Method and apparatus for detecting absolute position

Abstract: A rod member (21) provided with magnetic and non-­ magnetic portions (22A, 22B, 22C, 22D; 23) arranged alter­ natingly is prepared and a plurality of detecting heads (41, 42) for detecting magnetic resistance are disposed along the longitudinal direction of the rod member (21) with predetermined spaces, respectively. The pitches of the re­ spective pairs of the magnetic and non-magnetic portions (22A, 22B, 22C, 22D; 23) are arranged with pitches different with each other by the predetermined distances. Output signals transmitted from the detecting heads (41, 42) in accordance with the relative movement between the rod member (21) and the detecting heads (41, 42) are detected by phase detectors, and on the basis of the detected signals, the predetermined operation is carried out in an operation processing unit thereby to obtain the absolute positional relation between the rod member (21) and the detecting heads (41, 42) in, for example, a positioning system such as in a die casting machine.

Description: Background of the Invention This invention relates to a method and apparatus for detecting an absolute position of a rod member used for a positioning system in a machine such as a machine tool and a die casting machine. FIG. 1 shows a schematic principle construction of a position detecting means as the most important portion for a positioning system of a machine such as a machine tool and a die casting machine. Such a positioning system is disclosed in EP-A-0 115 008. Referring to FIG. 1, a plurality of magnetic materials 2 and the non-magnetic materials 3 are formed or arranged coaxially and alternatingly with equal pitches P on the outer or inner peripheral surface of a movable cylindrical rod 1. Primary excitation coils 6A and 6B and secondary induction coils 5A and 5B are coaxially located respectively in magnetic shield cores 10A and 10B which are located in a cylindrical detecting head portion 4 stationarily arranged so as to surround the rod 1. When the primary coils 6A and 6B are excited with an alternating current provided with phases I·sin ωt and I · cos ωt, respectively, the magnetic resistance is changed every one pitch in accordance with the movement of the rod 1 in the axial direction by the alternating arrangement of the magnetic materials 2 and the non-magnetic materials 3. The change of the magnetic resistance results in the induced potential change to the secondary induction coils 5A and 5B and an induced electromotive force E will be expressed as follows. E = K·sin ( ωt - 2 π X P ) where K: Conversion coefficient, X: Moving distance of rod, P: Pitch. In view of the phase (2π X p ) in this equation (1) it is found that only the moving distance X of the rod 1 is phase-shifted in comparison with the phase I·sin ωt in the primary excitation. Accordingly, the moving distance X is obtained by detecting the phase difference between these phases and taking out the phase difference as signal EO representing an electric potential. According to the unit shown in FIG. 1, however, the absolute distance can be obtained only in a case where the moving distance X of the rod 1 is within the range of one pitch P thereof. Namely, since the moving distance X is obtained only by an incremental form, when the moving distance X is over one pitch P, a quasi-absolute distance can be obtained by integrating the output potential signal EO, FIG. 2 shows a variation of the potential signal EO and the horizontal axis of the graph shown in FIG. 2 represents the moving distance X and the vertical axis thereof represents the level of the potential signal EO, which is output repeatedly every one pitch. The absolute position is thus detected by integrating the output potentials, but at the starting time of the movement of the rod. The integrated amount is under the reset condition, so that the absolute position can not be detected in this meaning. For this reason, in the conventional technique, it is restricted that the rod 1 should be absolutely returned to the original reference position at the starting time of the rod movement. FIG. 3 shows another example of a device for detecting the absolute position without having the restriction described above. In this device, parallelly arranged rods 1A and 1B are integrated so as to be both movable in their longitudinal, i.e. axial directions and detecting heads 4A and 4B are located near the rods 1A and 1B, respectively. The rod 1A is provided with a plurality of magnetic materials 2A and non-magnetic materials 3A alternatingly and the rod 1B is also provided with a plurality of the magnetic materials and the non-magnetic materials 3B. In this example, the rods 1A and 1B are constructed so that the pitch PA between one pair of the materials 2A and 3A is different from the pitch PB between one pair of the materials 2B and 3B, and accordingly the detecting heads 4A and 4B detect the different electric potentials E01 and E02 as shown in FIGS. 4A and 4B when the rods 1A and 1B are moved together. The absolute position can be detected by the combination of the potentials E01 and E02. In this device, however, it is required to locate the two rods 1A and 1B and the two detecting heads 4A and 4B, and this arrangement makes large the whole structure of the device, thus being expensive and not economical. Summary of the Invention An object of this invention is to improve defects or disadvantages of the prior art technique for detecting an absolute position of a movable member in a positioning system and to provide an effective method and a small apparatus for easily and at a low cost detecting the absolute position by means of using only one rod member according to the improved arrangement of the rod member and detecting heads with high operation precision. Another object of this invention is to provide rod members which are capable of using as a member of absolute detecting means and which have various arrangements of magnetic portions and non-magnetic portions in connection with the location of a plurality of detecting heads. According to this invention, these and other objects can be achieved by providing method for detecting an absolute position according to the features of claim 1. This invention also provides, for achieving the same purposes, an apparatus for detecting an absolute position according to the features of claim 5. Another aspect of this invention, there are also provided rod members which are capable of using as a member of absolute detecting means according to the features of claim 6. The nature, principle and utility of the invention will become more apparent from the following detailed description when feed in conjunction with the accompanying drawings. Brief Description of the Drawings In the accompanying drawings: FIG. 1 it a schematic view which shows a conventional arrangement of a rod and detecting heads for detecting an absolute position; FIG. 2 shows a graph which explains an operation analysis of the arrangement shown in FIG. 1; FIG. 3 is schematic view which shows another conventional arrangement of the rod 5 and the detecting heads; FIG. 4A and 4B show graphs which explain operation analysis of the arrangement shown in FIG. 3; FIGS. 5A through 5C and FIG. 6 respectively show schematic views of an arrangement of a rod and detecting heads and graphs explaining the operation analysis of the arrangement according to this invention; FIGS. 7A through 7D and FIGS. 8A and 8B show graphs which represent the relationship between the rod moving amount and phase detecting voltages based on the arrangement according to this invention; FIG. 9 is a block diagram which shows an example of arrangement of the apparatus according to this invention; FIGS. 10A through 10D respectively show an arrangement of a rod and detecting heads for detecting an absolute position according to this invention and graphs explaining an operation analysis of this arrangement; FIGS. 11A through 11D show another arrangement of a rod and detecting heads of this invention and graphs which explain an operation analysis of this arrangement; and FIGS. 12A through 12C show rod members which have various structures which are applicable to this invention, respectively. Description of the Preferred Embodiment FIGS. 5A through 5C are analytic views to be used for explaining the operation or a rod 21, generally having a circular cross section, based on the method of this invention, and referring to FIG. 5A, a plurality of magnetic materials 22A, 22B, 22C ... and non-magnetic portions 23 are alternatingly arranged on the outer peripheral surface of the rod 21 along the longitudinal direction thereof and the pitch of the respective paired magnetic and non-magnetic materials are minutely and successively increased by an increment ΔI as represented by I, I + ΔI, I + 2ΔI,.... The detecting heads 41 and 42 for detecting magnetic resistance are disposed in parallel with the rod 21 and in a spaced relation with each other by the distance I, i.e. The pitch distance, and primary and secondary excitation coils are wound in pairs around the detecting heads 41 and 42 such as described with reference to FIG. 1. FIGS. 5B and 5C show respectively phase detection voltages H1 and H2 detected as phase components of induced electromotive forces for the secondary coils of the detecting heads 41 and 42 with respect to the moving distance X of the rod 21. As is understood from FIGS. 5B and 5C, the period of the output H1 of FIG. 5B is different by a distance corresponding to the interval of the pitch I of the detecting heads 41 and 42 in comparison with the output H2 of FiG. 5C, thus causing the differences ΔI, 2ΔI, 3ΔI ... in the pitches. For this reason, for instance, when comparing the output voltages at the moving distance Ps, the phase detection voltage H1 of the detecting head 41 is represented by SS1, which is different from the phase detection voltage H2, being represented by SS2, of the detecting head 42. Supposing now that one pitch is divided into one thousand numbers, the phase detection voltage HH obtained by the detecting head is converted into "0" through "999" as shown in FIG. 6, and in that case, the moving distance Ps will be obtained as the following equation (2) or expression. Ps = ℓ + (ℓ+ Δℓ) +(ℓ+2Δℓ) + ℓ +3Δ ℓ 1000 × (SS1) = 3 × (ℓ+ Δℓ) + ℓ +3Δ ℓ 1000 × (SS1) With reference to the equation (2) and regarding the output characteristics of the phase detection voltages HC and HD of the detecting heads 41 and 42 represented by graphs of FIGS. 7A through 7D, a general equation of the moving distance Pn₁ (or Pn₂) will be expressed as follows. Pn = n ( ℓ + n-1 2 · Δℓ) + ℓ +n· Δℓ 1000 ·S where Pn: Moving distance of rod 21, n: Rod 21 passing pitch number, S: Phase detection output potential at the moving distance. The moving distance Pn₁ is expressed as follows when detected by the detecting head 41 on the basis of the equation (3). Pn₁ = n (ℓ + n-1 2 · Δℓ) + ℓ + n·Δℓ 1000 ·S1 In the similar manner, the distance Pn₁ will be expressed as follows when detected by the detecting head 42. Pn₁ = n (ℓ + Δℓ + n-1 2 · Δℓ) + ℓ + Δℓ + n· Δℓ 1000 · S2 = n (ℓ + n+1 2 · Δℓ) + ℓ + (n+1) Δℓ 1000 · S2 Since the moving distances Pn₁ in the equations (4) and (5) are in general equal to each other, the following relation or expression (6) will be established. n (ℓ + n-1 2 · Δℓ) + ℓ + n·Δℓ 1000 ·S1 = n ( ℓ + n+1 2 · Δℓ) + ℓ + (n+1) Δℓ 1000 · S2 S1 = ℓ + (n+1) · Δℓ ℓ + n·Δℓ ·S2 + n· Δℓ ℓ + n· Δℓ × 1000 Although the equation (6) is obtained with respect to the moving distance Pn₁ under the detected voltage condition represented by the graphs of FIGS. 7A and 7B, it will be necessary in actual to consider conditions represented by the graphs of FIGS. 7C and 7D. Referring to the graphs of FIGS. 7C and 7D, the moving direction Pn₂ will be expressed as follows as the equation (7) by substituting the value S1 in the equation (4) with the value S3 and as the equation (8) by substituting the values n and S2 in the equation (5) with the values (n-1) and S4, respectively. Where the values S3 and S4 are phase detection voltage values given by the detecting heads 41 and 42. Pn₂ = n( ℓ + n-1 2 · Δℓ) + ℓ + n· Δℓ 1000 ·S3 Pn₂ = (n-1) ( ℓ + n 2 · Δℓ) + ℓ + n·Δℓ 1000 ·S4 Accordingly, the following equation or expression (9) will be established. S3 = S4 - ℓ ℓ + n· Δℓ × 1000 Consequently, the pitch number n can be obtained by optionally selecting the equation (6) or (9) with the values or amounts S1 to S4, I and ΔI, which are preliminarily known. In other words, the absolute value of the moving distance X of the rod 21 can be obtained from the thus obtained pitch number n. The pitch number n is obtained by subsequently substituting n = 0, 1, 2,... into the equations (6) or (9) and finding the pitch number n by which the equality of the equations (6) or (9) is established. In this stage, it may be necessary to consider the fact as to whether or not the equations (6) and (9) are satisfied with another value or solution other than the solution n. Supposing now that one solution of the value n is calculated from the equation (6) as n = n₀, i.e. that the following equation (10) is established: S1 = ℓ + (n o +1)·Δℓ ℓ +n o · Δℓ · S2 + n o · Δℓ ℓ + n o · Δℓ × 1000 Supposing also that another solution of the value n, is obtained from the equation (6) as n = (m≠n₀), the following equation (11) will be established. S1 = ℓ + (m+1) · Δℓ ℓ + m· Δℓ · S2 + m· Δℓ ℓ + m·Δℓ × 1000 In these equations (10) and (11), the values S1 and S2 should be equated, and accordingly, the following equation (12) will be established with respect to the value S1. S1 = ℓ + (n o +1) · Δℓ ℓ + n o · Δℓ ·S2 + n o · Δℓ ℓ + n o · Δℓ × 1000 = ℓ + (m+1) · Δℓ ℓ + m· Δℓ ·S2 + m· Δℓ ℓ + m· Δℓ × 1000 Accordingly, the value S2 is obtained as follows. S2 = ℓ Δℓ × 1000 In comparison with the pitch distnce I and the minute increment ΔI, the following equation (14) will be of course understood. I>ΔI and as described before with reference to FIG. 6, the phase detection voltage S2 of the detecting head will satisfy the following relation. 0 ≦ S2 < 1000 The value S2 of the equation (13) is of course above 1000 as shown hereunder. S2 = ℓ Δℓ × 1000 > 1000 and the equation (13)′ is in conflict with the fact of the equation (15) - This conflict proves that the assumption of the existence n = (≠n₀) is erroneous one, and accordingly this reveals the fact that the value n in the equation (6) has only one solution. It will be easily understood from this fact that the value n in the equation (9) has also only one value, i.e. one solution. As described hereinbefore, it is found that the equation (6) or (9) have only one solution with respect to the pitch numbers, i.e. n in this case, and in the next step, it will be necessary to refer to the degree of the calculation precision with which the calculation of the pitch numbers n should be performed in a case where the calculation is done by the successive iteration method described hereinbefore, and in this invention, this matter is referred to with reference to graphs regarding the output voltages shown in FIGS. 8A and 8B. Referring to the graphs of FIGS. 8A and 8B, the output H1 of the detecting head 41 is designated by a value K₁₁ when the rod 21 moves by pitch number n; that is, the rod moving amount X designates the distance Pn, and when the rod 21 moves by pitch number (n+1), the output H2 of the detecting head 42 is designated by values K₂₁ and K₂₂ corresponding to the values K₁₁, K₁₁ at the distances Pn and Pn+1. Accordingly, it will be found that the difference between the values K₂₁ and K₂₂ is the precision to be obtained. Supposing now that the value S2 is designated K₂₁ and K₂₂ in cases of pitch numbers of n and (n+1), respectively, the equation (6) will be expressed as follows. ℓ + (n+1)· Δℓ ℓ + n· Δℓ · K₂₁ + n· Δℓ ℓ + n· Δℓ × 1000 = ℓ + (n+2)· Δℓ ℓ + (n+1)· Δℓ · K₂₂ + (n+1)· Δℓ ℓ + (n+1)· Δℓ × 1000 With this equation (16), when the pitch number n approaches the maximum value, the following equation (17) will be established. Δℓ ℓ +n· Δℓ ≒ Δℓ ℓ + (n+1)· Δℓ Accordingly, the equation (16) will be alternatively expressed as follows. K₂₁ - K₂₂ = Δℓ · ℓ {ℓ + (n+1)· Δℓ}² × 1000 In an actual calculation is use of concrete numerical values such as, where n max = ℓ Δℓ = 50 When the values of the condition (18) are introduced into the above equation (3), the moving distance Pn of the rod 21, i.e. detectable maximum absolute position P n.max , will be expressed as follows. P n·max = 50· (2000+ 50-1 2 · 40) + 2000+50·40 1000 · S ≒ 15 (cm) When the condition (18) is applied to the equation (16)′, the equation (16)′ is calculated as follows. K₂₁ - K₂₂ = 40·2000 { 2000+ (50+1) ·40 }² · 1000 ≒ 5 (pulses) According to these equations and calculations it is found that the detectable maximum absolute position of the rod 21 is 15 cm under the condition (18); namely, in the case where the minimum resolution of the rod moving amount X is 40 µm, the distance of one pitch I is 2000 µm and the pitch number n is 50. When it is required to obtain or calculate the absolute position Ps of the rod 21, it will be necessary to first obtain the pitch number n by the successive iteration method in use of the equation (6) to which is applied the phase detection voltages S1 and S2 of the detecting heads 41 and 42 or the equation (9) to which is applied the phase detection voltages S3 and S4. In this method, it is found that the obtained pitch number n is a correct value by discriminating the equality of the equation (6) (or the equation (9)) with an error range below 5 pulses as obtained by the equation (22). FIG. 9 is a block diagram representing one embodiment of an apparatus for carrying out the method described hereinbefore according to this invention. Referring to FIG. 9, an exciting power source 51 is operatively connected to a sine wave output unit 52 generating a sine wave signal and a cosine wave output unit 53 generating a cosine wave signal, and the sine wave signal and the cosine wave signal output from the output units 52 and 53 are transmitted to the primary coils 401 and 403 of the detecting heads 41 and 43, respectively. Phase-modulated output signals PM1 and PM2 obtained from the secondary coils 402 and 404 are respectively input into phase detectors 55A and 55B to which is applied an output signal SY from a reference signal generating circuit 56 in synchronism with the exciting power source 51 thereby to carry out the phase detection. The phase detection signals H1 and H2 from the phase detectors 55A and 55B are input into analog-to-digital (A/D) converters 57A and 57B in which the phase detection signals H1 and H2 are converted into digital signals DS1 and DS2, respectively, which are then input into an operation processing unit 59 which comprises a micro-computer and so on. The phase detection signals H1 and H2 are also input into a comparator 58 from the phase detectors 55A and 55B to discriminate the fact as to which one of the signals H1 and H2 is larger in the levels and then to transmit the discriminated signal DS3 from the comparator 58 into the operation processing unit 59. In this embodiment, the phase detection outputs H1 and H2 of the phase detectors 55A and 55B are in parallel digitalized by the A/D converters 57A and 57B, but the outputs H1 and H2 may be output selectively by locating a selector through which the output pass, and in the latter case, the selected one output is digitalized by only one A/D converter. The operation of the apparatus having construction shown in FIG. 9 will be explained hereunder with reference to FIGS. 5A through 5C. As described hereinbefore, the magnetic materials 22A,22B,22C ... and the non-magnetic portions 23 are alternatingly and coaxially disposed on the outer peripheral surface of the rod 21, and as also described with reference to FIG. 1, the output voltages having modulated phases are generated on the secondary coils 5A and 5B as represented by the equation (1) by adding the sine and cosine wave voltages to the primary coils 6A and 6B of the detecting heads. In the similar manner, when the phase-modulated output signals PM1 and PM2 generated from the secondary coils 402 and 404 of the detecting heads 41 and 42 are input into the phase detectors 55A and 55B, the phase detection voltages H1 and H2 shown in FIGS. 5B and 5C are output. When it is now required to obtain the absolute position in a case where the rod 21 moves from the position 0 to the position Ps (i.e. X:O → Ps), the pitch number n is obtained by first substituting the values SS1 and SS2 for the values S1 and S2 in the equation (6). In the next step, when the thus obtained pitch number n and S = SS1 are introduced into the equation (3), the moving distance Pn is calculated as the absolute position Ps. In these steps, since these operations or calculations are carried out by the digital processing, the phase detection signals H1 and H2 are input into the A/D converters 57A and 57B to digitally convert the same, and the thus obtained digital output signals DS1 and DS2 are input into the operation processing unit 59. With the example shown in FIGS. 5A and 5B, since value SS1 is larger than the value SS2(SS1 > SS2), i.e. H1 > H2, the discrimination signal DS3 reaches, for example, "H" level thereby to instruct to operate the equation (6). On the other hand, in case the positional relationship shown in the graphs of FIGS. 7C and 7D, the relation between the values H1 and H2 to be measured becomes H1 < H2, so that the discrimination signal DS3 is represented by "L" level for example, thereby to instruct to operate the equation (9). FIGS. 10A through 10D show another embodiment of this invention which three detecting heads 43, 44 and 45 to improve the operation precision, and accordingly, this embodiment will be available and effective for rendering easy the operations. The detecting heads 44 and 45 are located at positions apart from the detecting head 43 by distance corresponding to two and three pitches, respectively, as shown in FIG. 10A, and FIGS. 10B, 10C and 10D show graphs representing the phase detection voltages H3, H4 and H5 of the detecting heads 43, 44 and 45, respectively. As illustrated, in this embodiment, the differences of the pitches increase gradually in the arranged order of the respective phase detection voltages H3, H4 and H5 so that the operation can be made easily. FIGS. 11A through 11D show a further embodiment according to this invention, in which three detecting heads 46, 47 and 48 are also arranged as shown in FIG. 10A, but at positions different from those shown in FIG. 10A. Namely, in FIG. 11A, the detecting heads 47 and 48 are positioned apart from the detecting head 46 by the distances corresponding to three pitches and five pitches, respectively. The detecting heads 46, 47 and 48 of this embodiment have longitudinal lengths I, (I + ΔI) and (I + 2ΔI), respectively, so that the potential differences between the phase detection output voltages H6, H7 and H8 increase gradually in the arranged order as shown in FIGS. 11B through 11D. Thus, the operation is further made easy and the operation precision is also improved. With the illustrated embodiment, although, for the easy understanding of this invention, the detecting heads 46, 47 and 48 located at the specific positions so that the phases of the respective voltages accord with each other at the starting position of the moving distance X of the rod 21, the absolute position can be detected even if the detecting heads 46, 47 and 48 are located at optional position for the reason that the phases are found on the basis of the phase detection voltages H6, H7 and H8 output by the respective detecting heads 46, 47 and 48 in accordance with the mutual positional relationships therebetween. In the foregoing description, although all the operations or calculations are dealt with in the assumption that the phases detection voltages change linearly, strictly speaking, these voltages do not linearly change in an actual operation. It will be therefore required to correct them in the actual operation, to operate them by approximating to a linear, or to carry out the operation based on the required precision. FIGS. 12A to 12C are examples of a rod for showing arrangements of the magnetic material and the non-magnetic material on the rod. The rod 31 of FIG.12A is made of a magnetic material and a plurality of air gaps are formed as non-magnetic portions at positions having longitudinal widths 1/2, (I + ΔI)/2, (I + 2ΔI)/2, (I + 3ΔI)/3, ... as illustrated in FIG. 12A. The rod 31 of this type is produced with low cost. Referring to FIG. 12B, a magnetic material 35 is spirally wound up around the rod 32 so as to have an increased width rightwardly as viewed in FIG. 12B are a non-magnetic material 38 is formed between the respective spirals of the magnetic material 35. Such technique as winds the magnetic material around the rod member is made possible by producing a plastic made magnetic material in the recent technical development. FIG. 12C shows a further example of the rod 33 made of magnetic material 36 so as to have a spiral groove having a longitudinal width increasing gradually rightwardly. The air gap of the spiral groove is formed as non-magnetic portions which are arranged alternatingly with respect to the magnetive portions 36 of the rod 33. The grooves, i.e. air gaps, shown in FIGS. 12A and 12C may be filled with a non-magnetic material to make smooth the outer peripheral surfaces of the rods 31 and 33 respectively. With the examples shown in FIGS. 12A through 12C, although the magnetic portion and the non-magnetic portion are arranged in equal ratio of areas, the alternation of this ratio is easily made in the present working technique and is of course within the scope of this invention. In addition, it will be easily understood by those skilled in the art that this invention is applicable to a linear magnet scale as well as and also in the foregoing, although the exciting signal is referred to as a sine wave (or cosine wave), signals having other wave shapes such as square waves, triangular waves or the like. According to the method and apparatus of this invention, an absolute position can relatively easily measured or operated by the simple construction with low cost in use of a rod member on which magnetic portions and non-magnetic portions are alternatingly arranged with various patterns. It should be understood that many modifications and adaptations of the invention will become apparent to those skilled in the art.

Claims: A method for detecting an absolute position of a movable member as measured from a reference position comprising the steps of: preparing a rod (21) as the movable member, on which magnetic (22A,22B, ...) and non-magnetic materials are alternatingly arranged along a longitudinal direction of the rod with pitches which are gradually increased by an increment Δℓ so that said pitches are expressed as ℓ, ℓ + Δℓ, ℓ + 2Δℓ, ...; locating first and second detecting heads (41,42) which generate electrical signals corresponding to magnetic resistance along and in parallel with the longitudinal direction of said rod and said first and second detecting heads being separated from each other with a predetermined space; moving the movable member to a position to be measured; detecting and digitally storing in memory means said electrical signals as phase signals (S₁,S₂) transmitted from said first and second detecting heads in response to phasic variation of magnetic resistance which is caused by a relation movement between said rod and said first and second detecting heads in the longitudinal direction thereof; performing a predetermined operation in accordance with said phase signals (S1,S2) and said ℓ, Δℓ and an integer n representing the number of pitches passing said detecting heads to obtain an absolute positional relationship between said rod and said first and second detecting heads (41,42) on the basis of a result of said predetermined operation. A method for detecting an absolute position of a movable member according to claim 1, wherein the following equation is established: S1 - ℓ + (n+1) · Δℓ ℓ + n· Δℓ · S2 + n· Δℓ ℓ + n· Δℓ × 1000 or S1 - S2 - ℓ ℓ ·n· Δℓ × 1000 A method for detecting an absolute position of a movable member according to claim 1, further comprising a third detecting head, wherein the second detecting head is apart from the first detecting head by a distance (2ℓ + Δℓ) and the third detecting head is apart from the first detecting head by a distance (3ℓ + 3Δℓ). A method for detecting an absolute position of a movable member according to claim 1, further comprising a third detecting head, wherein said second detecting head is apart from said first detecting head by a distance (3ℓ + 3Δℓ) and said third detecting head is apart from said first detecting head by a distance (5ℓ + 10Δℓ), and said first, second and third detecting heads have longitudinal lengths ℓ, (ℓ + Δℓ) and (ℓ + 2Δℓ), respectively. An apparatus for detecting an absolute position of a movable member as measured from a reference position, comprising: a rod (21) as the movable member provided at predetermined positions with plural pairs of magnetic (22A,22B, ...) and non-magnetic materials (23) with pitches which are gradually increased by increment Δℓ so that said pitches are expressed as ℓ, ℓ + Δℓ, ℓ + 2Δℓ, ...; first and second detecting heads (41,42) respectively located along and in parallel with said rod in the longitudinal direction thereof so as to generate electrical signals corresponding to magnetic resistance and respectively separated from each other with a space ℓ corresponding to the length of first pitch; first and second phase detectors (55A,55B) connected to said first and second detecting heads respectively to detect said electrical signals as phase signals (S1,S2) therefrom in response to phasic variation of magnetic resistance which is caused by a relation movement between said rod and said first and second detecting heads in the longitudinal direction thereof when the movable member moves to a position to be measured; first and second analog-to-digital converters (57A,57B) connected to said first and second phase detectors respectively to digitize said phase signals therefrom; an operation processing means (59) connected to said first and second analog-to-digital converters to store said phase signals therefrom, and to represent an absolute position (Pn₁) of the movable member by the following two equations S1 - ℓ + (n+1) · Δℓ ℓ + n· Δℓ · S2 + n· Δℓ ℓ + n· Δℓ × 1000 or S1 - S2 - ℓ ℓ ·n· Δℓ × 1000 in which an integer n represents a number of said pitches passing the first and second detecting heads, and to determine the integer n which satisfies said two equations and then to obtain the absolute position through applying the integer n to said one of the equations. A rod adapted for detecting an absolute position, said rod being relatively movable with respect to a plurality of detecting heads disposed along and in parallel with an axial direction of said rod which has a circular outer configuration and which comprises a magnetic material constituting magnetic portions and which is provided with a plurality of gaps constituting non-magnetic portions, and being provided with said magnetic portions and said non-magnetic portions that are alternated in the axial direction of said rod with pitches which are varied by a predetermined length and that are formed spirally on an outer peripheral surface of said rod so that said pitches are successively varied on the peripheral surface.

Inventors: HAKATA YOSHITAMI, IWAMOTO NORIHIRO, SUZUKI KIMIO, TSUBOI HIROYUKI, HAKATA, YOSHITAMI, IWAMOTO, NORIHIRO, SUZUKI, KIMIO, TSUBOI, HIROYUKI
Applicants: TOSHIBA MACHINE CO LTD, TOSHIBA KIKAI KABUSHIKI KAISHA
Application year: 1986
Main classification: G01D5
IPC codes: G01D5, B23Q17, G01B7