POSITION MEASURING APPARATUS AND METHOD FOR OPERATING THE POSITION MEASURING APPARATUS
20170074682 · 2017-03-16
Assignee
Inventors
Cpc classification
International classification
Abstract
A position measuring apparatus measures the position(s) of an electrically conductive measurement object which can be moved over a measurement section, along which coils are positioned. A measuring coil is provided between every two excitation coils, through each of which excitation coils an alternating excitation current flows, which current is predefined to be in phase opposition from excitation coil to excitation coil. The alternating magnetic fields produced by the alternating excitation currents induce eddy currents in the electrically conductive measurement object when the measurement object moves past the excitation coils. The measuring coils provide an AC measurement voltage which is induced by the eddy currents flowing in the measurement object when the measurement object moves past the at least one measuring coil. The position of the measurement object is determined on the basis of the at least one AC measurement voltage.
Claims
1. Position measuring apparatus to measure the position (s) of an electrically conductive measurement object (28) which is moveable over a measurement section (18), along which coils (14; 14a, 14b; 16) are positioned, wherein an odd number of coils (14; 14a, 14b; 16) is provided; the coils at the odd positions are excitation coils (14; 14a, 14b) which are flowed through by an alternating excitation current (20) respectively which is provided to be in phase opposition, from excitation coil (14; 14a, 14b) to excitation coil (14; 14a, 14b), such that the alternating magnetic fields (22; 15 22a, 22b) generated by the alternating excitation currents (20) induce eddy currents in the electrically conductive measurement object (28) when the measurement object (28) moves past the excitation coils (14; 14a, 14b); the coil (16) at at least one even position between two excitation coils (14; 14a, 14b) is a measurement coil (16) providing a measurement alternating voltage (30, 30, 30 . . . ) which is induced by the eddy currents flowing in the measurement object (28) when the measurement object (28) moves past the at least one measurement coil (16); and a determination of the position (s_Mess) of the measurement object (28) is provided on the basis of the at least one measurement alternating voltage (30, 30, 30 . . . ).
2. Position measuring apparatus to measure the position (s) of an electrically conductive object (28) which is moveable over a measurement section (18), along which coils (14, 16) are positioned, wherein the coils (14, 16) are excitation coils (14) alternating at the even positions and in chronological order at the odd positions, said excitation coils being flowed through by a alternating excitation current (20) respectively which is provided to be in phase opposition from excitation coil (14) to excitation coil (14) by means of a switching device (92a, 92b) such that the alternating magnetic fields (22) generated by the alternating excitation currents (20) induce eddy currents in the electrically conductive measurement object (28) when the measurement object (28) passes the excitation coils (14); the one coil (16) is alternately connected as a measurement coil (16) at at least one odd position and correspondingly in chronological order at at least one even position between two excitation coils (14) by the switching device (92a, 92b), said measurement coils providing measurement alternating voltages (30, 30, 30 . . . ) respectively, which is induced by the eddy currents flowing in the measurement object (28) when the measurement object (28) passes the measurement coils (16); and a determination of the position (s_Mess) of the measurement object (28) is provided on the basis of the measurement alternating voltages (30, 30, 30 . . .).
3. Position measuring apparatus according to claim 1, wherein the coils (14, 14a, 14b, 16) are positioned in a row along the measurement section (18) one next to the other; and the measurement object (28) is arranged to toe moveable along the front side of the coils (14, 16).
4. Position measuring apparatus according to claim 3, wherein the coils (14, 14a, 14b, 16) are positioned in a straight line in a row along the measurement section (18) one next to the other; and the measurement object (28) is arranged to be moveable in a straight line along the front side of the coils (14, 14a, 14b, 16).
5. Position measuring apparatus according to claim 1, wherein the coils (14, 14a, 14b, 16) are positioned in a row along the measurement section (18); the coils (14, 16) are implemented to be annular coils (14, 14a, 14b, 16); and the measurement object (28) is arranged to be moveable in the central opening of the annular coils.
6. Position measuring apparatus according to claim 1, wherein the coils (14, 14a, 14b, 16) are positioned along a curved measurement section (18); and the measurement object (28) is arranged to be moveable along the curved measurement section (18).
7. Position measuring apparatus according to claim 6, wherein the coils (14, 14a, 14b, 16) are arranged on a circle periphery along the measurement section (18) one next to the other; and the measurement object (28) is rotationally moveable.
8. Position measuring apparatus according to claim 7, wherein the coils (14, 14a, 14b, 16) are aligned perpendicularly to the rotational axis (80) of the circle and the measurement object (28) is arranged to be rotationally moveably on an inner or outer circle periphery with regard to the coils (14, 14a, 14b, 16).
9. Position measuring apparatus according to claim 7, wherein the coils (14, 14a, 14b, 16) are positioned and aligned in parallel to the rotational axis (80) of the circle on the circumference of the circle; and the measurement object (28) is moved in the axial direction with regard to the coils (14, 14a, 14b, 16) and is arranged to be rotationally moveable.
10. Position measuring apparatus according to claim 1, wherein coil cores (24, 26) are provided and the coil cores (24, 26) are designed to be U-shaped.
11. Position measuring apparatus according to claim 1, wherein coil cores (24, 26) are provided; the coil cores (24, 26) are designed to be E-shaped and the coil windings are arranged on the central E-arm.
12. Position measuring apparatus according to claim 1, wherein an oscillator (60) having direct digital synthesis and a voltage/current converter (62) are provided for providing the alternating excitation current (20).
13. Position measuring apparatus according to claim 1, wherein the excitation coils (14; 14a, 14b) are at least one part of the inductance (L1, L2) of an LC-oscillator (70).
14. Position measuring apparatus according to claim 1, wherein the frequency of the alternating excitation current (20) ranges from 100 kHz to 10 MHz.
15. Position measuring apparatus according to claim 1, wherein a non-ferromagnetic measurement object (28) is provided.
16. Position measuring apparatus according to claim 1, wherein a ferromagnetic measurement object (28) is provided.
17. Method for operating the position measuring apparatus (12, 13) according to claim 1, wherein at least two measurement coils (16) are provided; a certain phase position is allocated to each measurement coil (16); a quadrature signal pair (q.sub.sin, q.sub.cos) is calculated as the sum of the products of the voltages (U1, U2, . . . Um) which are obtained from the measurement alternating voltages (30, 30, 30) provided by the measurement coils (16) by demodulation with the correct preceding sign, and sine functions having a phase position which is allocated to the measurement coils (16) respectively, and, as the sum of the products of the voltages (U1, U2, . . . Um) and cosine functions, likewise having the phase position which is allocated to the measurement coils (16) respectively; and the position (S_Mess) of the measurement object (28) is determined from the phase of the two quadrature signals (q.sub.sin, q.sub.cos).
18. Method according to claim 17, wherein a background value is detected which occurs without a measurement object (28) present; and the background value is subtracted from the voltages (U1, U2, . . . Um).
19. Method according to claim 17, wherein a normalization to align the ranges (49) is carried out, said ranges (49) lying between positive maxima (44, 44, 44) and negative maxima (48, 48, 48) of the voltages (U1, U2, . . . Um).
20. Method according to claim 17, wherein a linearization of the connection between the measured and the actual position (S_Mess, s) of the measurement object (28) is carried out.
21. Method according to claim 20, wherein the linearization is carried out by means of a determination of the phase positions allocated to the measurement coils (16).
22. Method according to claim 17, wherein envelope factors (c.sub.i.sup.env) are provided; the signal courses (40, 40, 40 . . . ) having an envelope factor (c.sub.i.sup.env) respectively are weighted in such a way that the signal courses (40, 40, 40 . . . ), which have been gained from the measurement alternating voltages (30, 30, 30) of the measurement coils (16), which are positioned at the ends of the measurement section (18), by demodulation with the correct sign, are weighted to be lower than the signal courses (40, 40, 40 . . . ), which have been gained from the measurement alternating voltages (30, 30, 30) of the measurement coils (16), which are positioned in the center of the measurement section (18), by demodulation with the correct sign.
Description
BRIEF DESCRIPTION OF THE FIGURES
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DETAILED DESCRIPTION OF THE EXEMPLARY EMBODIMENTS
[0076]
[0077] An alternating current is provided as a excitation current 20, such that the magnetic fields 22a, 22b are alternating magnetic fields 22a, 22b. The frequency of the excitation current 20 typically ranges from 100 kHz to a few MHz, for example up to 10 MHz. The alternating magnetic fields 22a, 22b directed in opposite directions are coupled to the central coil 16 which serves as a measurement coil 16. In the exemplary embodiment shown, all coils 14a, 14b, 16 contain a rod-shaped magnetic core 24a, 24b, 26 respectively which consists of a magnetisable, preferably a ferromagnetic, material, for example iron.
[0078] The position measuring apparatus 12 according to the invention detects the position of a measurement object 28 with regard to the sensor unit 10, said object moving along the measurement section 18. A substantial advantage of the position measuring apparatus 12 according to the invention is that the measurement object 28 can be implemented as a simple, electrically conductive measurement object 28. For example, an electrical insulator can be provided as a measurement object 28 which is provided with an electrically conductive coating. For example, aluminium, copper, tin and similar are suitable as a non-ferromagnetic material. Alternatively, the measurement object 28 can also be produced from a ferromagnetic material such as iron. Due to the electrical conductivity, eddy currents are induced in particular on the surface of the measurement object 28 due to the alternating magnetic fields 22a, 22b, said eddy currents being surrounded on their part by a magnetic excitation which is not shown in more detail.
[0079] Without a measurement object 28 present in the region of the sensor unit 10, a part of the alternating magnetic fields 22a, 22b directed in opposite directions of the two excitation coils 14a, 14b is coupled to the measurement coil 16 and occurs as a background value. Under the condition that the structure is implemented to be at least approximately symmetrical and the alternating magnetic fields 22a, 22b directed in opposite directions of the excitation coils 14a, 14b have, as a consequence, at least approximately the same magnetic induction, a measurement alternating voltage 30 provided by the measurement coil 16 is at least approximately equal to zero. The alternating magnetic field 22a of the excitation coil 14a positioned on the left-hand side induces a partial measurement alternating voltage in the measurement coil 16 having a first polarity and the alternating magnetic field 22b of the excitation coil 14b positioned on the right-hand side likewise generates a partial measurement alternating voltage in the measurement coil of the same amount, but of different polarity, such that the resulting measurement alternating voltage 30 of both induced partial measurement alternating voltages is at least approximately equal to zero.
[0080] An alignment within the sensor unit 10 can occur in that the positions of the individual coils 14a, 14b, 16 are adjusted. In principle it is already sufficient to only adjust the position of the measurement coil 16. Later, a purely numerical alignment is described in which, on the one hand, the range 49 recorded in
[0081] The background value can both, as already described, be adjusted to zero mechanically, and also electronically by means of a differential amplifier or subtracted numerically after a digitalisation.
[0082] In
[0083] The parts shown in
[0084] To obtain the voltage U of the signal course 40, the measurement alternating voltage 30 is demodulated with the correct polarity. The signal course 40 is depicted depending on the position s of the measurement object 28. The signal course 40 results if the electrically conductive measurement object 28 moves along the measurement section 18. For the demodulation with the correct polarity, a cycle signal can be used as a reference signal, whose frequency is identical to the frequency of the excitation current 20.
[0085] If the measurement object 28 is approached by the right-hand side of the measurement coil 16, as depicted in the exemplary embodiment according to
[0086] If the measurement object 28 is moved further to the left in the direction of the measurement coil 16, the signal course 40 firstly increases further, because a larger surface of the measurement object 28 is exposed to the alternating magnetic excitation 22b of the right-hand excitation coil 14b and the eddy currents or the magnetic alternating magnetic fields accompanying the eddy currents occur closer in the region of the measurement coil 16.
[0087] If the measurement object 28 moves further to the left in the direction of the left excitation coil 14a, eddy currents are also increasingly generated in the measurement object 28 by the alternating magnetic excitation 22a of the left-hand excitation coil 14a which, however, due to the opposite orientation of the alternating magnetic excitation 22a, lead to magnetic fields directed in opposite directions with regard to the alternating magnetic excitation 22b of the right-hand excitation coil 14b and therefore partially compensate for the eddy currents induced by the right-hand excitation coil 14b. After the passing of a first signal maximum 44 corresponding to a first positive amplitude, a signal drop 46 therefore occurs.
[0088] A state of equilibrium in which the measurement alternating voltage 30 and the voltage U are equal to zero and the signal course 40 passes the zero line occurs if the measurement object 28 assumes a position s which lies in the centre of the sensor unit 10.
[0089] If the measurement object 28 moves further to the left in the direction of the left-hand excitation coil 14a, the alternating magnetic excitation 22a of the left-hand excitation coil 14a predominates, such that the signal drop 46 continues with a now negative measurement alternating voltage 30 demodulated with the correct sign.
[0090] The influence of the alternating magnetic excitation 22a of the left-hand excitation coil 14a increasingly strengthens while the influence of the alternating magnetic excitation 22b of the right-hand excitation coil 14b increasingly reduces until a second, negative signal maximum 48 is reached.
[0091] If the measurement object 28 is moved out from the sensor unit 10 to the left along the measurement section 18, a signal increase 50 occurs again after the negative signal maximum 48. If the measurement object 28 is moved out from the detection region of the sensor unit 10 to the left, the signal course 40 falls again to the zero line.
[0092] In the region between the first signal maximum 44 and the second signal maximum 48 of opposite polarity, the monotonously decreasing signal decrease 46 occurs which becomes a corresponding signal increase during a movement of the measurement object 28 along the measurement section 18 from the left side in the direction of the right side. In this region, the voltage U gained from the measurement alternating voltage 30 can be clearly allocated to a certain position s of the measurement object 28.
[0093] As already explained, due to mechanical inaccuracies, a background value can occur. The background value can be both, as already described, adjusted mechanically to zero and electronically by means of a differential amplifier or subtracted numerically after a digitalisation.
[0094] Later, a purely numerical alignment is described in which, on the one hand, the range 49 recorded in
[0095]
[0096] Alternatively, the excitation current 20 can be provided with an LC oscillator 70. A corresponding block diagram of a circuit arrangement is shown in
[0097] Since the measurement object 28 is preferably implemented as a non-magnetisable measurement object 28, the frequency range of the excitation current 20 can be determined to be comparatively high and, for example, lies above 100 kHz and can extend until, for example, 10 MHz. In this frequency range, the oscillator 60 or the LC oscillator 70 can be implemented with simple circuit means. A particular advantage of the comparatively high frequency range of the excitation current 20 lies in that the position s of the measurement object 28 can be determined comparatively quickly from the measurement alternating voltage 30 or from the voltage U.
[0098] Purely in principle, a conductive, magnetisable, preferably ferromagnetic, material can be provided as a measurement object 28.
[0099] In
[0100] If it is ensured chat the measurement object 28 is freely moveable in the central opening of the coils 14a, 14b, 16, alternatively to the depicted straight-line measurement section 18, a curved measurement section 18 can also be provided.
[0101] In
[0102] The excitation current 20 leads to the provision of alternating magnetic fields 22a, 22b, originating from the two outer excitation coils 14a, 14b, wherein in this exemplary embodiment, the alternating magnetic fields 22a, 22b are orientated substantially perpendicularly to the rotational axis 80. The alternating magnetic excitation 22a of the left excitation coil 14a and the alternating magnetic excitation 22b of the right excitation coil 14b are also here aligned in opposite directions again. In the shown exemplary embodiment, it is again assumed that the coils 14a, 14b, 16 have rod-shaped magnetic cores 24a, 24b, 26, preferably ferromagnetic magnetic cores 24a, 24b, 26 respectively.
[0103] Purely in principle, it is possible to deviate from the circular design and to provide any predetermined, curved measurement section 18.
[0104] Only one sensor unit 10 has been shown from the position measuring apparatus 12 according to the invention in
[0105] A corresponding exemplary embodiment which expands the design of the position measuring apparatus 12 shown in
k=2m+1
wherein m is the number of measurement coils 16.
[0106] Purely in principle, the arrangement shown in
[0107]
[0108] The signal courses 40, 40, 40 have positive maxima 44, 44, 44 and negative maxima 48, 48, 48 respectively, between which a range 49 occurs respectively, as recorded in
[0109] Depending on potentially present mechanical inaccuracies of the position measuring apparatus 12 according to the invention, a background value can occuras has been explained multiple times alreadywhich can be detected when the measurement object 28 is not present. Preferably, instead of or even in addition to an alignment of the entire arrangement, an electronic correction is provided. Here, the background value detected without the measurement object 28 is removed from the signal courses 40, 40, 40 of the voltage of the measurement alternating voltages U1, U2, . . . Um demodulated with the correct sign, for example by means of a differential amplifier.
[0110] Preferably, a normalisation is furthermore provided in which the range 49 is compensated for or normalised between the positive maxima 44, 44, 44 and negative maxima 48, 48, 48 belonging together.
[0111]
[0112]
K=M+2
wherein M is the number of available measurement alternating voltages 30, 30, 30.
[0113]
[0114] Also in this embodiment, three coils 14, 16 arranged one next to the other form a sensor unit 10, 10, 10 respectively.
[0115]
[0116] By switching the functions of the coils between the two work cycles, sensor units 10, 10, 10 locally shifted by a coil in chronological order result such that, therefore, an increased spatial resolution during the measuring of the position s with clearly reduced effort is achieved by using this embodiment of the position measuring apparatus 13 according to the invention.
[0117] The embodiment of the position measuring apparatus 13 according to the invention according to
[0118] Corresponding exemplary embodiments are shown in
[0119]
[0120] In
[0121] In
[0122] To determine the position s from the measurement alternating voltages 30, 30, 30 demodulated with the correct polarity, preferably a so-called multi-phase quadrature demodulation is suitable, which is described below in more detail. The range of the signal drop 46 of the signal course 40 in
[0123] Firstly, each measurement coil 16 of each sensor unit 10, 10, 10 . . . , or each signal course 40, 40, 40 . . . has a certain phase position which differ for example by 85 in the case of a plurality of measurement coils 16. It is required that the measurement signals 30, 30, 30 of the measurement coils 16 be demodulated with the correct sign in order to obtain the voltages U1, U2, . . . Um or the signal courses 40, 40, 40 shown in
[0124] The two analogous quadrature signals q.sub.sin, q.sub.cos result from the following equations:
[0128] The two analogous quadrature signals q.sub.sin, q.sub.cos are therefore obtained as a linear combination of the voltages U1, U2, . . . Um of the signal courses 40, 40, 40 . . . , which have been obtained from the measurement alternating voltages 30, 30, 30 . . . demodulated with the correct sign, wherein the two quadrature signals q.sub.sin, q.sub.cos are calculated as the sum of the products of the voltages U1, U2 . . . Um and sine functions having a phase position which is allocated to the signal courses 40, 40, 40 . . . respectively and as the sum of the products of the voltages U1, U2, . . . Um and cosine functions, likewise having the phase position which is allocated to she sensor units 10, 10, 10 or the measurement coils 16 or the signal courses 40, 40, 40, . . . respectively.
[0129] The position s_Mess is obtained from the position-dependent phase parameters of the quadrature signals q.sub.sin, q.sub.cos, for example using the arc tangens function in the fourth quadrant. An ambiguity due to phase jumps by 360 can therefore be eliminated in a simple manner, because a certain signal course 40, 40, 40 clearly dominates depending on the actual position s of the measurement object 28 and therefore the position s can be allocated at least roughly to a certain signal, course 40, 40, 40.
[0130] A position measurement on the basis of the multiphase quadrature demodulation is shown in
[0131] A further position measurement on the basis of the multiphase quadrature demodulation is shown in
[0132] By means of the measurements shown in
[0133]
[0134]
[0135]
[0136] The shown examples prove the insensitivity with respect to errors in the position measuring apparatus 12, 13 according to the invention during the application of the multiphase quadrature demodulation to determine the position s_Mess of the measurement object 28.
[0137] A particularly advantageous embodiment of the method according to the invention for determining the position s_Mess of a measurement object 28 using the position measuring apparatus 12, 13 according to the invention is explained by means of
[0138] The embodiment provides the use of an envelope factor c.sub.i.sup.env by which the voltages U1, U2, . . . Um corresponding to the signal courses 40, 40, 40 . . . are multiplied respectively. The envelope factors c.sub.i.sup.env are provided in such a way that the signal courses 40, 40, 40 . . . which are gained from the measurement coils 16 lying furthest at the ends of the position measuring apparatus 12, 13 according to the invention respectively are weighted to be lower and the signal courses 40, 40, 40 . . . obtained from the measurement coils 16 positioned in the centre of the measurement section 18 are weighted to be higher.
[0139] In
[0140] The result for the determination of the position s_Mess without the advantageous embodiment relating to the multiplication of the signal courses 40, 40, 40 . . . with the envelope factors c.sub.i.sup.env is depicted in
[0141] According to the advantageous embodiment, the signal courses 40, 40, 40 . . . shown in
TABLE-US-00001 i c.sub.i.sup.env 1 0.45 2 0.85 3 1.00 4 1.00 5 0.85 6 0.45
according to the formula:
U.sub.1.sup.env=U.sub.1c.sub.i.sup.env,
wherein, with U.sub.1, the voltages of the measurement alternating voltages 30, 30, 30 demodulated with the correct sign and provided by the measurement coils 16 are to be labelled corresponding to the signal courses 40, 40, 40.
[0142] The signal, courses resulting due to the weighting with the envelope factors c.sub.i.sup.env are shown in
[0143] The result of the position determination with the advantageous embodiment by multiplication of the signal courses 40, 40, 40, . . . with the envelope factors c.sub.i.sup.env is depicted in