[go: up one dir, main page]

WO1999011999A1 - Method and apparatus for measuring rotation motion - Google Patents

Method and apparatus for measuring rotation motion Download PDF

Info

Publication number
WO1999011999A1
WO1999011999A1 PCT/FI1997/000519 FI9700519W WO9911999A1 WO 1999011999 A1 WO1999011999 A1 WO 1999011999A1 FI 9700519 W FI9700519 W FI 9700519W WO 9911999 A1 WO9911999 A1 WO 9911999A1
Authority
WO
WIPO (PCT)
Prior art keywords
sensor
voltage
magnetic field
value
gauged
Prior art date
Application number
PCT/FI1997/000519
Other languages
French (fr)
Inventor
Harri Saario
Original Assignee
Harri Saario
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
Priority to FI961010A priority Critical patent/FI103215B1/en
Priority claimed from FI961010A external-priority patent/FI103215B1/en
Application filed by Harri Saario filed Critical Harri Saario
Priority to PCT/FI1997/000519 priority patent/WO1999011999A1/en
Publication of WO1999011999A1 publication Critical patent/WO1999011999A1/en

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01PMEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
    • G01P3/00Measuring linear or angular speed; Measuring differences of linear or angular speeds
    • G01P3/42Devices characterised by the use of electric or magnetic means
    • G01P3/44Devices characterised by the use of electric or magnetic means for measuring angular speed
    • G01P3/48Devices characterised by the use of electric or magnetic means for measuring angular speed by measuring frequency of generated current or voltage
    • G01P3/481Devices characterised by the use of electric or magnetic means for measuring angular speed by measuring frequency of generated current or voltage of pulse signals
    • G01P3/487Devices characterised by the use of electric or magnetic means for measuring angular speed by measuring frequency of generated current or voltage of pulse signals delivered by rotating magnets
    • 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
    • G01B7/30Measuring arrangements characterised by the use of electric or magnetic techniques for measuring angles or tapers; for testing the alignment of axes
    • 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
    • G01D3/00Indicating or recording apparatus with provision for the special purposes referred to in the subgroups
    • G01D3/02Indicating or recording apparatus with provision for the special purposes referred to in the subgroups with provision for altering or correcting the law of variation
    • 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
    • G01D5/142Mechanical 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 using Hall-effect devices
    • G01D5/145Mechanical 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 using Hall-effect devices influenced by the relative movement between the Hall device and magnetic fields

Definitions

  • the invention is concerned with the method that conforms to the introduction of the patent claim 1 and with the equipment that conforms to the introduction of the patent claim 8 to gauge rotary motion.
  • a disadvantage of this solution is generating a magnetic field. Separate magnets ought to have the same strength and they ought to be in a segmental form filling the circumference of the circle. Besides, the gauging instrument must work out arithmetical operations to find out the angle value.
  • the solution is not adapted for example for a quick regulating of the angle position of the axle where the axle must be stopped in a predetermined angle position, go immediately to a new position etc.
  • the identifier has a rotating axle with a wheel or a corresponding element on which circumference there are poles with positive and negative magnets alternately in large numbers. While the axle is rotating, the magnets are passing the three Hall sensors placed one after another in the direction of rotation. Each sensor gives a variable signal output. By combining the sensor outputs it is possible to double the output frequency and to improve the accuracy.
  • the Hall sensors can be advantageously manufactured as one component.
  • a disadvantage of the US patent 5,241 ,267 is a need of a multipolar magnetic wheel or ring as well as the fact that the invention is only adapted for gauging slow rotation. With the solution it is possible to gauge the rotation of 360° when we know the number of the magnetic poles on the circumference of the wheel and when we sum up the course of the poles past the sensors. The gauging system will make rather complex.
  • Figure 1 shows a permanent magnet and the Hall sensors in its field
  • Figure 2 shows voltage signals coming from the Hall sensors by functions of the rotational position
  • Figure 3 shows the voltage signal of the sensor 1 by an ascending output
  • Figure 4 shows the block diagram of the gauging system
  • Figure 4a shows an ascending transmitting signal
  • Figure 5 shows the placing of the magnetic field and the sensors by the gauging instrument.
  • Figure 1 shows a permanent magnet 4 that has the poles N and S, and that generates a magnetic field round itself.
  • the magnetic field flux is represented by the lines of force 3.
  • the sensor 2 is in out-of-phase of approximately 90° in relation to the sensor 1.
  • the phase displacement can be selected between 80° and 160° in this method.
  • the sensor arrangement shown in the figure 1 is viewed so that the sensors 1 and 2 are in their positions and the magnet 4 is rotating parallel with the figure.
  • the magnet 4 is attached for example to a rotating axle.
  • the Hall sensor 1 In the position shown in the figure 1 the Hall sensor 1 is in the strongest field and gives a maximum output. The field by the sensor 2 is lower.
  • Figure 2 graphically shows the voltage signals 5 and 6 emitted by the sensors 1 and 2 by a function of the swing angle of the magnet 4.
  • the voltage signals are generated in a way that conforms to the invention by using normal Hall sensors to indicate the magnetic field strength.
  • This way to carry out the gauging process includes a calibration circuit of the sensor 1 in which the voltage signal of the sensor 1 is calibrated between Uz and Ux volt. In an advantageous form of performance Uz is 1 V and Ux is 2,5 V. In the position shown in the figure 1 , as the pole N of the magnet 4 is in the strongest field by the sensor 1 , the voltage signal 5 is calibrated into value Ux.
  • the voltage signal 6 emitted by the sensor 2 is calibrated to the voltage value Ux in that angle position of the magnet 4 where the signal of the sensor 1 has its maximum value Ux, and in that angle position where the voltage signal of the sensor 1 has the value Uz.
  • the former angle position is 180° and the latter one is 360°. This is possible as the voltage signal of the sensor 2 is amplified by its maximum value higher than Ux. For the value Uy is regulated just the best approximately 1 ,2 Ux.
  • the curve 6 then intersects the voltage level Ux by the angle values 180 s , 360°, 540° etc. So, the gauging equipment indicates the processed voltage signals 5 and 6 coming from the sensors 1 and 2 as shown in the figure 2 while the magnet 4 is rotating.
  • Figure 3 shows the inverting of the voltage signal 5 of the sensor 1 conforming to the invention. This way to carry out the gauging process discovers the voltage signal 5 of the sensor 1 while the magnet 4 is rotating and the voltage of the signal is passing the maximum voltage value Ux. By help of the calibration circuit it is found out if the amplified voltage 6 of the sensor 2 exceeds the value Ux. If so, the magnet 4 rotates towards a higher angle value as the figure 2 shows, that is, in the figure 1 the magnet 4 rotates clockwise from the initial position.
  • the inverter inverts the curve 5 in this respect 180 s round the voltage axis Ux to a curve 5'.
  • the inverting is carried out in the whole angular area 180 s - 360 s irrespective of which direction of rotation the area is reached from.
  • the frequency selected is just fast enough, for example 0 - 20 kHz, it is possible to get an accurate signal curve according to the figure 3 also of the quick rotation.
  • the signal in the area of full revolution can also be a descending one, like in the situation in which the magnet 4 is rotating in another direction.
  • Inverting of the curve 5 stops by the angle values 0 s , 360 s , 720 s etc while the magnet is rotating clockwise because Uy is lower than Ux.
  • the inverting begins by these angle values when the magnet 4 begins to rotate anti-clockwise, for Uy is then higher than Ux.
  • the inverting stops in anti-clockwise rotation by the angle values like 540 s and 180 s .
  • Inverting of the curve 5 (comparison Uy higher than Ux) is viewed while passing the maximum point of the curve 5 in either direction.
  • the corresponding angle values in the figure 2 are for example 180 s , 540 s etc.
  • inverting of the curve 5 is viewed while passing the Uz point of the curve 5 from either direction, too.
  • the corresponding angle values in the figure 2 are for example 0 s , 360 s , 720 s etc.
  • Figure 4 shows a way to carry out the gauging process in the form of a block diagram. It includes a part 4 that generates a magnetic field and a part 19 that gauges the magnetic field strength and consists of the Hall sensors 1 and 2.
  • the part 4 is attached to the part to be gauged like to an axle, and it rotates with the axle in the first or second direction.
  • the block 14 there is an analog switch by which is selected, controlled by the comparator, if the signal inverted by the inverter 10 or the uninverted signal before the inverter is taken to be processed.
  • the inverted signal is selected by the switch 14, if the voltage condition from the comparator 13 Uy is higher than Ux is met.
  • To the comparator 13 comes a voltage from the sensor 2 and a voltage reference from the block 12 (comparison Ux/Uy).
  • the signal of the sensor 1 comes via an amplifier 9 into the block 14, and the inverter 10 inverts the signal.
  • a revolution counter, a frequency counter or a rotational speed counter is added to the block diagram if the part to be gauged rotates more than 360° or if it is for example a rotating axle.
  • Figure 5 shows an application attached to the gauging instrument.
  • a magnetic field generator 4 according to the invention, and a part 19 with the sensors 1 and 2 gauging the strength of the field.
  • the part 19 is placed round the magnet 4.
  • the sensors 1 and 2 indicate the rotation of the axle of the analog gauge 20, and the corresponding signals are transmitted through a cable 18 to the gauging equipment that conforms to the invention.
  • the part 19 was made into a ring to protect the sensors 1 and 2. The ring is easily to be attached round the generating instruments of the magnetic field.
  • the invention can be modified in many ways within the inventive idea specified in the patent claims.
  • the method and the equipment can be adapted to indicate and gauge slow or quick rotation, as well as to slow or quick swinging motions. This can be done by a graphic curve for example according to the figure 3, or by an angle value, and the number and speed of the revolutions can be indicated by the rotary motion.

Landscapes

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

Abstract

A method and an equipment to gauge rotary motion in which the device sampling the rotation of the part to be gauged includes a part (4) that generates a magnetic field, and a part (19) placed in the magnetic field mentioned which has at least the first (1) and the second (2) sensor gauging the field strength with the result that the parts (4 and 19) are rotating in relation to each other when the part to be gauged is rotating. The information on the magnetic field strength emitted by the first sensor is processed by voltage information in the unit of measurement. The maximum value of this information is registered to mark a certain angle position of the rotation. The information on the magnetic field strength emitted by the second sensor is processed by amplified voltage information in the unit of measurement. When the voltage information of the first sensor passes the maximum voltage point (Ux) and when the amplified voltage information of the second sensor exceeds (Ux), the unit of measurement inverts the voltage figure of the first sensor 180° round the voltage axis (Ux) to produce an ascending voltage signal per a full revolution in the first direction.

Description

METHOD AND APPARATUS FOR MEASURING ROTATION MOTION
The invention is concerned with the method that conforms to the introduction of the patent claim 1 and with the equipment that conforms to the introduction of the patent claim 8 to gauge rotary motion.
In the US patent 5,130,650 we already know the identification of the angle position in rotating axle where plenty of magnetic poles are placed on the axle circle as segments so that half of the poles are positive and half are negative, and together they form a bipolar ring. Two sensors identifying the magnetic field strength are placed outside the ring at an angle of 90Q in relation to each other. Both sensors give a piece of continuously changing information on the magnetic field strength while the axle is rotating. The signals are simple sinusoidal. By using two sensors the signals are of form S1 =fcosα and S2=fsin . The signals can be processed by using a well-known electronic system whereupon the angle value is numeric.
A disadvantage of this solution is generating a magnetic field. Separate magnets ought to have the same strength and they ought to be in a segmental form filling the circumference of the circle. Besides, the gauging instrument must work out arithmetical operations to find out the angle value. The solution is not adapted for example for a quick regulating of the angle position of the axle where the axle must be stopped in a predetermined angle position, go immediately to a new position etc.
In the US patent 5,241 ,267 we know an identification of rotary motion to reach a high degree of accuracy. The identifier has a rotating axle with a wheel or a corresponding element on which circumference there are poles with positive and negative magnets alternately in large numbers. While the axle is rotating, the magnets are passing the three Hall sensors placed one after another in the direction of rotation. Each sensor gives a variable signal output. By combining the sensor outputs it is possible to double the output frequency and to improve the accuracy. The Hall sensors can be advantageously manufactured as one component.
A disadvantage of the US patent 5,241 ,267 is a need of a multipolar magnetic wheel or ring as well as the fact that the invention is only adapted for gauging slow rotation. With the solution it is possible to gauge the rotation of 360° when we know the number of the magnetic poles on the circumference of the wheel and when we sum up the course of the poles past the sensors. The gauging system will make rather complex.
The meaning of the invention in question is to solve these problems by using only one simple bipolar magnetic field and two sensors that identify the field while the field and the sensors are rotating in relation to each other. To a rotating or swinging axle, of which motion is gauged, is attached either a magnet or sensors. Characteristic of the method and the equipment that conform to the invention is what is presented in the patent claims.
By the method and the equipment that conform to the invention, with a simple magnet and a sensor position, by viewing outputs of two sensors, it is possible to generate an output signal of the rotary motion of the axle to be gauged which is continuously ascending or descending between 0° and 360°. A single output signal unambiguously correspond with each angle value. The axle can rotate in either direction. In continuous rotation there is used a revolution counter to count full revolutions.
The invention is represented below by referring to the enclosed drawings in which
Figure 1 shows a permanent magnet and the Hall sensors in its field Figure 2 shows voltage signals coming from the Hall sensors by functions of the rotational position Figure 3 shows the voltage signal of the sensor 1 by an ascending output Figure 4 shows the block diagram of the gauging system Figure 4a shows an ascending transmitting signal Figure 5 shows the placing of the magnetic field and the sensors by the gauging instrument.
Figure 1 shows a permanent magnet 4 that has the poles N and S, and that generates a magnetic field round itself. The magnetic field flux is represented by the lines of force 3. In the magnetic field there are two Hall sensors 1 and 2. The sensor 2 is in out-of-phase of approximately 90° in relation to the sensor 1. The phase displacement can be selected between 80° and 160° in this method.
The sensor arrangement shown in the figure 1 is viewed so that the sensors 1 and 2 are in their positions and the magnet 4 is rotating parallel with the figure. The magnet 4 is attached for example to a rotating axle. In the position shown in the figure 1 the Hall sensor 1 is in the strongest field and gives a maximum output. The field by the sensor 2 is lower.
Figure 2 graphically shows the voltage signals 5 and 6 emitted by the sensors 1 and 2 by a function of the swing angle of the magnet 4. The voltage signals are generated in a way that conforms to the invention by using normal Hall sensors to indicate the magnetic field strength. This way to carry out the gauging process includes a calibration circuit of the sensor 1 in which the voltage signal of the sensor 1 is calibrated between Uz and Ux volt. In an advantageous form of performance Uz is 1 V and Ux is 2,5 V. In the position shown in the figure 1 , as the pole N of the magnet 4 is in the strongest field by the sensor 1 , the voltage signal 5 is calibrated into value Ux. The magnet
4 being swung 180° and the pole S being by the sensor 1 , the voltage signal
5 is calibrated into the voltage value Uz. After that, while the magnet 4 is rotating in either direction, the signal curve 5 shown in the figure 2 is generated. The voltage signal 6 emitted by the sensor 2 is calibrated to the voltage value Ux in that angle position of the magnet 4 where the signal of the sensor 1 has its maximum value Ux, and in that angle position where the voltage signal of the sensor 1 has the value Uz. The former angle position is 180° and the latter one is 360°. This is possible as the voltage signal of the sensor 2 is amplified by its maximum value higher than Ux. For the value Uy is regulated just the best approximately 1 ,2 Ux. The curve 6 then intersects the voltage level Ux by the angle values 180s, 360°, 540° etc. So, the gauging equipment indicates the processed voltage signals 5 and 6 coming from the sensors 1 and 2 as shown in the figure 2 while the magnet 4 is rotating.
Figure 3 shows the inverting of the voltage signal 5 of the sensor 1 conforming to the invention. This way to carry out the gauging process discovers the voltage signal 5 of the sensor 1 while the magnet 4 is rotating and the voltage of the signal is passing the maximum voltage value Ux. By help of the calibration circuit it is found out if the amplified voltage 6 of the sensor 2 exceeds the value Ux. If so, the magnet 4 rotates towards a higher angle value as the figure 2 shows, that is, in the figure 1 the magnet 4 rotates clockwise from the initial position.
The situation being this, the inverter inverts the curve 5 in this respect 180s round the voltage axis Ux to a curve 5'. The inverting is carried out in the whole angular area 180s - 360s irrespective of which direction of rotation the area is reached from. When the frequency selected is just fast enough, for example 0 - 20 kHz, it is possible to get an accurate signal curve according to the figure 3 also of the quick rotation.
Thus, in the angular area 180s - 360s there appears on each revolution an inverted curve 5', and in the area of full revolution there appears an ascending voltage signal. Analogously, the signal in the area of full revolution can also be a descending one, like in the situation in which the magnet 4 is rotating in another direction. Inverting of the curve 5 stops by the angle values 0s, 360s, 720s etc while the magnet is rotating clockwise because Uy is lower than Ux. However, the inverting begins by these angle values when the magnet 4 begins to rotate anti-clockwise, for Uy is then higher than Ux. Analogously, the inverting stops in anti-clockwise rotation by the angle values like 540s and 180s.
Inverting of the curve 5 (comparison Uy higher than Ux) is viewed while passing the maximum point of the curve 5 in either direction. The corresponding angle values in the figure 2 are for example 180s, 540s etc.
inverting of the curve 5 is viewed while passing the Uz point of the curve 5 from either direction, too. The corresponding angle values in the figure 2 are for example 0s, 360s, 720s etc.
By means of this way to carry out the gauging process we get an unambiguous ascending or descending voltage figure 5, 5' from the rotation of the magnet 4 per each full revolution. The voltage curve can also be linearized into a graph 7 simply by using well-known methods. Transforming the voltage signal further for example into a numeric angle value is well- known technology in itself.
Figure 4 shows a way to carry out the gauging process in the form of a block diagram. It includes a part 4 that generates a magnetic field and a part 19 that gauges the magnetic field strength and consists of the Hall sensors 1 and 2. The part 4 is attached to the part to be gauged like to an axle, and it rotates with the axle in the first or second direction. For the sensor 1 there is calibration in the block 8 into a maximum value Ux. For the sensor 2 there is calibration in the block 11 into the values Ux by the angle values 180s and 360s.
In the block 14 there is an analog switch by which is selected, controlled by the comparator, if the signal inverted by the inverter 10 or the uninverted signal before the inverter is taken to be processed. The inverted signal is selected by the switch 14, if the voltage condition from the comparator 13 Uy is higher than Ux is met. To the comparator 13 comes a voltage from the sensor 2 and a voltage reference from the block 12 (comparison Ux/Uy).
The signal of the sensor 1 comes via an amplifier 9 into the block 14, and the inverter 10 inverts the signal. The inverted or uninverted signal selected by the switch 14 is transferred via a buffer 15 to a convertor from where a signal concerning a full revolution can move on after being modified and linearized, too, if required, by an ascending or descending voltage signal or, as represented in the figure 4a, by an ascending current signal for example l=24 - 40 mV (corresponding 0s - 360s).
A revolution counter, a frequency counter or a rotational speed counter is added to the block diagram if the part to be gauged rotates more than 360° or if it is for example a rotating axle.
Figure 5 shows an application attached to the gauging instrument. In the application there are a magnetic field generator 4 according to the invention, and a part 19 with the sensors 1 and 2 gauging the strength of the field. The part 19 is placed round the magnet 4. The sensors 1 and 2 indicate the rotation of the axle of the analog gauge 20, and the corresponding signals are transmitted through a cable 18 to the gauging equipment that conforms to the invention. The part 19 was made into a ring to protect the sensors 1 and 2. The ring is easily to be attached round the generating instruments of the magnetic field.
The invention can be modified in many ways within the inventive idea specified in the patent claims. The method and the equipment can be adapted to indicate and gauge slow or quick rotation, as well as to slow or quick swinging motions. This can be done by a graphic curve for example according to the figure 3, or by an angle value, and the number and speed of the revolutions can be indicated by the rotary motion.

Claims

PATENT CLAIMS
1. A method to indicate or gauge a swing angle or rotation in the first or second direction. The device sampling the rotation of the part to be gauged consists of a part (4) that generates a magnetic field, and a part (19) placed in the magnetic field mentioned which includes the first sensor (1 ) gauging the magnetic field (3) strength, and the second sensor (2) which is out-of- phase with the first sensor. Then the parts (4) and (19) are rotating in relation to each other while the part to be gauged is rotating, and from the sensors mentioned in the method are transmitted the intensity signals of the magnetic field (3) to the unit of measurement which processes the signals and by help of them indicates swing or rotary motion of the part to be gauged, is k n o w n for the property that
- the information of the magnetic field (3) strength emitted by the first sensor (1 ) is processed in the unit of measurement by a piece of voltage information (5), of which maximum value (Ux) and minimum value (Uz) are registered to mark certain angle positions of the rotation,
- the information of the magnetic field (3) strength emitted by the second sensor (2) is processed in the unit of measurement by a piece of amplified voltage information (6) compared to the previous one, of which voltage of the maximum value (Uy) is defined essentially higher than (Ux),
- while the voltage information of the first sensor (1) is passing the maximum voltage point (Ux) or the minimum voltage point (Uz), the amplified voltage information (6) of the second sensor (2) is discovered. When the value of the amplified voltage information is higher than (Ux), the unit of measurement inverts the voltage figure of the first sensor (1 ) 180s round the voltage axis (Ux) to create an ascending or descending voltage signal per a full revolution in the first direction.
2. The method in accordance with the patent claim 1 is k n o w n for the property that by passing the maximum voltage value (Ux) of the first sensor (1 ) the value of the amplified voltage information of the second sensor (2) being lower than (Ux) indicates that the direction of rotation of the part to be gauged is opposite in relation to the first direction.
3. The method in accordance with the patent claims 1 and 2 is k n o w n for the property that the first (1 ) and the second (2) sensors are out-of-phase between 80s and 160s, just best between 90s and 110s, and the amplified voltage information of the second sensor is calibrated into the value (Ux) when the first sensor emits the maximum value (Ux) and the minimum value (Uz).
4. The method in accordance with some of the previous patent claims 1 - 3 is k n o w n for the property that the signals of the sensors (1 ) and (2) are indicated by positive voltage values between (Uz - Ux) and (Uz - Uy).
5. The method in accordance with some of the previous patent claims 1 - 4 is k n o w n for the property that the minimum value (Uz) of the voltage (5) corresponds with the angle position 0s and the maximum value (Ux) corresponds with the angle position 180s.
6. The method in accordance with some of the previous patent claims 1 - 5 is k n o w n for the property that the voltage signal (6) of the second sensor (2) is amplified 15 - 30% higher by its maximum value than the signal (Ux) of the first sensor.
7. The method in accordance with some of the previous patent claims 1 - 4 is k n o w n for the property that the unit of measurement generates a voltage signal per revolution of the part to be gauged, possibly linearizes the signal (7) and the number of full revolutions is discovered by help of the revolution counter attached to the unit of measurement.
8. An equipment to gauge or indicate rotary motion or the swing angle in the first or second direction whereupon the device sampling the rotation of the part to be gauged includes a part (4) that generates a magnetic field and a part (19) placed in the magnetic field mentioned. The part (19) consists of at least the first sensor (1 ) that gauges the magnetic field (3) strength, and the second sensor (2) that is out-of-phase with the first sensor, whereupon the parts (4) and (19) are rotating in relation to each other while the part to be gauged is rotating and whereupon the strength signals of the magnetic field (3) are transmitted to the unit of measurement which processes the signals, and by help of them indicates the rotary and swinging motion of the part to be gauged, is k n o w n for the property that the equipment includes
- an amplifier (9) that amplifies the voltage information (6) on the same magnetic field (3) strength emitted by the second sensor (2) essentially higher than the voltage information of the first sensor,
- an inverter (10) that inverts the voltage information of the first sensor (1 ) in relation to the voltage axis (Ux) (fig. 3) while the voltage information of the sensor (1 ) is passing the maximum value (Ux) or the minimum value (Uz) if the voltage information (6) of the second sensor (2) is higher than (Ux),
- a convertor (16) to indicate the rotational position of the part to be gauged in the area of full revolution by an ascending or descending voltage value (5,5') or (7), or by an ascending or descending current value (17).
9. The equipment in accordance with the patent claim 8 is k n o w n for the property that the minimum voltage information (Uz) of the first sensor (1 ) is regulated to correspond with the rotational angle value 0s, 360s etc and the maximum voltage information (Ux) is regulated to correspond with the angle value 180s, 540s etc.
10. The equipment in accordance with the patent claim 8 and 9 is k n o w n for the property that the sensors (1 and 2) are placed in a ring-shaped part (19), and the part is attached round the axle to be gauged or a corresponding element at the point where the generating instruments (4) of the magnetic field are situated.
PCT/FI1997/000519 1996-03-05 1997-09-04 Method and apparatus for measuring rotation motion WO1999011999A1 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
FI961010A FI103215B1 (en) 1996-03-05 1996-03-05 Method and apparatus for measuring rotational motion
PCT/FI1997/000519 WO1999011999A1 (en) 1996-03-05 1997-09-04 Method and apparatus for measuring rotation motion

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
FI961010A FI103215B1 (en) 1996-03-05 1996-03-05 Method and apparatus for measuring rotational motion
PCT/FI1997/000519 WO1999011999A1 (en) 1996-03-05 1997-09-04 Method and apparatus for measuring rotation motion

Publications (1)

Publication Number Publication Date
WO1999011999A1 true WO1999011999A1 (en) 1999-03-11

Family

ID=26160130

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/FI1997/000519 WO1999011999A1 (en) 1996-03-05 1997-09-04 Method and apparatus for measuring rotation motion

Country Status (1)

Country Link
WO (1) WO1999011999A1 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2011004120A2 (en) 2009-07-07 2011-01-13 Moving Magnet Technologies (Mmt) Multi-periodic absolute position sensor
US8970210B2 (en) 2009-11-06 2015-03-03 Moving Magnet Technologies (Mmt) Bidirectional magnetic position sensor having field rotation
US10041780B2 (en) 2010-09-29 2018-08-07 Moving Magnet Technologies (Mmt) Position sensor

Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0059763A1 (en) * 1980-09-22 1982-09-15 Fanuc Ltd. D.c. generator type non-contact speed sensing device
GB2169085A (en) * 1984-12-19 1986-07-02 Risto Tanner Direction indicating apparatus
US4703261A (en) * 1983-12-15 1987-10-27 Maag Gear-Wheel And Machine Company Limited Differential Hall-effect gear measure feeler
US4791366A (en) * 1985-10-31 1988-12-13 Alpine Electronics Inc. Apparatus including a pair of angularly spaced sensors for detecting angle of rotation of a rotary member
US4829248A (en) * 1984-09-20 1989-05-09 Loubier Robert J Hall effect sensing apparatus and method
DE3919926A1 (en) * 1989-06-19 1990-12-20 Vdo Schindling METHOD FOR DETERMINING THE ABSOLUTE POSITION OF A POINTER IN A DISPLAY DEVICE AND DISPLAY DEVICE
EP0729011A1 (en) * 1995-02-22 1996-08-28 Mikuni Corporation Magnetic position sensor

Patent Citations (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0059763A1 (en) * 1980-09-22 1982-09-15 Fanuc Ltd. D.c. generator type non-contact speed sensing device
US4703261A (en) * 1983-12-15 1987-10-27 Maag Gear-Wheel And Machine Company Limited Differential Hall-effect gear measure feeler
US4829248A (en) * 1984-09-20 1989-05-09 Loubier Robert J Hall effect sensing apparatus and method
GB2169085A (en) * 1984-12-19 1986-07-02 Risto Tanner Direction indicating apparatus
US4791366A (en) * 1985-10-31 1988-12-13 Alpine Electronics Inc. Apparatus including a pair of angularly spaced sensors for detecting angle of rotation of a rotary member
DE3919926A1 (en) * 1989-06-19 1990-12-20 Vdo Schindling METHOD FOR DETERMINING THE ABSOLUTE POSITION OF A POINTER IN A DISPLAY DEVICE AND DISPLAY DEVICE
EP0729011A1 (en) * 1995-02-22 1996-08-28 Mikuni Corporation Magnetic position sensor

Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2011004120A2 (en) 2009-07-07 2011-01-13 Moving Magnet Technologies (Mmt) Multi-periodic absolute position sensor
FR2947902A1 (en) * 2009-07-07 2011-01-14 Moving Magnet Technologies M M T ABSOLUTE AND MULTI-PERIODIC POSITION SENSOR
WO2011004120A3 (en) * 2009-07-07 2011-12-01 Moving Magnet Technologies (Mmt) Multi-periodic absolute position sensor
KR20120049250A (en) * 2009-07-07 2012-05-16 무빙 마그네트 테크놀로지스 Multi-periodic absolute position sensor
CN102472642A (en) * 2009-07-07 2012-05-23 移动磁体技术公司 Multi-cycle absolute position sensor
US8890514B2 (en) 2009-07-07 2014-11-18 Moving Magnet Technologies (Mmt) Magnetic multi-periodic absolute position sensor
CN102472642B (en) * 2009-07-07 2015-08-19 移动磁体技术公司 Multi-periodic absolute position sensor
KR101721087B1 (en) 2009-07-07 2017-03-29 무빙 마그네트 테크놀로지스 Multi-periodic absolute position sensor
US8970210B2 (en) 2009-11-06 2015-03-03 Moving Magnet Technologies (Mmt) Bidirectional magnetic position sensor having field rotation
US10041780B2 (en) 2010-09-29 2018-08-07 Moving Magnet Technologies (Mmt) Position sensor

Similar Documents

Publication Publication Date Title
EP3385678B1 (en) Rotary position sensor
US6229299B1 (en) System and method for computing the angular velocity and direction of a rotational body
US4924180A (en) Apparatus for detecting bearing shaft wear utilizing rotatable magnet means
US5742160A (en) Apparatus for determining angular position and rotational speed using a rotating magnet and a directional magnetometer
US11984837B2 (en) Method for determining an angular position of a rotating component, in particular of an electric motor for a clutch actuation system of a vehicle
CA2476464A1 (en) Methods and apparatus for sensing angular position of a rotatable shaft
US5038607A (en) Wind speed and wind direction signal generator
JP5288320B2 (en) Apparatus and method for measuring rotational balance of high-speed rotating body
EP0375019A1 (en) Device for detecting the movement of a part
US4762007A (en) Torque measuring apparatus
EP0716306A2 (en) Shaft rotation sensor with spaced directional magnetic sensors and method
JP2004223511A (en) Unbalance dynamic load generator
CN106871850A (en) Angle measurement unit and the method for operation angle measurement apparatus
WO1999011999A1 (en) Method and apparatus for measuring rotation motion
CN208937345U (en) Machine test rack console
GB2497721A (en) Calibrating a drive system for a motor
EP3875913A1 (en) Hybrid position sensor
JP4243902B2 (en) A turntable acceleration generating apparatus provided with a method for estimating an eccentric position of an acceleration sensor and an eccentricity adjusting function in the turntable acceleration generating apparatus.
JPH0618339A (en) Measuring device for braking torque generated by electromagnetic retarder and torque adjusting device
EP0882943A1 (en) "Device for determining a momentary angular position"
US11512980B2 (en) Absolute position detection device and detection method of rotating body
ATE267387T1 (en) ROTATION ANGLE SENSOR
JP2024502666A (en) Non-contact position sensor with permanent magnet, measuring device, application method of non-contact position sensor
CN219736414U (en) Single-turn absolute value magnetic encoder
EP0606942A1 (en) Angular speed and position measuring device and method

Legal Events

Date Code Title Description
AK Designated states

Kind code of ref document: A1

Designated state(s): US

AL Designated countries for regional patents

Kind code of ref document: A1

Designated state(s): AT BE CH DE DK ES FI FR GB GR IE IT LU MC NL PT SE

121 Ep: the epo has been informed by wipo that ep was designated in this application
DFPE Request for preliminary examination filed prior to expiration of 19th month from priority date (pct application filed before 20040101)
WWE Wipo information: entry into national phase

Ref document number: 1997940170

Country of ref document: EP

WWW Wipo information: withdrawn in national office

Ref document number: 1997940170

Country of ref document: EP

NENP Non-entry into the national phase

Ref country code: CA

122 Ep: pct application non-entry in european phase