GB2461099A - Position sensing apparatus and method with feedback control of excitation signal - Google Patents

Position sensing apparatus and method with feedback control of excitation signal Download PDF

Info

Publication number
GB2461099A
GB2461099A GB0811418A GB0811418A GB2461099A GB 2461099 A GB2461099 A GB 2461099A GB 0811418 A GB0811418 A GB 0811418A GB 0811418 A GB0811418 A GB 0811418A GB 2461099 A GB2461099 A GB 2461099A
Authority
GB
United Kingdom
Prior art keywords
aerial
signal
feedback
magnetic field
receive
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
GB0811418A
Other versions
GB0811418D0 (en
GB2461099B (en
Inventor
Jonathan Michael Hayes
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
AVX Electronics Technology Ltd
Original Assignee
TT Electronics Technology Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by TT Electronics Technology Ltd filed Critical TT Electronics Technology Ltd
Priority to GB0811418.3A priority Critical patent/GB2461099B/en
Publication of GB0811418D0 publication Critical patent/GB0811418D0/en
Priority to EP09766141A priority patent/EP2304390A2/en
Priority to PCT/GB2009/001563 priority patent/WO2009153580A2/en
Publication of GB2461099A publication Critical patent/GB2461099A/en
Application granted granted Critical
Publication of GB2461099B publication Critical patent/GB2461099B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D5/00Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/12Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means
    • G01D5/14Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage
    • G01D5/20Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage by varying inductance, e.g. by a movable armature
    • G01D5/204Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage by varying inductance, e.g. by a movable armature by influencing the mutual induction between two or more coils
    • G01D5/2053Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage by varying inductance, e.g. by a movable armature by influencing the mutual induction between two or more coils by a movable non-ferromagnetic conductive element
    • G01D5/206Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage by varying inductance, e.g. by a movable armature by influencing the mutual induction between two or more coils by a movable non-ferromagnetic conductive element constituting a short-circuiting element
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01BMEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
    • G01B7/00Measuring arrangements characterised by the use of electric or magnetic techniques
    • G01B7/003Measuring arrangements characterised by the use of electric or magnetic techniques for measuring position, not involving coordinate determination
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D5/00Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/12Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means
    • G01D5/14Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage
    • G01D5/20Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage by varying inductance, e.g. by a movable armature
    • G01D5/204Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage by varying inductance, e.g. by a movable armature by influencing the mutual induction between two or more coils
    • G01D5/2073Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable using electric or magnetic means influencing the magnitude of a current or voltage by varying inductance, e.g. by a movable armature by influencing the mutual induction between two or more coils by movement of a single coil with respect to two or more coils

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measurement Of Length, Angles, Or The Like Using Electric Or Magnetic Means (AREA)
  • Transmission And Conversion Of Sensor Element Output (AREA)

Abstract

An inductive position sensor has electromagnetic coupling between transmit aerial 9 and receive aerial 7 via intermediate coupling element (magnetic field generator 1 (27, fig. 2) which varies with relative position of first 5 and second members 3 along measurement direction X, whereas electromagnetic coupling between transmit aerial 9 and feedback aerial 11 via intermediate coupling element 1 does not vary in the measurement direction. The strength of an excitation signal applied to one of first 9 and second aerial 7 (depending which used as transmit / receive) is adjusted using a feedback loop to make the strength of a signal representative of electromagnetic coupling between first aerial 9 and third aerial 11 via intermediate coupling element match a reference level. The feedback loop may control amplitude or frequency of the excitation signal. Modifications include an embodiment where magnetic field generator 1 is powered directly, removing need for the transmit aerial; another where a single receive / feedback aerial is used in place of receive aerial 7 and feedback aerial 11. The receive / feedback aerial would operate alternately in receive and feedback modes. Alternatively combined receive / feedback aerial may be used with two transmit aerials each applying excitation signals at different frequencies. Invention ensures position signal induced in receive aerial is predominantly dependent on position of sensor element along measurement direction and does not vary due to variations in position of sensor element perpendicular to measurement direction, variations in properties of resonant circuit 27 fig.2 due to temperature or humidity or variations in transmit aerial due to environmental factors or variation in amplitude of current supplied to aerial.

Description

POSITION SENSING APPARATUS AND METHOD
This invention relates to a position sensing apparatus and method for generating information indicative of the relative position between two members.
Various inductive sensors are known for determining the relative position between two members. In these inductive sensors, the electromagnetic coupling between a transmit aerial and a receive aerial, typically via an intermediate coupling element, varies along a measurement path. Therefore, the signal induced in the receive aerial in response to an excitation signal being applied to the transmit aerial is indicative of the relative position of the first and second members.
A problem with such inductive sensors is that there are a number of other factors which can affect the electromagnetic coupling between the transmit aerial and the receive aerial, and this can affect the accuracy of the position measurement. To address this problem, various ratiometric techniques have been utilised in which the strength of two electromagnetic couplings is compared.
International Patent Publication WO 95/31696 discusses a position sensor in which a transmit winding, a first receive winding and a second receive winding are formed on a first member and a resonant circuit is formed on a second member. The electromagnetic coupling between the transmit winding and the first receive winding via the resonant circuit varies with the relative position of the first and second members in accordance with a first sinusoidal function, whereas the electromagnetic coupling between the transmit winding and the second receive winding via the resonant circuit varies with the relative position of the first and second members in accordance with a second sinusoidal function which is a quarter of a cycle out of phase with the first sinusoidal function. A signal representative of the relative position between the first and second members is determined by calculating the arctangent of the ratio between the amplitude of the signal induced in the first receive winding and the amplitude of the signal induced in the second receive winding in response to a drive signal at the resonant frequency of the resonant circuit being applied to the transmit winding.
However, this calculation is not straightforward to implement.
International patent publication WO 03/038379 discusses an inductive position sensor in which first and second transmit windings and a receive winding are formed on a first member and a resonant circuit is formed on a second member. The first transmit winding is arranged to generate a magnetic field having a component which varies along a measurement direction in accordance with a first sinusoidal function, and the second transmit winding is arranged to generate a magnetic field having a component which varies along the measurement direction in accordance with a second sinusoidal function which is one quarter of a cycle out of phase with the first sinusoidal function. By applying respective oscillating excitation signals to the first and second transmit windings which are one quarter of a cycle out of phase with each other, a signal is induced in the receive winding having a phase which is indicative of the relative position of the first and second members.
In order to measure the phase of the induced signal in a straightforward manner, the frequency of the oscillating signal needs to be relatively low, whereas for high signal strength the frequency of the oscillating signal needs to be relatively high. The position sensor of WO 03/038379 addresses these conflicting requirements by using an oscillating signal at a relatively low frequency to modulate a carrier signal at a relatively high frequency, with the frequency of the carrier signal being set so as to induce a resonant signal in the resonant circuit.
While the performance of the position sensor of WO 03/038379 is high, for some applications such high performance is not required and therefore a less complicated position sensor, and accordingly less expensive, with a lower performance would be preferred.
In accordance with an aspect of the present invention, there is provided a position sensor in which a first aerial and a second aerial are fixed relative to a first member and a magnetic field generator is fixed relative to a second member. An excitation signal generator generates an excitation signal which causes the magnetic field generator to generate a magnetic field which induces a signal in the first aerial indicative of the relative position between the first and second members. The excitation signal generator includes a feedback controller which varies the excitation signal in accordance with a signal representative of the electromagnetic coupling between the magnetic
field generator and the second aerial.
Other aspects of the invention are set out in the accompanying claims.
An exemplary embodiment of the present invention will now be described with reference to the accompanying figures in which: Figure 1 schematically shows a perspective view of a position sensor; Figure 2 shows the main components of the position sensor illustrated in Figure 1; Figure 3 shows in more detail the conductive tracks formed on a first printed circuit board forming part of the position sensor illustrated in Figure 1; Figure 4A shows the layout of a transmit aerial formed on the first printed circuit board; Figure 4B shows the layout of a receive aerial formed on the first printed circuit board; Figure 4C shows the layout of a feedback aerial formed on the first printed circuit board; and Figure 5 shows in more detail the conductive tracks formed on a second printed circuit board forming part of the position sensor illustrated in Figure 1; Figure 6 is a circuit diagram showing in more detail an oscillator forming part of the position sensor illustrated in Figure 1; Figure 7 is a circuit diagram showing in more detail a divide-by-four circuit forming part of the position sensor illustrated in Figure 1; Figure 8 is a circuit diagram showing in more detail a feedback ioop employed in the position sensor illustrated in Figure 1; and Figure 9 is a circuit diagram showing in more detail circuitry employed to generate a position-dependent signal in the position sensor illustrated in Figure 1.
System Overview Figure 1 schematically shows a position sensor for sensing the position of a sensor element 1 which is slidably movable relative to a support 3 to allow linear movement along a measurement direction (the direction X m Figure 1). A first printed circuit board (PCB) 5 extends along the measurement direction adjacent to the support 3 and has thereon conductive tracks which form a receive aerial 7, a transmit aerial 9 and a feedback aerial 11, each of which are connected to a control unit 13. In this exemplary embodiment, a display 15 is also connected to the control unit 13 for displaying a number representative of the position of the sensor element 1 along the support 3.
As shown in Figure 1, the first PCB 5 is generally rectangular in shape with the lengthwise axis aligned with the measurement direction and the widthwise axis aligned perpendicular to the measurement direction. The receive aerial 7, the transmit aerial 9 and the feedback aerial 11 are connected to the control unit 13 via a lengthwise edge of the first PCB 5, which corresponds to the position value of x equals zero, with the position value increasing along the length of the first PCB 5 from the lengthwise edge corresponding to x equals zero.
Figure 2 schematically shows the main components of the position sensor illustrated in Figure 1. As shown, an oscillator 21 generates an oscillating signal at 16 MBz. The signal output by the oscillator is input to a conventional divide-by-four circuit 23 which outputs four signals at 4 MHz, namely: -a first signal (hereafter called the 0° signal); -a second signal (hereafter called the 90° signal) which lags the first signal by a quarter of a cycle; -a third signal (hereafter called the 1800 signal) which lags the first signal by haifa cycle; and -a fourth signal (hereafter called the 270° signal) which lags the first signal by three-quarters of a cycle.
The 0° and 180° signals output by the divide-by-four circuit 23 are input to drive circuitry 25 which generates an excitation signal which is applied to the transmit aerial 9, which results in the generation of a magnetic field which oscillates at 4MHz. As will be described in more detail hereafter, in accordance with the invention, the amplitude of the excitation signal is controlled by a feedback loop.
In this embodiment, the sensor element 1 has a resonant circuit 27 which is formed by an inductive winding 29 and a capacitor 31 mounted on a second PCB. The resonant frequency of the resonant circuit is at 4MHz, and accordingly the oscillating magnetic field generated by the transmit aerial induces an oscillating signal at 4MHz in the resonant circuit 27. As those skilled in the art will appreciate, the resonant signal induced in the resonant circuit 27 is shifted in phase by a quarter of a cycle from that of the oscillating
magnetic field.
The resonant signal induced in the resonant circuit 27 itself generates an oscillating magnetic field, and this oscillating magnetic field induces signals in the receive aerial 7 and the feedback aerial 11. In this embodiment, the amplitude of the oscillating signal induced in the feedback aerial 11 by the resonant signal in the resonant circuit 27 does not vary with the position of the sensor element 1 along the measurement direction, while the amplitude of the of the oscillating signal induced in the receive aerial 7 by the resonant signal in the resonant circuit 27 varies linearly in accordance with the position of the sensor element 1 along the measurement direction.
Although the signal induced in the feedback aerial 11 does not vary in accordance with the position of the sensor element 1 along the measurement direction, it may vary for a number of different factors including: -variations in the distance between the sensor element 1 and the first PCB 5 in a direction perpendicular to the measurement direction of the first PCB 5; -variations in the frequency of the ceramic resonator in the oscillator 21; -variation in the amplitude of the current supplied to the transmit aerial 9 as a result of variation in the impedance of the drive cicuitry 25 and the impedance of the conductive track forming the transmit aerial with environmental factors such as temperature; and -variations in the resonant properties of the resonant circuit 27 with changing environmental factors, e.g. temperature, humidity.
In a similar fashion, these factors will cause a variation in the amplitude of the signal induced in the receive aerial 7, and uncorrected those variations would lead to inaccuracy in the measurement reading.
Accordingly, in this embodiment a feedback control loop is used to vary the amplitude of the excitation signal to cause the amplitude of the signal induced in the feedback aerial 11 to be set at a reference level.
As shown in Figure 2, the signal induced in the feedback aerial 11 is input to a synchronous detector 33 which performs synchronous detection at the excitation frequency using the 90° and 270° outputs of the divide-by-four circuit 23 in order to take into account the phase shift introduced by the resonant circuit 27. The output of the synchronous detector 33 approximates a full-wave rectified signal, and is passed through a low pass filter 35 to generate a DC signal corresponding to the amplitude of the signal induced in the feedback winding.
The output of the low pass filter 35 is input to a servo-system 37 along with a reference voltage level generated by a reference voltage level generator 39. The output of the servo-system 37 is input to the drive circuitry 25 to control the amplitude of the excitation signal applied to the transmit aerial 9.
In operation, the servo-system 37 controls the amplitude of the excitation signal so that the signal output by the low pass filter 35 matches the reference voltage level, thereby forming a feedback control loop.
As a result of this feedback control, the amplitude of the signal induced in the receive aerial 7 is predominantly dependent on the position of the sensor element along the measurement direction. As shown in Figure 2, the signal induced in the receive aerial 7 is input to a synchronous detector 41 which performs synchronous detection at the excitation frequency using the 90° and 2700 outputs of the divide-by-four circuit 23 in order to take into account the phase shift introduced by the resonant circuit 27. The output of the synchronous detector 41 is then input to a low-pass filter and buffer 43, whose output is a DC signal having an amplitude which is dependent on the position of the sensor element 1 along the measurement direction.
In the exemplary embodiment, the signal output by the low pass filter and buffer 43 is converted to a numerical value which is then displayed on the display 15.
The layouts of the receive aerial 7, the transmit aerial 9, the feedback aerial 11 and the resonant circuit 27 will now be described in more detail, followed by a more detailed description of the main components of the circuitry.
Aerial Layouts Figure 3 shows the layout of the conductive tracks on the first PCB 5 which form the receive aerial 7, the transmit aerial 9 and the feedback aerial 11. In this embodiment, the first PCB 5 is a multi-layer PCB with conductive tracks being deposited on both planar surfaces (referred to hereafter as the top surface and the bottom surface for ease of reference), with connection bet*een the conductive tracks on the top and bottom surfaces occurring through via holes. In Figure 3 and the following Figures, conductive tracks deposited on the top surface are shown by solid lines whereas conductive tracks deposited on the bottom surface are shown by dashed lines.
For ease of explanation, Figures 4A to 4C respectively show just the conductive tracks forming the transmit aerial 9, the receive aerial 7 and the feedback aerial 11. As shown in Figures 4A to 4C, the transmit aerial 9 is almost exclusively formed by conductive tracks deposited on the bottom surface of the first PCB 5, whereas the receive aerial 7 and the feedback aerial 11 are predominantly formed on the top surface of the first PCB 5.
The transmit aerial 9 has a first set of three current loops around the periphery of the first PCB 5, with a second set of three current loops in the same sense as the first set positioned adjacent the widthwise edge of the first PCB 5 away from the widthwise edge corresponding to x equals zero. The second set of three current loops extend over about one fifth of the length of the first PCB 5.
The feedback aerial 11 has a first set of three current loops which extend from the widthwise edge of the first PCB 5 corresponding to x equals zero over about four fifths of the length of the first PCB 5, and a second set of six current loops in the opposite sense to the first set of three current loops which extend over the remaining fifth of the length of the first PCB 5 so that they are substantially aligned with the second set of three current loops of the transmit aerial. In this way, the transmit aerial 9 and the feedback aerial 11 are balanced (i.e. an alternating electromagnetic field generated by the transmit aerial 9 directly induces substantially no signal in the feedback aerial 11) in a manner which is well known to those skilled in the art.
The receive aerial 7 extends over about four fifths of the length of the first PCB 5 from the widthwise edge corresponding to x equals zero. The pattern of the conductive track of the receive aerial 7 is such that any perpendicular electromagnetic field component close to the position x equals zero passes through six current ioops in one sense, and then moving in the measurement direction without changing sense the number of current loops reduces from five, then four then, three, then two and then one until finally at the central point of the length of the receive aerial 7 any perpendicular electromagnetic field component passes through no current loops. Continuing along the measurement direction, the sense of the current loops changes and the number of current loops increase from one, to two, to three, to four, to five and finally to six.
The particular arrangement of the receive aerial 7 results in the signal induced in the receive aerial 7 varying in dependence on the position of the sensor element 1 in a linear manner from a maximum positive value adjacent to x equals zero, reducing to zero in the middle of the receive winding, and then reducing further to a maximum negative value at the end of the receive aerial 7 away from x equals zero. In addition, the anti-symmetric arrangement of the current loops of the receive aerial 7 leads to the receive aerial 7 being substantially balanced with respect to the transmit aerial 9.
For completeness, Figure 5 shows that the inductor 29 of the resonant circuit 27 of the sensor element 1 is formed by conductive track on the second PCB arranged in a concentric set of current loops. The ends of the conductive track are joined by the capacitor 31 (not shown in Figure 5).
Circuitry Components As shown in Figure 6, the oscillator 21 employs a standard oscillator circuit. In this embodiment, the oscillator circuit includes a ceramic oscillator 51, which combines both good stability and relatively low cost. As shown in Figure 7, the divide-by-four circuit 23 is a conventional circuit using two flip-flops 61a,61b. The outputs of the flip-flop 61a supply the 900 and 270° signals, while the outputs of flip-flop 61b supply the 0° and 180° signals.
Figure 8 shows the circuitry within the feedback ioop from the feedback aerial 11 to the drive circuitry 25 which supplies the excitation signal to the transmit aerial 9. As shown, the signal induced in the feedback aerial 11 is input to a crossover analogue switch which forms the synchronous detector 33. As discussed above, the crossover analogue switch is controlled by the 900 signal and 270° signal to take account of the phase shift introduced by the resonant circuit 27.
The output of the synchronous detector 33 is input, via the low pass filter 35, to the inverting input of an operational amplifier forming part of the servo-system 37. A potential divider is used as the reference voltage level generator 39, and the resultant reference voltage level is input to the non-inverting input of the operational amplifier of the servo-system 37.
As those skilled in the art will recognise, the servo system 37 is effectively a P-I-D (proportional -integral -derivative) controller in which the integral component dominates. In other words, the historical variation between the signals input to the non-inverting and inverting inputs of the operational amplifier largely determine any change in the output of the servo-system 37. For the particular components used in this embodiment, this was found to produce good results.
The output of the servo-system 37 supplies the power rail for the drive circuitry 25, which as discussed above supplies an oscillating excitation signal to the transmit aerial 9 in accordance with the 0° and 180° signals. The drive circuitry itself is a well-known arrangement employing a pair of MOSFETS.
S
In use, if the signal induced in the feedback aerial 11 exceeds a desired level, then the signal input to the inverting input of the operational amplifier of the servo system 37 will rise above the reference voltage level. This leads to the output of the servo system 37 dropping, resulting in a decrease in the amplitude of the oscillating excitation signal and accordingly a decrease in the amplitude of the signal induced in the feedback aerial 11. Similarly, if the signal induced in the feedback aerial 11 falls below a desired level, then the signal input to the inverting input of the operational amplifier of the servo system 37 will drop below the reference voltage level. This leads to the output of the servo system 37 increasing, resulting in an increase in the amplitude of the oscillating excitation signal and accordingly an increase in the amplitude of the signal induced in the feedback aerial 11.
Figure 9 shows the circuitry used to process the signal from the receive aerial 7. As shown, the signal induced in the receive aerial 7 is input to the synchronous detector 41, which in this embodiment comprises an analogue cross-over switch. As discussed above, the analogue cross-over switch is driven by the 90° and 270° signals to take account of the phase shift introduced by the resonant circuit 27. The potential divider circuit in the synchronous detector 41 is used to set a virtual ground about which the signal received from the receive aerial 7 oscillates.
The output of the synchronous detector 41 is input to a low pass filter and buffer 43, which outputs a DC signal which varies in accordance with the position of the sensor element along the measurement direction.
MODIFICATIONS AND FURTHER EMBODIMENTS
In the exemplary embodiment, a feedback ioop controls the amplitude of a drive signal applied to the transmit aerial 9 at a substantially fixed frequency. Alternatively, a voltage-controlled oscillator could be used with the feedback loop controlling the frequency of the oscillating signal generated by the voltage-controlled oscillator. In this way, the strength of the signal induced in the resonant circuit would be varied as the frequency of the excitation signal moved relative tothe resonant frequency (i.e. increasing as the excitation frequency approaches the resonant frequency and decreasing as the excitation frequency moves away from the resonant frequency), and therefore the strength of the signal induced in the feedback aerial would vary.
In the exemplary embodiment, a passive resonant circuit 27 on the sensor element 1 acts as an intermediate coupling element between the transmit aerial and both the receive aerial and the feedback aerial.
Alternatively an active resonant circuit, including a power source for amplification, could be used. A non-resonant intermediate coupling element could alternatively be used, for example a ferrite element, a conductive disk or a simple wire loop. Unlike the resonant circuit, these other intermediate coupling elements do not introduce a 90° phase shift and therefore the circuitry can be slightly simplified. However, the use of a resonant circuit as an intermediate coupling element gives higher signal strength.
The intermediate coupling element could include a non-linear element, such as a diode, so that a magnetic field oscillating at an excitation frequency induces a current in the intermediate coupling element having frequency components away from the excitation frequency. This would result in a signal being induced in the receive aerial at these new frequency components, which could be detected and have improved noise immunity with respect to the excitation signal generating circuitry.
The intermediate coupling element effectively acts as a magnetic field generator which is powered through inductive coupling with the transmit aerial. In an alternative embodiment, a magnetic field generator on the sensor element could be directly powered, with the excitation signal applied being controlled in accordance with the signal induced in the feedback aerial. Such art arrangement has the advantage of removing the need of a transmit aerial, but also has the significant disadvantage of requiring electrical connections to the sensor element.
Two synchronous detectors are employed in the exemplary embodiment, one to detect the signal induced in the receive aerial and one to detect the signal induced in the feedback aerial. This allows the feedback loop to work continuously. In an alternative embodiment, a single feedback/receive aerial could be used in a first mode as a feedback aerial and in a second mode as a receive aerial, the first mode and the second mode being sequentially selected. The amplitude of the drive signal applied in the second mode is determined by the strength of the signal induced in the
S
feedback/receive aerial in the first mode. This requires using in the first mode a first transmit aerial whose electromagnetic coupling via the resonant circuit with the feedback/receive aerial does not vary with the position of the sensor element, and in the second mode a second transmit aerial whose electromagnetic coupling via the resonant circuit with the feedback/receive aerial does vary with position of the sensor element.
Another alternative would be to apply an excitation signal at a first frequency to a first transmit aerial, whose electromagnetic coupling via the resonant circuit with a feedback/receive aerial does not vary with position of the sensor element along the measurement direction, and concurrently to apply an excitation signal at a second frequency (which is different from the first frequency) to a second transmit aerial whose electromagnetic coupling via the resonant circuit with the feedback/receive aerial does vary with position. In this way, the strength of the signal induced in the feedback receive aerial at the first frequency can be used to adjust the amplitude of the excitation signal at the second frequency applied to the second transmit aerial.
Those skilled in the art will appreciate that there are many different possible layouts of the aerials. Those skilled in the art will also recognise that synchronous detection is not essential, and for example could be replaced by a full-wave or half-wave rectifier arrangement.
While 4IVlIHz has been found to be a convenient frequency of operation, other frequencies could be used. Typically, the operational frequency will be in the range from 10kHz to 10MHz.
S
In the exemplary embodiments described above, the position sensor measures the position of a first member (the sensor element 1) relative to a second member (the first PCIB 5) along a rectilinear measurement path.
Alternatively, the position sensor could be adapted to measure linear position along a curved measurement path, for example a circle (i.e. a rotary position sensor), by varying the layout of the transmit aerial, the receive aerial and the feedback aerial in a manner which would be apparent to a person skilled in the art. The position sensor could also be used as a speed detector by taking a series of measurements of the position of the first member relative to the second member at known timings.
In the exemplary embodiment, the aerials are formed by conductive tracks on a printed circuit board. Alternatively, a different planar substrate could be used. Further, if the aerials are themselves sufficiently rigid then they could be fixed relative to the first member and the resonant circuit could be fixed relative to the second member without the use of a substrate. It is also not essential that the aerials be planar because, for example, a cylindrical geometry could be used.
Of course, as the position sensor detects the relative position between first and second members, it does not matter which of the first member and the second member are moved, or even if both are moved.

Claims (9)

  1. SCLAIMS1. Apparatus for generating information indicative of the relative position between a first member and a second member, the apparatus comprising: a first aerial and a second aerial fixed relative to the first member and a magnetic field generator fixed relative to the second member; and an excitation signal generator operable to generate an excitation signal which causes the magnetic field generator to generate a magnetic field which induces a signal in the first aerial indicative of the relative position between the first and second members, wherein the excitation signal generator comprises a feedback loop operable to vary the generated excitation signal in accordance with a signal representative of the electromagnetic coupling between the magnetic field generator and the second aerial.
  2. 2. Apparatus according to claim 1, further comprising a third aerial fixed relative to the first member, wherein the excitation signal generator is arranged to apply the excitation signal to the third aerial in order to generate a magnetic field which induces the magnetic field generator to generate said first-mentioned magnetic field, whereby the magnetic field generator acts as an intermediate coupling element between the third aerial and the first aerial and between the third aerial and the second aerial.S
  3. 3. Apparatus according to claim 2, wherein the magnetic field generator comprises a resonant circuit, and the excitation signal generator is operable to cause the third aerial to generate an oscillating magnetic field having a frequency component operable to induce resonance in the resonant circuit.
  4. 4. Apparatus according to claim 2 or 3, wherein the feedback ioop is arranged to control the amplitude of the drive signal.
  5. 5. Apparatus according to any preceding claim, wherein the feedback controller comprises a servo-system operable to generate an output which depends upon the difference between the amplitude of the signal induced in the second aerial and a reference value.
  6. 6. Apparatus according to claim 5, wherein the servo-system is arranged to generate an output which depends predominantly on the integral of said difference between the amplitude of the signal induced in the second aerial and the reference value over a period of time.
  7. 7. Apparatus according to any preceding claim, wherein the first and second aerials are fumed on a planar substrate.S
  8. 8. Apparatus according to claim 7, wherein the planar substrate is a printed circuit board.
  9. 9. Apparatus for generating information indicative of the relative position between a first member and a second member, the apparatus comprising: a first aerial, a second aerial and a third aerial fixed relative to the first member and an intermediate coupling element fixed relative to the second member, wherein the electromagnetic coupling between the first aerial and the second aerial via the intermediate coupling element varies with the relative position of the first and second members along a measurement direction and the electromagnetic coupling between the first aerial and the third aerial via the intermediate coupling element does not vary with the relative position of the first and second members along the measurement direction; and an excitation signal generator operable to apply an excitation signal to one of the first aerial and the second aerial in order to induce a signal in the other of the first aerial and the second aerial indicative of the relative position between the first and second members, wherein the excitation signal generator comprises a feedback loop operable to vary the generated excitation signal in accordance with a signal representative of the electromagnetic coupling between the first aerial and the third aerial.
GB0811418.3A 2008-06-20 2008-06-20 Position sensing apparatus and method Expired - Fee Related GB2461099B (en)

Priority Applications (3)

Application Number Priority Date Filing Date Title
GB0811418.3A GB2461099B (en) 2008-06-20 2008-06-20 Position sensing apparatus and method
EP09766141A EP2304390A2 (en) 2008-06-20 2009-06-22 Position sensing apparatus and method
PCT/GB2009/001563 WO2009153580A2 (en) 2008-06-20 2009-06-22 Position sensing apparatus and method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
GB0811418.3A GB2461099B (en) 2008-06-20 2008-06-20 Position sensing apparatus and method

Publications (3)

Publication Number Publication Date
GB0811418D0 GB0811418D0 (en) 2008-07-30
GB2461099A true GB2461099A (en) 2009-12-23
GB2461099B GB2461099B (en) 2012-02-08

Family

ID=39682949

Family Applications (1)

Application Number Title Priority Date Filing Date
GB0811418.3A Expired - Fee Related GB2461099B (en) 2008-06-20 2008-06-20 Position sensing apparatus and method

Country Status (3)

Country Link
EP (1) EP2304390A2 (en)
GB (1) GB2461099B (en)
WO (1) WO2009153580A2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP3472567B1 (en) * 2016-06-17 2020-04-22 Thin Film Electronics ASA Wireless mechanism for detecting an open or closed container, and methods of making and using the same

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE112018008038T5 (en) * 2018-10-16 2021-06-24 Ab Elektronik Gmbh Position sensing device and method
US10760928B1 (en) * 2019-02-21 2020-09-01 Microsemi Corporation Planar linear inductive position sensor having edge effect compensation

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2004072653A2 (en) * 2003-02-17 2004-08-26 Sensopad Limited Sensing apparatus and method
US20040227644A1 (en) * 2003-05-15 2004-11-18 Yingjie Lin Linear position sensor
GB2417088A (en) * 2004-08-09 2006-02-15 Sensopad Ltd Inductive sensing apparatus with noise reduction
WO2006016147A2 (en) * 2004-08-09 2006-02-16 Sensopad Limited Inductive sensor

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB869899A (en) * 1958-03-03 1961-06-07 Eric Miles Langham Improvements in electrical measuring devices
US6124787A (en) * 1997-01-15 2000-09-26 Algonquin Scientific, Llc Tire pressure sensing system
DE10016540C1 (en) * 2000-03-03 2001-07-19 Balluff Gebhard Gmbh & Co Inductive measuring sensor has displaced measuring head provided with measuring inductive loop of varying geometric shape and reference loop of constant geometric shape
DE10219678C1 (en) * 2002-05-02 2003-06-26 Balluff Gmbh Inductive displacement sensor has angularly or linearly displaced measuring head provided with passive resonance circuit

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2004072653A2 (en) * 2003-02-17 2004-08-26 Sensopad Limited Sensing apparatus and method
US20040227644A1 (en) * 2003-05-15 2004-11-18 Yingjie Lin Linear position sensor
GB2417088A (en) * 2004-08-09 2006-02-15 Sensopad Ltd Inductive sensing apparatus with noise reduction
WO2006016147A2 (en) * 2004-08-09 2006-02-16 Sensopad Limited Inductive sensor

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP3472567B1 (en) * 2016-06-17 2020-04-22 Thin Film Electronics ASA Wireless mechanism for detecting an open or closed container, and methods of making and using the same
US11119158B2 (en) 2016-06-17 2021-09-14 Thin Film Electronics Asa Wireless mechanism for detecting an open or closed container, and methods of making and using the same

Also Published As

Publication number Publication date
WO2009153580A2 (en) 2009-12-23
GB0811418D0 (en) 2008-07-30
EP2304390A2 (en) 2011-04-06
WO2009153580A3 (en) 2010-03-11
GB2461099B (en) 2012-02-08

Similar Documents

Publication Publication Date Title
US7514919B2 (en) Sensing apparatus and method
CN1278104C (en) Induction sensing apparatus and method
US6002250A (en) Electronic linear scale using a self-contained, low-power inductive position transducer
EP2145158B1 (en) Transducer
US7298137B2 (en) Position sensing apparatus and method
WO2006016147A2 (en) Inductive sensor
JP2016509238A (en) Position detection system
US20080204116A1 (en) Sensing Apparatus And Method
EP1595115A2 (en) Sensing apparatus and method
GB2374424A (en) Induction sensing apparatus and method
GB2394295A (en) Position sensing apparatus utilising signals induced in two resonators placed on a moving member
GB2461099A (en) Position sensing apparatus and method with feedback control of excitation signal
GB2493399A (en) Inductive position sensor with multiple resonant circuits of differing resonant frequencies
RU2717904C1 (en) Method of measuring using differential sensor
SU1044962A1 (en) Article conductive layer thickness measuring method
JPH0667790A (en) Coordinate input device

Legal Events

Date Code Title Description
PCNP Patent ceased through non-payment of renewal fee

Effective date: 20130620