such that it does not cover any part of top or bottom conductor patterns 53, 55. In this position, the resonant circuit formed by a sensing element according to
In like manner, a linear position sensor can be fashioned to use in place of the rotational sensing element of
The present invention may also be useful in any application where it is desired to represent a variable frequency input (to insert as frequency input 13), as a potentiometric output voltage. This may include many types of applications where a sensing element is not used, and in which it is not desired to sense any physical parameter, other than a parameter represented by the frequency input.
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Number | Date | Country | |
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20100231191 A1 | Sep 2010 | US |