GB2188157A - Magnetic sensor arrangements - Google Patents

Magnetic sensor arrangements Download PDF

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Publication number
GB2188157A
GB2188157A GB08705449A GB8705449A GB2188157A GB 2188157 A GB2188157 A GB 2188157A GB 08705449 A GB08705449 A GB 08705449A GB 8705449 A GB8705449 A GB 8705449A GB 2188157 A GB2188157 A GB 2188157A
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Prior art keywords
sensor
arrangement according
magnetic field
output
ofthe
Prior art date
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Granted
Application number
GB08705449A
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GB8705449D0 (en
GB2188157B (en
Inventor
Emerson Hardy Oetzmann
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Allard Way Holdings Ltd
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GEC Avionics Ltd
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Publication of GB8705449D0 publication Critical patent/GB8705449D0/en
Publication of GB2188157A publication Critical patent/GB2188157A/en
Application granted granted Critical
Publication of GB2188157B publication Critical patent/GB2188157B/en
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/02Measuring direction or magnitude of magnetic fields or magnetic flux

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  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Magnetic Variables (AREA)

Abstract

A magnetic sensor arrangement of the kind wherein an output representative of an applied magnetic field is produced by a piezoelectric member (1) secured to a magnetostrictive member (2) placed in the magnetic field includes an electromagnet (4) for applying an alternating magnetic field to the sensor, and a synchronous demodulator (18) for detecting the amplitude and phase of the alternating a component of the output of the magnetic sensor. The arrangement overcomes the effects of surface charge build-up, thermal expansion and electron drift in the sensor. In a modification a further electromagnet coupled to the output of demodulator 18 is arranged so as to apply a d.c. magnetic field to the sensor having a magnitude dependant upon the applied magnetic field but in opposition thereto to provide a negative feedback arrangement. <IMAGE>

Description

SPECIFICATION Magnetic sensor arrangements This invention reiates to magnetic sensor arrangements.
More particularlythe invention relates to magnetic sensor arrangements of the kind incorporating a magnetic sensor comprising a magnetostrictive first member having a dimension dependent on the strength of an applied magnetic field, and a piezoelectric second member, secured to the first member, so as to generate a potential difference representative of said dimension ofthe first member and hence of the magnitude ofthe applied magnetic field.
In such magnetic sensors build-up of charge on the surfaces of the second member, thermal expansion ofthe first and second members and electron drift in the second member can create a potential difference in addition to the potential difference indicative ofthe magnitude ofthe applied magnetic field and hence result in the sensor being noisy and unstable in operation.
It is an object of the present invention to provide a magnetic sensor arrangement wherein the above disadvantages are overcome.
According to the present invention there is provided a magnetic sensor arrangement comprising a magnetic sensor having a magnetostrictivefirst member having a dimension dependent on the strength of an applied magnetic field, and a piezoelectric second member secured to said first member so as to generate a potential difference representative of said dimension of said first member, said potential difference constituting the output of the sensor; an electromagnet arranged to apply an alternating magnetic field to said sensor in the direction of the said dimension; and circuit meansfordetecting the amplitude ofthe alternating component of the output of said sensor.
Various magnetic sensor arrangements in accordance with the invention will now be described byway of example with reference to the accompanying drawings of which Figure lisa perspective view of a first magnetic sensorsuitablefor use in the arrangements; Figure2 is a graph illustrating the operation of the sensor of Figure 1; Figure 3 is a schematic diagram of a first magnetic sensor arrangement using the sensor of Figure 1; Figure4is a graph showing waveforms occurring in operation of the magnetic sensor arrangement of Figure 3; Figure 5is a schematic diagram of a second magnetic sensor arrangement using the sensor of Figure 1; and Figure 6 is a perspective view of a second magnetic sensor suitable for use in the arrangements.
The magnetic sensors make use of the magnetostrictive and piezoelectric effects. A magnetostrictive material changes its dimensions when placed in a magneticfield and a piezoelectric material builds up a surface charge/voltage when it is subject two compression or tension.
Referring to Figure 1, the first magnetic sensor to be described comprises a rectangular strip of piezoelectricmaterial 1 sandwiched between two rectangular strips of electrically conductive magnetostrictive material 2 having a smallerwidth than the strip of piezoelectric material 1. The strips 2 are ofthe same length as the strip 1 and are positioned centrally on opposite main surfaces ofthe strip 1, with their narrower ends in register with the narrower ends of the strip 1. The piezoelectric material of the strip 1 is polarised so thatwhen subject two compression or extension in a direction parallel to its main faces, the strip 1 will generate a potential difference between its main surfaces.The two strips of magnetostrictive material 2 also serve as electrodes of the sensor and are each provided with a lead 3.
The strip 1 suitably consists of polyvinylidene fluoride (PVDF) and the strips 2 suitably consit of material known bythetrade names Metglas2605C0 (Allied Corporation) or Vitrovac 40-40 (Vacuumschmelze GmBH).
When the magnetic sensor is placed in a magnetic field directed parallel to the planes of the strips 1 and 2, the strips 2 will expand in the direction of the applied field and consequently stretch the strip of piezoelectric material 1 in the same direction. A dc potential difference is consequently generated between the main faces of the strip 1 whose value is representative ofthe strength of the applied field.
The potential difference may thus be applied to a suitable electric circuit via the leads 3 to obtain a measure ofthefield strength. The relationship between the applied magnetic field and the expansion ofthestrips is non-linear as shown bythe curve C in Figure 2. The same non-linear relationship exists between the generated potential and applied magneticfield,the relationship between the potential and the expansion being approximately linear.
It will be appreciated that the sensitivity ofthe sensorwill depend on the direction of the applied field, the sensor exhibiting maximum sensitivity in the direction ofthe lengths ofthe strips 1,2 and a minimum sensitivity in the direction of the widths of the strips 1, 2. Thus the sensor exhibits a dipole characteristic. In this connection the material ofthe strip 1 may suitably be itself made directionally sensitive so that it does not respond so readilyto change of dimension across its width as along its length. Since a change in length will normally be associated with a change of width of reverse sense, use of such a material will also increase the potential difference generated by a given change in length.
The above described simple dcsensor arrangement suffers from a build-up of charge on the surfaces of the strip 1, thermal expansion of the strips 1,2 and drift in the piezoelectric strip 1 itself.
As a result the sensor is noisy and unstable in operation. These difficuities may be overcome by using the sensor in a circuit in accordance with the invention as shown in Figure 3.
Referring to Figure 3 the circuit includes a solenoid 4 in which the sensor 1,2,3 is placed with its longitudinal axes parallel to the direction of the magnetic field produced bythe solenoid 4. The sensor 1,2,3 with the solenoid 4 surrounding it, is placed with its longitudinal axis in the direction of the magnetic field to be measured.
In operation an alternating current is supplied to the solenoid 4from a source 5. In consequence, due to the shape of the curve C, the extension of the strips 2 varies with the alternating field produced by the solenoid 4 by an amount dependent on the value of the field to be measured about a mean value of extension set by the value of the field to be measured. Hence a unidirectional voltage having undulationsofanamplitudesetbythefieldto be measured appears between the leads 3 of the sensor.
This will be further explained with reference to Figure 2.
If the magneticfieldto be measured has avalueas indicated by the line 6 in Figure 2 and the alternating magnetic field due to the solenoid 4 has an amplitude indicated by the waveform 7,then the corresponding extension of the strips 2 varies as indicatedbythewaveform8abouta meanvalue indicated by the line 9. Due to the shape of the curve Cin Figure 2 the amplitude and phaseofthevariation ofthe extension of the strips 2 depends respectively upon the value and direction of the magneticfield to be measured.
Hencefora magneticfieldto be measured of a value indicated by the line 10 in Figure 2 of smaller value than the value indicated bytheline6,butthe same direction, the corresponding extension ofthe strips 2 is as indicated by waveform 11 in Figure 2 abouta mean value indicated by line 12. Forafieldto be measured of value indicated by line 13 in Figure 2 ofthe opposite direction to the value indicated by lines 6 and 10, the extension ofthe strips 2 is as indicated bywaveform 14abouta mean value indicated by the line 15, the waveform 7 which is opposite to that ofwaveforms 8 and 11.
Thewaveforms8,11 and 14areshown in Figure4 to facilitate comparison.
The voltages produced between the leads 3 are, of course, of corresponding waveform to the extensions ofthe strips 2.
Referring again to Figure 3, the voltage between the leads 3 is fed via a differential amplifier 16to a bandpass filter 17. This removes the dc component ofthe output of the amplifier 16 and hence removes the aforementioned effects of drift and noise in the strips 1. The output offilter 17 will, therefore, comprise a double sideband suppressed carrier version of a carrier of the frequency of the source 5 amplitude modulated by the field to be measured.
The output of the filter 17 is fed to a synchronous demodulator 18 wherein its amplitude is detected followed by a low pass filter 19 to provide a dc signal whose value is representative of the value ofthe magnetic field to be measured.
Referring now to Figure 5, in a modification ofthe circuit of Figure 3 the output ofthe filter 19 is supplied to the positive inputofadifferentialdc amplifier 20 whose output is supplied via a coil 21 to load resistor 22. The voltage across the resistor 22 constitutes the output ofthe circuit and is applied to the negative input of the amplifier 20. The coil 21 is arranged adjacent the sensor 1,2,3 so as to applyto the sensor a magnetic field in opposition to the field to be measured. Hence the circuit operates as a dc negative feedback arrangement increasing the dynamic range ofmagneticfieldto bemeasuredto which the sensorwill respond. The system linearity is also increased.
It will be understood that whilst the sensor described above byway of example comprises a strip of piezoelectric material sandwiched between two strips of magnetostrictive material, the sensor of an arrangement according to the invention may have many alternative geometric forms.
Referring to Figure 6, one such alternative form of sensor comprises a central electrical Iy conductive member 23 around the outside of which is secured a tubular member 24 of piezoelectric material around the outside of which, in turn, there is secured a tubular member of magnetostrictive material 25.
With the piezoelectricmember24appropriately polarised, the sensor has a maximum sensitivityto an applied magnetic field in the axial direction. This arrangement has the advantage compared with the arrangement of Figure 1 that it is symmetrical inthe plane perpendicularto its axis ofmaximum sensitivity.
In another alternative form, not illustrated,the sensor comprises a circular plate of piezoelectric material sandwiched between two identically sized circular plates of magnetostrictive material. With the piezoelectric plate appropriately polarised the sensor acts as a unidirectional sensor to fields in a direction parallel to the plates.
In a further alternative form, not illustrated, a single planar member of magnetostrictive material is sandwiched between two plantar members of piezoelectric material, and metal electrodes are provided on the major surfaces of the piezoelectric members remote from the magnetostrictive member. An output is then derived from between a lead connected to the two electrodes and a lead connected to the magnetostrictive member.
Itwill further be understood thatwhilstinthe sensors described above the mag netostrictive members are electrically conductive and serve as electrodes, in other sensors the magnetostrictive members may be associated with layers of a suitable metal, such as gold, which serve as electrodes.

Claims (12)

1. A magnetic sensor arrangement comprising: a magnetic sensor having a magnetostrictivefirst member having a dimension dependent on the strength of an applied magnetic field, and a piezoelectric second member secured to said first member so as to generate a potential difference representative of said dimension of said first member, said potential difference constituting the output of the sensor; an electromagnet arranged to apply an alternating magnetic field to said sensor in the direction of the said dimension; and circuit means for detecting the amplitude ofthe alternating component of the output of said sensor.
2. An arrangement according to Claim 1 wherein said circuit means also detects the phase of said alternating component.
3. An arrangement according to Claim 1 or Claim 2 wherein said circuit means comprises a synchronous demodulator.
4. An arrangement according to any one ofthe preceding claims wherein said circuit means includes filter means to remove the dc component in the output of the sensor.
5. An arrangement according to Claim 4wherein said circuit means includesfiltermeansfor smoothing the detected signal.
6. An arrangement according to any one of the preceding claims further including an electromagnet responsive to the output of said circuit means to apply a dc magnetic field to said sensor having a magnitude dependent on the first-mentioned applied magneticfield but in opposition thereto, thereby to provide a negative feedback arrangement.
7. An arrangement according to any one ofthe preceding claims wherein said first member is secured to a first surface of said second member and said output is derived from between said first surface and a second surface of said second member opposite said first surface.
8. An arrangement according to Claim 7 wherein a magnetostrictivethird member having a dimension dependent on the strength of said magnetic field is secured to said second surface.
9. An arrangement according to any one of the preceding claims wherein said members are of planarform and are secured to one another in parallel relationship.
10. An arrangement according to any one of Claims 1 to 8wherein said members are of cylindrical form and are secured to one another in co-axial relationship.
11. An arrangement according to any one ofthe preceding claims wherein the or said magnetrostrictive member consists of an electrically conductive material and serves as an electrode for sensing said potential difference.
12. A magnetic sensor arrangement substantially as herein before described with referenceto Figure3 or Figure 5 ofthe accompanying drawings.
GB8705449A 1986-03-10 1987-03-09 Magnetic sensor arrangements Expired - Lifetime GB2188157B (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
GB8605871 1986-03-10

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GB8705449D0 GB8705449D0 (en) 1987-04-15
GB2188157A true GB2188157A (en) 1987-09-23
GB2188157B GB2188157B (en) 1990-07-18

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Cited By (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0246780A2 (en) * 1986-05-21 1987-11-25 Gec Avionics Limited Magnetic field direction indicating devices
US4975643A (en) * 1989-04-05 1990-12-04 Fisher Controls International, Inc. Measurement and control of magnetostrictive transducer motion using strain sensors
WO2000060369A1 (en) * 1999-04-05 2000-10-12 Spinix Corporation Passive solid-state magnetic field sensors and applications therefor
US6279406B1 (en) 1998-07-31 2001-08-28 Yi-Qun Li Passive solid-state magnetic field sensors and applications therefor
US6580271B2 (en) * 1999-07-20 2003-06-17 Spinix Corporation Magnetic field sensors
WO2004070408A1 (en) * 2003-02-04 2004-08-19 Nec Tokin Corporation Magnetic sensor
WO2013181970A1 (en) * 2012-06-04 2013-12-12 国民技术股份有限公司 Ac magnetic field sensing device
WO2014113694A1 (en) * 2013-01-17 2014-07-24 Northeastern University Magnetoelectric pickup element for detecting oscillating magnetic fields
CN103983925A (en) * 2014-06-03 2014-08-13 重庆材料研究院有限公司 Magnetic field detection device based on magnetorheological elastomer
CN103983925B (en) * 2014-06-03 2016-11-30 重庆材料研究院有限公司 Field detecting device based on magnetic rheology elastic body

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB709528A (en) * 1951-01-24 1954-05-26 Clevite Corp A magnetostrictive and electromechanical transducer device

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB709528A (en) * 1951-01-24 1954-05-26 Clevite Corp A magnetostrictive and electromechanical transducer device

Cited By (20)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0246780A3 (en) * 1986-05-21 1988-11-30 Gec Avionics Limited Magnetic field direction indicating devices
US4866384A (en) * 1986-05-21 1989-09-12 Gec-Marconi Limited Relative phase magnetic field direction indicating devices useful as compasses
EP0246780A2 (en) * 1986-05-21 1987-11-25 Gec Avionics Limited Magnetic field direction indicating devices
US4975643A (en) * 1989-04-05 1990-12-04 Fisher Controls International, Inc. Measurement and control of magnetostrictive transducer motion using strain sensors
US6809515B1 (en) * 1998-07-31 2004-10-26 Spinix Corporation Passive solid-state magnetic field sensors and applications therefor
US6279406B1 (en) 1998-07-31 2001-08-28 Yi-Qun Li Passive solid-state magnetic field sensors and applications therefor
US6437558B2 (en) 1998-07-31 2002-08-20 Spinix Corporation Passive solid-state magnetic field sensors and applications therefor
US6809516B1 (en) 1999-04-05 2004-10-26 Spinix Corporation Passive magnetic field sensors having magnetostrictive and piezoelectric materials
WO2000060369A1 (en) * 1999-04-05 2000-10-12 Spinix Corporation Passive solid-state magnetic field sensors and applications therefor
US6580271B2 (en) * 1999-07-20 2003-06-17 Spinix Corporation Magnetic field sensors
WO2004070408A1 (en) * 2003-02-04 2004-08-19 Nec Tokin Corporation Magnetic sensor
WO2013181970A1 (en) * 2012-06-04 2013-12-12 国民技术股份有限公司 Ac magnetic field sensing device
CN103454596A (en) * 2012-06-04 2013-12-18 国民技术股份有限公司 Alternating magnetic field sensing device
US20150192645A1 (en) * 2012-06-04 2015-07-09 Nationz Technologies Inc. Alternating magnetic field sensing device
US9606192B2 (en) 2012-06-04 2017-03-28 Nationz Technologies Inc. Alternating magnetic field sensing device
CN103454596B (en) * 2012-06-04 2017-04-12 国民技术股份有限公司 Alternating magnetic field sensing device
WO2014113694A1 (en) * 2013-01-17 2014-07-24 Northeastern University Magnetoelectric pickup element for detecting oscillating magnetic fields
US9508333B2 (en) 2013-01-17 2016-11-29 Northeastern University Magnetoelectric pickup element for detecting oscillating magnetic fields
CN103983925A (en) * 2014-06-03 2014-08-13 重庆材料研究院有限公司 Magnetic field detection device based on magnetorheological elastomer
CN103983925B (en) * 2014-06-03 2016-11-30 重庆材料研究院有限公司 Field detecting device based on magnetic rheology elastic body

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GB8705449D0 (en) 1987-04-15
GB2188157B (en) 1990-07-18

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