US20020074995A1 - Increased output variable reluctance sensor . - Google Patents
Increased output variable reluctance sensor . Download PDFInfo
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- US20020074995A1 US20020074995A1 US09/742,517 US74251700A US2002074995A1 US 20020074995 A1 US20020074995 A1 US 20020074995A1 US 74251700 A US74251700 A US 74251700A US 2002074995 A1 US2002074995 A1 US 2002074995A1
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01D—MEASURING 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
- G01D5/00—Mechanical 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
- G01D5/12—Mechanical 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
- G01D5/14—Mechanical 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
- G01D5/20—Mechanical 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
- G01D5/2006—Mechanical 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 self-induction of one or more coils
- G01D5/2013—Mechanical 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 self-induction of one or more coils by a movable ferromagnetic element, e.g. a core
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01P—MEASURING LINEAR OR ANGULAR SPEED, ACCELERATION, DECELERATION, OR SHOCK; INDICATING PRESENCE, ABSENCE, OR DIRECTION, OF MOVEMENT
- G01P3/00—Measuring linear or angular speed; Measuring differences of linear or angular speeds
- G01P3/42—Devices characterised by the use of electric or magnetic means
- G01P3/44—Devices characterised by the use of electric or magnetic means for measuring angular speed
- G01P3/48—Devices characterised by the use of electric or magnetic means for measuring angular speed by measuring frequency of generated current or voltage
- G01P3/481—Devices characterised by the use of electric or magnetic means for measuring angular speed by measuring frequency of generated current or voltage of pulse signals
- G01P3/488—Devices 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 variable reluctance detectors
Definitions
- This invention relates to a variable reluctance sensor. More specifically, this invention relates to a reluctance sensor which enhances low output signals by reducing magnetic flux leakage.
- a common type of sensor used in automotive components is a variable reluctance sensor which functions by sensing the change in reluctance from a ferrous target as the air gap between the sensor and the target changes. This is usually accomplished by cutting slots in the target and passing it by the sensor.
- a variable reluctance sensor is used because it is rugged and is of relatively low cost.
- the variable reluctance sensor typically has a pole piece with a coil of wire.
- a magnet is located in the sensor and generates a magnetic field in the coil.
- the target object is a ferrous material such as steel or iron whose movement effects the flux within the coil generated by the magnet.
- a target object may be a gear whose teeth are in proximity to the variable reluctance sensor.
- the reluctance is measured from the pole piece or magnet and is proportional to the distance from the target object.
- the magnet may either be in the front of the pole or the rear of the pole piece.
- Another configuration is having a stacked magnetic material forming a rectangular pole piece having alternating ferrous and magnetic material. The reluctance change on one end of the stack also changes the flux paths in the other end which creates the voltage change in the coil.
- the output of the variable reluctance sensor depends on the rate of change of magnetic flux in the coil.
- the voltage generated by the coil is proportional to the number of turns in the coil. Given the air gap between the pole piece and the target object as well as magnetic paths through the pole piece and other sensor assembly, some of the magnetic flux leaks and does not affect the coil. Generally, it is desirable to have a higher voltage output for easier reading of the sensor output. Thus, the more leakage of magnetic field flux, the lower the voltage output. At low speeds of the target object, lower rate of change of flux is generated in the coil, which combined with inherent leaks, results in a lower voltage output from the sensor.
- the present reluctance sensors may be enhanced in order to increase low voltage output.
- added ferrous paths may be created by providing additional pole pieces near the target object.
- the additional pole pieces allow the capture of additional flux thus increasing overall voltage output.
- these modifications add cost and complexity to the system, nullifying the advantages of the variable reluctance sensor.
- the present invention may be embodied in a variable reluctance sensor for determining the position of a moveable target object.
- the sensor has a magnet and a pole piece coupled to the magnet.
- a wire coil is located annularly around the pole piece.
- a second bucking magnet is annularly located around the coil which generates a flux field.
- a control unit is coupled to the wire coil which measures the sinusoidal signal generated in the coil from the movement of the target object.
- the present invention may also be embodied in a method of increasing the voltage output from a variable reluctance sensor.
- the sensor has a pole piece, a coil located annularly around the pole piece, and a magnet.
- a bucking magnet is added around the coil to produce flux to cancel leaking flux from the sensor to increase coil voltage output.
- FIG. 1 is a perspective view of a variable reluctance sensor according to one embodiment of the present invention.
- FIG. 2 is an exploded perspective view of the variable reluctance sensor of FIG. 1
- FIG. 3 is cross sectional flux diagram of the magnetic fields surrounding the variable reluctance sensor in FIG. 1 without the addition of bucking magnets.
- FIG. 4 is cross sectional flux diagram of the magnetic fields surrounding the variable reluctance sensor in FIG. 1 with the addition of bucking magnets.
- FIG. 5 is a circuit diagram model of the variable reluctance sensor according to one embodiment of the present invention.
- FIG. 6 is a graph of the output of the variable reluctance sensor with the placement of the bucking magnets according to the present invention in comparison with a standard variable reluctance sensor.
- FIG. 7 is a circuit schematic of a control circuit used by the variable reluctance sensor according to one embodiment of the present invention.
- FIG. 8 is a cross sectional flux diagram of a second variable reluctance sensor.
- FIGS. 1 - 4 show a perspective, exploded perspective and cross sectional views of a variable reluctance sensor generally indicated at 10 , embodying the general principles of the present invention.
- the variable reluctance sensor 10 senses the rotation of a target object 12 .
- the target object must be made of a ferrous material such as steel and may move in a linear or angular motion relative to the variable reluctance sensor 10 .
- the target object 12 in this example is a gear and the sensor 10 detects the rotation of the gear.
- any rotational or linear movement device may be used with the sensor 10 .
- the target object 12 which is sensed by the sensor 10 is typically rotated around an axis (not shown) to insure strict angular movement.
- the outputs of the sensor 10 are coupled to a control system 14 .
- the sensor 10 has a disk shaped magnet 16 which is coupled to a pole piece 18 .
- the pole piece has a proximal end which is close to the target object 12 and a distal end. There is an air gap between the proximal end of the pole piece 18 and the target object 12 .
- the pole piece 18 has a platter 20 which is located on the distal end of the pole piece 18 and supports the magnet 16 .
- the pole piece 18 is a ferrous material and has a wire coil 22 which is coupled to the control system 14 . It is to be understood that the magnet 16 may be located in any appropriate location to generate a magnetic field within the coil 22 . For example, the magnet 16 may be located on a platter on the proximal end of the pole piece 18 .
- a circular covering 24 is located over the coil 22 to protect the coil 22 .
- the circular covering 24 is typically an insulator material such as plastic.
- Two pairs of bucking magnets 26 and 28 are coupled around the coil 22 .
- a single ring magnet with one pole on the inside of the ring and another pole on the outside could be used for the magnets 26 and 28 .
- the target object 12 moves rotationally and has a series of gear teeth 30 . Since the target object 12 is metal, its movement changes the flux in the wire coil 22 .
- FIG. 3 is a cross section of the sensor 10 .
- the flux generates a voltage output from the coil 22 which is coupled to the control system 14 .
- FIG. 3 models the magnetic flux lines without the bucking magnets 26 and 28 .
- a series of flux lines 32 are leaking from the pole piece 18 and the coil 22 .
- the leaking flux reduces the electrical output measurable from the coil 22 .
- the leaking flux thus significantly affects the output at low speeds of the target object 12 because the generated flux change is proportional to the speed of the target object 12 and thus is low to begin with.
- FIG. 4 is a flux diagram of the sensor 10 in FIG. 1 with the bucking magnets 26 and 28 .
- the movement of the target object 12 shapes a magnetic field in the coil 22 with a series of flux lines.
- the bucking magnets 26 and 28 force the flux from the magnetic field to travel through the pole piece 18 and the coil 22 .
- the bucking magnets 26 and 28 thus prevent leaking of the flux from the pole piece 18 and therefore increase the flux change and ultimate voltage from the coil 22 .
- FIG. 5 shows an electrical circuit representation 58 of the interaction between the coil 22 and the target object 12 in FIGS. 1 - 4 .
- the target object 12 is represented by a target resistor 60 .
- the gap between the target object 12 and the sensor 10 is modeled by an air gap resistor 62 .
- the flux leaking from the end of the pole 18 opposite the platter 20 is represented by a resistor 64 while the flux leaking from the pole 18 to the coil 22 is represented by a resistor 66 .
- Two resistors 68 and 70 are in parallel and represent the flux leaks from the platter 20 and the magnet 16 .
- the pole piece 18 is represented by two resistors 72 and 74 which create a voltage drop representing the flux generated in the coil 22 ultimately detected by the control circuit 14 .
- the platter 20 is represented by a resistor 76 .
- the magnet 16 is represented by a voltage source 78 .
- the current in the circuit diagram 58 represents the flux.
- the bucking magnets 26 and 28 create flux which replaces the leakage flux and enhances the flux generated in the coil.
- the bucking magnets 26 and 28 are modeled as voltage sources 80 and 82 which are in series with the resistors 72 and 74 . Using the electrical model, additional voltage sources result in greater outputs.
- the increase in current as a result of the voltage sources 80 and 82 on the resistors 64 and 66 results in greater voltage/flux across the resistors 72 and 74 .
- the elimination of the leakage flux and the addition of the flux from the two bucking magnets 26 and 28 thus increases the reluctance output.
- the bucking magnets 26 and 28 may be increased in length to optimize the cancellation of flux leakage. Additionally, the length of the bucking magnets 26 and 28 may be altered to produce the largest voltage output for a selected target and air gap configuration.
- FIG. 6 is a voltage graph 100 representing the voltage outputs from the coil 22 in FIG. 1.
- a bottom trace 102 represents the voltage output of the sensor 10 without the bucking magnets 26 and 28 .
- a top trace 104 represents the voltage output of the coil 22 with bucking magnets 26 and 28 . As may be seen, the flux leakage is reduced and the corresponding voltage is higher resulting in a more usable sensor.
- FIG. 7 is a schematic of the control circuit 14 which receives an output from the coil 22 of the sensor 10 .
- the motion of the target object 12 generates a sinusoidal signal 18 from the coil 22 as the magnetic flux changes due to the velocity of the target object 12 .
- the outputs of the sensor 10 are coupled to a zero detection circuit 110 which detects the time when the sinusoidal signal crosses zero in order to determine the frequency of the signal which is proportional to the speed of the target. It is to be understood that any other appropriate circuit may be used to detect changes in the flux. For example, a peak detection circuit may be used instead of the zero crossing detection circuit 110 .
- the zero crossing detection circuit 110 has an input 112 which is coupled to the output of the sensor 10 .
- a diode 114 clips the negative part of the voltage signal.
- the input 112 is coupled to the negative input of an operational amplifier 116 .
- the positive input of the operational amplifier 116 is coupled to a reference resistor 118 .
- Another resistor 120 is coupled to a voltage source 122 .
- the resistor 120 and resistor 118 provide a reference level voltage to compare the negative input of the operational resistor 118 .
- the output of the operational amplifier 116 therefore goes high when the negative input is higher than the reference voltage indicating a zero crossing point.
- the output of the operational amplifier 116 is coupled to a micro-controller 124 .
- the micro-controller 124 may be any specific, dedicated controller or a programmable microprocessor, application specific integrated circuit (ASIC) or any other comparable circuit.
- the micro-controller 124 processes the output of the operational amplifier 116 by reading the number of high pulses in a certain time period indicating the frequency of the teeth 30 detected by the sensor 10 and therefore the position or speed of the target object 12 .
- the micro-controller 124 uses this data to control devices.
- the micro-controller 124 is coupled to a transmission shift assembly 126 .
- the micro-controller 124 will activate the transmission shift assembly when the target object 12 which determines the transmission shaft speed reaches a certain speed.
- FIG. 8 is a perspective view of a variable reluctance sensor 200 according to the present invention which senses the absolute position of a linearly moving target object 202 .
- the target object is a rod 204 which is attached to the traveling portion of a suspension system 206 .
- the suspension system 206 holds a wheel 208 . By determining the position of the rod 204 , the position of the wheel 208 may be determined for adjustments by the suspension system.
- the outputs of the sensor 200 are coupled to a control system 210 which is identical to the control system 14 described with reference to FIG. 7 above.
- the sensor 200 is similar to the sensor 10 described with reference to FIGS. 1 - 3 above.
- the sensor 200 has a disk shaped magnet 212 which is coupled to a pole piece 214 .
- the pole piece has a proximal end which is close to the target object 202 and a distal end. There is an air gap between the proximal end of the pole piece 214 and the target object 202 .
- the pole piece 214 has a platter 216 which is located on the distal end of the pole piece 214 and supports the magnet 212 .
- the pole piece 214 is a ferrous material and has a wire coil 218 which is coupled to the control system 210 . It is to be understood that the magnet 212 may be located in any appropriate location to generate a magnetic field within the coil 218 .
- a covering 220 is located over the coil 218 to protect the coil 218 .
- the circular covering 218 is typically an insulator material such as plastic.
- Two pairs of magnets 222 and 224 are coupled around the coil 218 .
- the rod 204 is made of a ferrous material such as steel and has a series of teeth 226 . Since the rod 204 is metal, its movement changes the flux in the wire coil 218 by the movement of the teeth 226 relative to the sensor 200 . The flux generated by the movement of the rod 204 generates a voltage output from the coil 218 which is coupled to the control system 210 . The magnets 222 and 224 force the flux from the magnetic field to travel through the pole piece 214 and the coil 218 . The magnets 222 and 224 thus prevent leaking of the flux from the pole piece 214 and therefore increase the flux change and voltage output from the coil 218 .
- the present invention may be employed in any application which requires determination of linear position or rotational position.
- Examples in the automotive field include suspension travel, crankshaft or crankshaft rotation and positioning, wheel speed and transmission shaft speed.
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Abstract
Description
- This invention relates to a variable reluctance sensor. More specifically, this invention relates to a reluctance sensor which enhances low output signals by reducing magnetic flux leakage.
- It is desirable in many applications to determine the precise position or speed of various objects which linearly traverse a defined path or a rotational path. For example, the position or speed of numerous items in the automotive field such as transmission input and output shafts, crankshaft or tone wheels for anti-lock braking systems. A common type of sensor used in automotive components is a variable reluctance sensor which functions by sensing the change in reluctance from a ferrous target as the air gap between the sensor and the target changes. This is usually accomplished by cutting slots in the target and passing it by the sensor.
- A variable reluctance sensor is used because it is rugged and is of relatively low cost. The variable reluctance sensor typically has a pole piece with a coil of wire. A magnet is located in the sensor and generates a magnetic field in the coil. The target object is a ferrous material such as steel or iron whose movement effects the flux within the coil generated by the magnet. For example, a target object may be a gear whose teeth are in proximity to the variable reluctance sensor. The reluctance is measured from the pole piece or magnet and is proportional to the distance from the target object. The magnet may either be in the front of the pole or the rear of the pole piece. Another configuration is having a stacked magnetic material forming a rectangular pole piece having alternating ferrous and magnetic material. The reluctance change on one end of the stack also changes the flux paths in the other end which creates the voltage change in the coil.
- The output of the variable reluctance sensor depends on the rate of change of magnetic flux in the coil. The voltage generated by the coil is proportional to the number of turns in the coil. Given the air gap between the pole piece and the target object as well as magnetic paths through the pole piece and other sensor assembly, some of the magnetic flux leaks and does not affect the coil. Generally, it is desirable to have a higher voltage output for easier reading of the sensor output. Thus, the more leakage of magnetic field flux, the lower the voltage output. At low speeds of the target object, lower rate of change of flux is generated in the coil, which combined with inherent leaks, results in a lower voltage output from the sensor.
- The present reluctance sensors may be enhanced in order to increase low voltage output. For example, added ferrous paths may be created by providing additional pole pieces near the target object. The additional pole pieces allow the capture of additional flux thus increasing overall voltage output. However, these modifications add cost and complexity to the system, nullifying the advantages of the variable reluctance sensor.
- Such corrections also require extra processing for the additional pole pieces which increase the complexity and cost of the device.
- Thus, there exists a need for an increased output reluctance sensor. There is also a need for a reluctance sensor which does not require excessive processing components. There is a further need for a reluctance sensor which provides high output from target objects with low flux levels.
- The present invention may be embodied in a variable reluctance sensor for determining the position of a moveable target object. The sensor has a magnet and a pole piece coupled to the magnet. A wire coil is located annularly around the pole piece. A second bucking magnet is annularly located around the coil which generates a flux field. A control unit is coupled to the wire coil which measures the sinusoidal signal generated in the coil from the movement of the target object.
- The present invention may also be embodied in a method of increasing the voltage output from a variable reluctance sensor. The sensor has a pole piece, a coil located annularly around the pole piece, and a magnet. A bucking magnet is added around the coil to produce flux to cancel leaking flux from the sensor to increase coil voltage output.
- It is to be understood that both the foregoing general description and the following detailed description are not limiting but are intended to provide further explanation of the invention claimed. The accompanying drawings, which are incorporated in and constitute part of this specification, are included to illustrate and provide a further understanding of the method and system of the invention. Together with the description, the drawings serve to explain the principles of the invention.
- FIG. 1 is a perspective view of a variable reluctance sensor according to one embodiment of the present invention.
- FIG. 2 is an exploded perspective view of the variable reluctance sensor of FIG. 1
- FIG. 3 is cross sectional flux diagram of the magnetic fields surrounding the variable reluctance sensor in FIG. 1 without the addition of bucking magnets.
- FIG. 4 is cross sectional flux diagram of the magnetic fields surrounding the variable reluctance sensor in FIG. 1 with the addition of bucking magnets.
- FIG. 5 is a circuit diagram model of the variable reluctance sensor according to one embodiment of the present invention.
- FIG. 6 is a graph of the output of the variable reluctance sensor with the placement of the bucking magnets according to the present invention in comparison with a standard variable reluctance sensor.
- FIG. 7 is a circuit schematic of a control circuit used by the variable reluctance sensor according to one embodiment of the present invention.
- FIG. 8 is a cross sectional flux diagram of a second variable reluctance sensor.
- While the present invention is capable of embodiment in various forms, there is shown in the drawings and will hereinafter be described a presently preferred embodiment with the understanding that the present disclosure is to be considered as an exemplification of the invention, and is not intended to limit the invention to the specific embodiment illustrated.
- Referring now to the drawings and more particularly to FIGS. 1-4 which show a perspective, exploded perspective and cross sectional views of a variable reluctance sensor generally indicated at 10, embodying the general principles of the present invention.
- In general, the
variable reluctance sensor 10 senses the rotation of atarget object 12. The target object must be made of a ferrous material such as steel and may move in a linear or angular motion relative to thevariable reluctance sensor 10. Thetarget object 12 in this example is a gear and thesensor 10 detects the rotation of the gear. Of course, it is to be understood that any rotational or linear movement device may be used with thesensor 10. Thetarget object 12 which is sensed by thesensor 10 is typically rotated around an axis (not shown) to insure strict angular movement. - The outputs of the
sensor 10 are coupled to acontrol system 14. Thesensor 10 has a disk shapedmagnet 16 which is coupled to apole piece 18. The pole piece has a proximal end which is close to thetarget object 12 and a distal end. There is an air gap between the proximal end of thepole piece 18 and thetarget object 12. Thepole piece 18 has aplatter 20 which is located on the distal end of thepole piece 18 and supports themagnet 16. Thepole piece 18 is a ferrous material and has awire coil 22 which is coupled to thecontrol system 14. It is to be understood that themagnet 16 may be located in any appropriate location to generate a magnetic field within thecoil 22. For example, themagnet 16 may be located on a platter on the proximal end of thepole piece 18. - A
circular covering 24 is located over thecoil 22 to protect thecoil 22. Thecircular covering 24 is typically an insulator material such as plastic. Two pairs of bucking 26 and 28 are coupled around themagnets coil 22. Alternatively, a single ring magnet with one pole on the inside of the ring and another pole on the outside could be used for the 26 and 28. Themagnets target object 12 moves rotationally and has a series ofgear teeth 30. Since thetarget object 12 is metal, its movement changes the flux in thewire coil 22. - The flux generated by the
magnet 16 and shaped by thetarget object 12 is shown in FIG. 3 which is a cross section of thesensor 10. The flux generates a voltage output from thecoil 22 which is coupled to thecontrol system 14. FIG. 3 models the magnetic flux lines without the bucking 26 and 28. In this case a series ofmagnets flux lines 32 are leaking from thepole piece 18 and thecoil 22. The leaking flux reduces the electrical output measurable from thecoil 22. The leaking flux thus significantly affects the output at low speeds of thetarget object 12 because the generated flux change is proportional to the speed of thetarget object 12 and thus is low to begin with. - The operation of the
sensor 10 will now be explained with reference to FIG. 4 which is a flux diagram of thesensor 10 in FIG. 1 with the bucking 26 and 28. The movement of themagnets target object 12 shapes a magnetic field in thecoil 22 with a series of flux lines. The bucking 26 and 28 force the flux from the magnetic field to travel through themagnets pole piece 18 and thecoil 22. The bucking 26 and 28 thus prevent leaking of the flux from themagnets pole piece 18 and therefore increase the flux change and ultimate voltage from thecoil 22. - FIG. 5 shows an electrical circuit representation 58 of the interaction between the
coil 22 and thetarget object 12 in FIGS. 1-4. Thetarget object 12 is represented by atarget resistor 60. The gap between thetarget object 12 and thesensor 10 is modeled by anair gap resistor 62. The flux leaking from the end of thepole 18 opposite theplatter 20 is represented by a resistor 64 while the flux leaking from thepole 18 to thecoil 22 is represented by aresistor 66. Two 68 and 70 are in parallel and represent the flux leaks from theresistors platter 20 and themagnet 16. - The
pole piece 18 is represented by two 72 and 74 which create a voltage drop representing the flux generated in theresistors coil 22 ultimately detected by thecontrol circuit 14. Theplatter 20 is represented by aresistor 76. Themagnet 16 is represented by avoltage source 78. The current in the circuit diagram 58 represents the flux. Thus, it is beneficial to maximize the voltage measured across the output represented by the 72 and 74. The buckingresistors 26 and 28 create flux which replaces the leakage flux and enhances the flux generated in the coil. The buckingmagnets 26 and 28 are modeled asmagnets 80 and 82 which are in series with thevoltage sources 72 and 74. Using the electrical model, additional voltage sources result in greater outputs. The increase in current as a result of theresistors 80 and 82 on thevoltage sources resistors 64 and 66 results in greater voltage/flux across the 72 and 74. The elimination of the leakage flux and the addition of the flux from the two buckingresistors 26 and 28 thus increases the reluctance output. The buckingmagnets 26 and 28 may be increased in length to optimize the cancellation of flux leakage. Additionally, the length of the buckingmagnets 26 and 28 may be altered to produce the largest voltage output for a selected target and air gap configuration.magnets - The output of the
sensor 10 may be shown in FIG. 6 which is avoltage graph 100 representing the voltage outputs from thecoil 22 in FIG. 1. Abottom trace 102 represents the voltage output of thesensor 10 without the bucking 26 and 28. Amagnets top trace 104 represents the voltage output of thecoil 22 with bucking 26 and 28. As may be seen, the flux leakage is reduced and the corresponding voltage is higher resulting in a more usable sensor.magnets - FIG. 7 is a schematic of the
control circuit 14 which receives an output from thecoil 22 of thesensor 10. The motion of thetarget object 12 generates asinusoidal signal 18 from thecoil 22 as the magnetic flux changes due to the velocity of thetarget object 12. The outputs of thesensor 10 are coupled to a zerodetection circuit 110 which detects the time when the sinusoidal signal crosses zero in order to determine the frequency of the signal which is proportional to the speed of the target. It is to be understood that any other appropriate circuit may be used to detect changes in the flux. For example, a peak detection circuit may be used instead of the zerocrossing detection circuit 110. - The zero
crossing detection circuit 110 has aninput 112 which is coupled to the output of thesensor 10. Adiode 114 clips the negative part of the voltage signal. Theinput 112 is coupled to the negative input of anoperational amplifier 116. The positive input of theoperational amplifier 116 is coupled to areference resistor 118. Anotherresistor 120 is coupled to a voltage source 122. Theresistor 120 andresistor 118 provide a reference level voltage to compare the negative input of theoperational resistor 118. The output of theoperational amplifier 116 therefore goes high when the negative input is higher than the reference voltage indicating a zero crossing point. - The output of the
operational amplifier 116 is coupled to amicro-controller 124. Themicro-controller 124 may be any specific, dedicated controller or a programmable microprocessor, application specific integrated circuit (ASIC) or any other comparable circuit. The micro-controller 124 processes the output of theoperational amplifier 116 by reading the number of high pulses in a certain time period indicating the frequency of theteeth 30 detected by thesensor 10 and therefore the position or speed of thetarget object 12. Themicro-controller 124 uses this data to control devices. In this example, themicro-controller 124 is coupled to a transmission shift assembly 126. Themicro-controller 124 will activate the transmission shift assembly when thetarget object 12 which determines the transmission shaft speed reaches a certain speed. - FIG. 8 is a perspective view of a
variable reluctance sensor 200 according to the present invention which senses the absolute position of a linearly movingtarget object 202. In this case the target object is arod 204 which is attached to the traveling portion of asuspension system 206. Thesuspension system 206 holds awheel 208. By determining the position of therod 204, the position of thewheel 208 may be determined for adjustments by the suspension system. - The outputs of the
sensor 200 are coupled to acontrol system 210 which is identical to thecontrol system 14 described with reference to FIG. 7 above. Thesensor 200 is similar to thesensor 10 described with reference to FIGS. 1-3 above. Thesensor 200 has a disk shapedmagnet 212 which is coupled to apole piece 214. The pole piece has a proximal end which is close to thetarget object 202 and a distal end. There is an air gap between the proximal end of thepole piece 214 and thetarget object 202. Thepole piece 214 has aplatter 216 which is located on the distal end of thepole piece 214 and supports themagnet 212. Thepole piece 214 is a ferrous material and has awire coil 218 which is coupled to thecontrol system 210. It is to be understood that themagnet 212 may be located in any appropriate location to generate a magnetic field within thecoil 218. - A covering 220 is located over the
coil 218 to protect thecoil 218. Thecircular covering 218 is typically an insulator material such as plastic. Two pairs of 222 and 224 are coupled around themagnets coil 218. - The
rod 204 is made of a ferrous material such as steel and has a series ofteeth 226. Since therod 204 is metal, its movement changes the flux in thewire coil 218 by the movement of theteeth 226 relative to thesensor 200. The flux generated by the movement of therod 204 generates a voltage output from thecoil 218 which is coupled to thecontrol system 210. The 222 and 224 force the flux from the magnetic field to travel through themagnets pole piece 214 and thecoil 218. The 222 and 224 thus prevent leaking of the flux from themagnets pole piece 214 and therefore increase the flux change and voltage output from thecoil 218. - Of course, the present invention may be employed in any application which requires determination of linear position or rotational position. Examples in the automotive field include suspension travel, crankshaft or crankshaft rotation and positioning, wheel speed and transmission shaft speed.
- It will be apparent to those skilled in the art that various modifications and variations can be made in the method and system of the present invention without departing from the spirit or scope of the invention. Thus, the present invention is not limited by the foregoing descriptions but is intended to cover all modifications and variations that come within the scope of the spirit of the invention and the claims that follow.
Claims (12)
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US09/742,517 US6433534B1 (en) | 2000-12-20 | 2000-12-20 | Increased output variable reluctance sensor |
| PCT/IB2001/002908 WO2002082099A1 (en) | 2000-12-20 | 2001-12-20 | Variable reluctance sensor |
| GB0313792A GB2386429A (en) | 2000-12-20 | 2001-12-20 | Variable reluctance sensor |
| DE10197057T DE10197057T1 (en) | 2000-12-20 | 2001-12-20 | Variable reluctance sensor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US09/742,517 US6433534B1 (en) | 2000-12-20 | 2000-12-20 | Increased output variable reluctance sensor |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| US20020074995A1 true US20020074995A1 (en) | 2002-06-20 |
| US6433534B1 US6433534B1 (en) | 2002-08-13 |
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| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US09/742,517 Expired - Lifetime US6433534B1 (en) | 2000-12-20 | 2000-12-20 | Increased output variable reluctance sensor |
Country Status (4)
| Country | Link |
|---|---|
| US (1) | US6433534B1 (en) |
| DE (1) | DE10197057T1 (en) |
| GB (1) | GB2386429A (en) |
| WO (1) | WO2002082099A1 (en) |
Cited By (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2006105894A1 (en) * | 2005-04-04 | 2006-10-12 | Knorr-Bremse Systeme für Nutzfahrzeuge GmbH | Ride level control device of a vehicle |
| US20150086049A1 (en) * | 2013-09-24 | 2015-03-26 | Knowles Electronics, Llc | Increased compliance flat reed transducer |
| US9888322B2 (en) | 2014-12-05 | 2018-02-06 | Knowles Electronics, Llc | Receiver with coil wound on a stationary ferromagnetic core |
| CN114814270A (en) * | 2022-04-14 | 2022-07-29 | 四川新川航空仪器有限责任公司 | Variable magnetic flux rotation speed sensor |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US7138623B2 (en) * | 2004-12-13 | 2006-11-21 | Magna Powertrain Usa, Inc. | Power transfer device with contactless optical encoder and color reflective surface |
| US9377328B2 (en) * | 2012-01-24 | 2016-06-28 | GM Global Technology Operations LLC | Variable reluctance sensor using spatially modulated magnetic fields |
| US10571481B2 (en) * | 2015-11-11 | 2020-02-25 | Goodrich Corporation | Low wheel speed detection utilizing variable reluctance speed transducer |
Family Cites Families (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US3492518A (en) | 1966-02-11 | 1970-01-27 | Avtron Mfg Inc | Magnetic-electric pickup for toothed wheels and the like |
| US4268771A (en) | 1977-11-04 | 1981-05-19 | Lace Melvin A | Magnetic probe |
| US5422432A (en) | 1990-10-10 | 1995-06-06 | Thomas E. Dorn | Electromagnetic pickup for a plural-string musical instrument incorporating a coil around a multi-laminate ferromagnetic core |
| US5602472A (en) * | 1993-01-15 | 1997-02-11 | Hughes Electronics | Apparatus and method for determining angular position and rotational speed using a rotating magnet and a directional magnetometer |
| JP3635707B2 (en) * | 1995-03-03 | 2005-04-06 | 日本精工株式会社 | Rolling bearing unit with rotational speed detector |
-
2000
- 2000-12-20 US US09/742,517 patent/US6433534B1/en not_active Expired - Lifetime
-
2001
- 2001-12-20 GB GB0313792A patent/GB2386429A/en not_active Withdrawn
- 2001-12-20 DE DE10197057T patent/DE10197057T1/en not_active Ceased
- 2001-12-20 WO PCT/IB2001/002908 patent/WO2002082099A1/en not_active Ceased
Cited By (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2006105894A1 (en) * | 2005-04-04 | 2006-10-12 | Knorr-Bremse Systeme für Nutzfahrzeuge GmbH | Ride level control device of a vehicle |
| US20090212509A1 (en) * | 2005-04-04 | 2009-08-27 | Falk Hecker | Ride Level Control Device of a Vehicle |
| US20150086049A1 (en) * | 2013-09-24 | 2015-03-26 | Knowles Electronics, Llc | Increased compliance flat reed transducer |
| US9326074B2 (en) * | 2013-09-24 | 2016-04-26 | Knowles Electronics, Llc | Increased compliance flat reed transducer |
| US9888322B2 (en) | 2014-12-05 | 2018-02-06 | Knowles Electronics, Llc | Receiver with coil wound on a stationary ferromagnetic core |
| CN114814270A (en) * | 2022-04-14 | 2022-07-29 | 四川新川航空仪器有限责任公司 | Variable magnetic flux rotation speed sensor |
Also Published As
| Publication number | Publication date |
|---|---|
| DE10197057T1 (en) | 2003-12-04 |
| GB0313792D0 (en) | 2003-07-23 |
| WO2002082099A1 (en) | 2002-10-17 |
| GB2386429A (en) | 2003-09-17 |
| GB2386429A8 (en) | 2003-10-20 |
| US6433534B1 (en) | 2002-08-13 |
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