GB2116313A - Sine wave generator for position encoder - Google Patents

Sine wave generator for position encoder Download PDF

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Publication number
GB2116313A
GB2116313A GB08205558A GB8205558A GB2116313A GB 2116313 A GB2116313 A GB 2116313A GB 08205558 A GB08205558 A GB 08205558A GB 8205558 A GB8205558 A GB 8205558A GB 2116313 A GB2116313 A GB 2116313A
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GB
United Kingdom
Prior art keywords
pattern
axis
sinusoidal
optical
aperture
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
GB08205558A
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GB2116313B (en
Inventor
Douglas James Rogers
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Ferranti International PLC
Original Assignee
Ferranti PLC
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Ferranti PLC filed Critical Ferranti PLC
Priority to GB08205558A priority Critical patent/GB2116313B/en
Priority to DE19833305921 priority patent/DE3305921A1/en
Priority to FR8302903A priority patent/FR2522164A1/en
Priority to JP2863783A priority patent/JPS58157203A/en
Publication of GB2116313A publication Critical patent/GB2116313A/en
Application granted granted Critical
Publication of GB2116313B publication Critical patent/GB2116313B/en
Expired legal-status Critical Current

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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01DMEASURING NOT SPECIALLY ADAPTED FOR A SPECIFIC VARIABLE; ARRANGEMENTS FOR MEASURING TWO OR MORE VARIABLES NOT COVERED IN A SINGLE OTHER SUBCLASS; TARIFF METERING APPARATUS; MEASURING OR TESTING NOT OTHERWISE PROVIDED FOR
    • G01D5/00Mechanical means for transferring the output of a sensing member; Means for converting the output of a sensing member to another variable where the form or nature of the sensing member does not constrain the means for converting; Transducers not specially adapted for a specific variable
    • G01D5/26Mechanical 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 characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light
    • G01D5/32Mechanical 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 characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light
    • G01D5/34Mechanical 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 characterised by optical transfer means, i.e. using infrared, visible, or ultraviolet light with attenuation or whole or partial obturation of beams of light the beams of light being detected by photocells
    • G01D5/36Forming the light into pulses
    • G01D5/366Particular pulse shapes

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  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optical Transform (AREA)
  • Optical Elements Other Than Lenses (AREA)

Abstract

Optical means for generating a sinusoidal waveform having a low harmonic content includes a first member 17 bearing at least one pattern 11 of optical transmissivity which varies sinusoidally along an axis (14). A second member 18 carries at least one aperture 13 of width along the axis (14) lying between one quarter and three quarters of the wavelength of the sinusoidal pattern. A light-sensitive device is provided which is responsive to light passing through the aperture and the pattern from a light source, and means are provided for producing relative motion between the two members in a direction parallel to the axis (14), the signal being indicative of the relative position (displacement) of the members. One member may be circular for rotational motion. A further sinusoidal pattern 90 DEG displaced from those shown enable direction of movement to be determined. The pattern 11 may be provided by a shaped opaque strip, a variable density film or coating, or a member of parallel lines of ranging mark/space ratio. <IMAGE>

Description

SPECIFICATION Optical means for generating a sinusoidal waveform having a low harmonic content Optical means are frequently used for generating electrical signal waveforms which are subsequently processed by electronic circuitry.
Position encoders are one example of instruments using such means, and usually comprise two relatively movable members each carrying a pattern of some sort. A light source and a lightsensitive device co-operate with the two members to produce an electrical signal which may be used to determine the direction and extent of relative movement of the two members.
For most purposes a square-wave electrical signal is suitable, particularly if it is being used to operate digital circuitry. However, there are situations in which complex analog electronic circuitry is used to operate on the signals. In such circumstances it is preferable for the opticailyderived electrical signal to be sinusoidal, with as low a harmonic content as possible.
According to the invention there is provided optical means for generating a sinusoidal waveform having a low harmonic content, which includes a first member bearing a pattern of optical transmissivity which varies sinusoidally along an axis, a second member bearing an aperture having a width along said axis of between one-quarter and three-quarters of the wavelength of said sinusoidal pattern, a lightsensitive device responsive to light passing through said aperture and said pattern from a light source, and means for producing relative motion between said first and second members in a direction parallel to said axis.
Also according to the invention there is provided a position encoder which includes means as specified in the preceding paragraph in which the first member is carried by one of two bodies movable relative to one another in a direction parallel to said axis, and in which the second member is carried by the other of the two bodies.
The invention will now be described with reference to the accompanying drawings, in which: Figure 1 shows the form of the pattern on the first member; Figure 2 illustrates the optical arrangement; Figure 3 shows a practical form of the invention; Figure 4 shows detail of an alternative form of the embodiment of Figure 3; Figure 5 shows part of a shaft encoder incororating the invention.
Referring now to Figure 1 ,the first member 10 of opaque material I or carrying an opaque coating, has formed on it a pattern in the form of a variable-width slit 11 with sine-wave edges. A second member 12 has formed in it an aperture 13 having a width equal to about one-half of a wave-length of the sinusoidal pattern. If the two members are moved relative to one another in a direction parallel to the length of the slit 11, as indicated by the arrow 14, then the amount of light passing through both the pattern and the slit will vary in a sinusoidal manner.
Figure 2 shows the other components necessary to generate a sinusoidal electrical signal. The two members 10 and 12 are arranged adjacent and parallel to one another with a light source 1 5 on one side and a light-sensitive device 1 6 on the other side. Such arrangements are well known, and optical elements such as lenses have been omitted.
In order to generate the required waveform it is necessary to produce the relative motion between the two members. This is most easily done by making one of them in the form of a disc, which may then be rotated whilst the other member is stationary. Since the aperture 13 is easiler to form it is convenient to produce a disc bearing a number of apertures, whilst the stationary member carries the sinusoidal pattern. Figure 3 shows such an arrangement, with a stationary member, or index, illustrated at 1 7 and the rotatable disc or scale at 1 8.
In practice, in order to avoid errors due to unevenness of the light source or of the response of the light-sensitive device over its sensitive area, it is convenient to have a number of apertures in the scale overlapping a number of sinusoidal patterns on the index. The centres of the apertures must be spaced apart by the wavelength of the pattern so that the variations of light passing through each aperture are in phase with one another. In the case of a rotating scale the apertures must be arranged radiaily, and not exactly parallel to one another, and the sinusoidal patterns must be similarly arranged with wavelengths matched to the spacing of the apertures. Figure 4 shows part of such a scale and index. As shown in Figure 4, the index 1 7 carries three sinusoidal patterns 11 arranged parallel to one another.The scale 18, of which only part is shown has a number of apertures 13, four in the case illustrated, each of which extends over one half-cycle of each of the sinusoidal patterns. A single light-sensitive device responds to the light passing through all four apertures. This is a known technique for removing such errors. It is also possible to apply known techniques for removing d.c. offset voltages from the sinusoidal output. One technique involves using the same light-sensitive device to respond also to light passing through a second set of sinusoidally-varying strips. These co-operate with a set of slots arranged so that the variations in light received by the light-sensitive device from the two sets of strips are in anti-phase.
The width of the apertures 1 3 need not be exactly one-half of the wavelength of the sinusoidal pattern. Widths between one-quarter and three-quarters of a wavelength are suitable, but the centres of the apertures must be one wavelength apart. The particular advantage of the half-wavelength aperture is the complete cancellation of the even harmonics from the output of the detector and in the reduction of the odd harmonics by a factory equal to their harmonic number. The presence of harmonics is due to imperfections in the shape of the sinusoidal pattern. Other slit widths reduce the harmonic content by a lesser extent.
As has already been suggested, the sinewavegenerating means described above may be used as a position encoding device. In the case of the embodiment of Figures 3 and 4, these may be used as shaft angle encoders, using appropriate electronic circuitry. However, in order to determine direction of rotation of the disc, it is necessary to add a further pattern, or set of patterns. These are also sinusoidal envelopes, but displaced by one-quarter of a wavelength so as to provide, in conjunction with a separate set of apertures and a separate light-sensitive device, a cosine wave output The combination of the sine and cosine waveforms enables the direction of rotation of the disc to be determined. Figure 5 shows the relevant parts of the scale and index for a shaft encoder producing sine and cosine outputs.A similar arrangement may be used for a linear position encoder, in which case the scale is a straight elongated member with parallel apertures, rather than a disc bearing radial apertures.
The required sinusoidally-varying optical transmissivity required may be provided by other means than the transparent strip with sinusoidal edges. For example, it is possible to produce the same effect using a number of parallel lines of varying mark/space ratio. Alternatively a film or coating having sinusoidally-varying density may be used.
It will be appreciated that the requirement for producing a low harmonic sine wave depends upon relative movement between the two members referred to, and it does not matter which of them is moved and which is stationary. The sine (or cosine) waveform produced is very low in harmonic content and may be processed electronically with little or no distortion.

Claims (10)

1. Optical means for generating a sinusoidal waveform having a low harmonic content, which includes a first member bearing a pattern of optical transmissively which varies sinusoidally along an axis, a second member bearing an aperture having a width along said axis of between one-quarter and threequarters of the wavelength of said sinusoidal pattern, a lightsensitive device responsive to light passing through said aperture and said pattern from a light source, and means for producing relative motion between said first and second members in a direction parallel to said axis.
2. Optical means as claimed in Claim 1 in which the pattern of sinusoidally-varying optical transmissivity comprises a variable width transparent strip having edges formed by two sinusoidal waveforms of the same wavelength and in antiphase.
3. Optical means as claimed in either of Claims 1 or 2 in which one of said first and second members is in the form of a rotatable disc the other member being stationary relative to the disc.
4. Optical means as claimed in Claim 3, in which the stationary member is the first member carrying said pattern, the rotatable disc carrying a plurality of apertures the centres of which are spaced apart from one another by the wavelength of said pattern.
5. Optical apparatus as claimed in any one of the preceding claims in which each aperture has a width along said axis of one-half of the wavelength of the sinusoidal pattern.
6. Optical apparatus as claimed in any one of Claims 1 to 5 in which the first member carries a number of sinusoidal patterns in phase with one another, part of each pattern being aligned simultaneously with said aperture.
7. Optical means substantially as herein described with reference to Figures 1 to 4 of the accompanying drawings.
8. A position encoder which includes optical means as claimed in any one of the preceding claims in which the first member is carried by one of two bodies movable relative to one another in a direction parallel to said axis and in which the second member is carried by the other of said two bodies.
9. A position encoder as claimed in Claim 8 in which the first member also carries a second pattern of optical transmissivity which varies sinusoidally along the said axis, the first and second patterns being 900 out of phase with one another.
10. A position encoder substantially as herein described with reference to Figure 5 of the accompanying drawings.
GB08205558A 1982-02-25 1982-02-25 Sine wave generator for position encoder Expired GB2116313B (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
GB08205558A GB2116313B (en) 1982-02-25 1982-02-25 Sine wave generator for position encoder
DE19833305921 DE3305921A1 (en) 1982-02-25 1983-02-21 OPTICAL DEVICE FOR GENERATING A SINUS-SHAPED WAVE SHAPE WITH A LOW PART OF HARMONIOUS
FR8302903A FR2522164A1 (en) 1982-02-25 1983-02-23 OPTICAL MEANS FOR FORMING A LOW HARMONIC SINUSOIDAL SIGNAL, APPARATUS AND POSITION ENCODER THEREFOR
JP2863783A JPS58157203A (en) 1982-02-25 1983-02-24 Optical device for generating sinusoidal wave of low harmonic wave content

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
GB08205558A GB2116313B (en) 1982-02-25 1982-02-25 Sine wave generator for position encoder

Publications (2)

Publication Number Publication Date
GB2116313A true GB2116313A (en) 1983-09-21
GB2116313B GB2116313B (en) 1985-09-04

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Family Applications (1)

Application Number Title Priority Date Filing Date
GB08205558A Expired GB2116313B (en) 1982-02-25 1982-02-25 Sine wave generator for position encoder

Country Status (4)

Country Link
JP (1) JPS58157203A (en)
DE (1) DE3305921A1 (en)
FR (1) FR2522164A1 (en)
GB (1) GB2116313B (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5332896A (en) * 1991-11-04 1994-07-26 Dr. Johanness Heidenhain Gmbh Instrument for producing harmonics-free periodic signals
US5726445A (en) * 1995-06-22 1998-03-10 Dr. Johannes Heidenhain Gmbh Device for obtaining harmonic-free signals
EP1111345A2 (en) * 1999-12-23 2001-06-27 Dr. Johannes Heidenhain GmbH Position measuring device
US6914235B2 (en) 2001-06-27 2005-07-05 Dr. Johannes Heidenhain Gmbh Position measuring system and method for operating a position measuring system
GB2432662A (en) * 2005-11-28 2007-05-30 Avago Tech Ecbu Ip Optical encoder
US7312436B2 (en) 2004-08-31 2007-12-25 Dr. Johannes Heidenhain Gmbh Optical position measuring system with a detector arrangement and measuring graduation to produce partial filtering of undesired harmonics

Families Citing this family (10)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2549280B2 (en) * 1986-04-15 1996-10-30 ファナック 株式会社 Rotary Encoder
JPH01196515A (en) * 1988-02-01 1989-08-08 Fuji Electric Co Ltd Photoelectric conversion type rotary position detector
DE59104264D1 (en) * 1991-11-04 1995-02-23 Heidenhain Gmbh Dr Johannes Device for generating harmonic-free periodic signals.
DE59105538D1 (en) * 1991-12-20 1995-06-22 Heidenhain Gmbh Dr Johannes Photoelectric device for generating harmonic-free periodic signals.
CH690971A5 (en) * 1994-02-25 2001-03-15 Hera Rotterdam Bv Methods for measuring and exploitation of a shift of a scanning head with respect to a measuring scale and optical encoders for performing this method.
DE19830294C2 (en) * 1998-07-07 2000-12-07 Fraba Ag Measuring device
DE19962525B4 (en) * 1999-12-23 2013-11-21 Continental Automotive Gmbh Optical torque sensor
JP2008241243A (en) * 2005-06-30 2008-10-09 Mitsubishi Electric Corp Optical encoder
JP6032924B2 (en) * 2011-04-13 2016-11-30 キヤノン株式会社 Encoder
JP5755010B2 (en) 2011-04-14 2015-07-29 キヤノン株式会社 Encoder

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3814934A (en) * 1972-11-10 1974-06-04 Gilbert & Barker Mfg Co Pulse generating apparatus responsive to shaft rotation

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5332896A (en) * 1991-11-04 1994-07-26 Dr. Johanness Heidenhain Gmbh Instrument for producing harmonics-free periodic signals
US5726445A (en) * 1995-06-22 1998-03-10 Dr. Johannes Heidenhain Gmbh Device for obtaining harmonic-free signals
EP1111345A2 (en) * 1999-12-23 2001-06-27 Dr. Johannes Heidenhain GmbH Position measuring device
EP1111345A3 (en) * 1999-12-23 2002-08-07 Dr. Johannes Heidenhain GmbH Position measuring device
US6452159B2 (en) 1999-12-23 2002-09-17 Johannes Heidenhain Gmbh Position measuring system
US6914235B2 (en) 2001-06-27 2005-07-05 Dr. Johannes Heidenhain Gmbh Position measuring system and method for operating a position measuring system
US7312436B2 (en) 2004-08-31 2007-12-25 Dr. Johannes Heidenhain Gmbh Optical position measuring system with a detector arrangement and measuring graduation to produce partial filtering of undesired harmonics
GB2432662A (en) * 2005-11-28 2007-05-30 Avago Tech Ecbu Ip Optical encoder
US7399956B2 (en) 2005-11-28 2008-07-15 Avago Technologies Ecbuip Pte Ltd Optical encoder with sinusoidal photodetector output signal
GB2432662B (en) * 2005-11-28 2009-09-23 Avago Tech Ecbu Ip Optical encoder
CN1975340B (en) * 2005-11-28 2010-05-12 安华高科技Ecbuip(新加坡)私人有限公司 Optical encoder with sinusoidal photodetector output signal

Also Published As

Publication number Publication date
DE3305921A1 (en) 1983-09-01
GB2116313B (en) 1985-09-04
JPS58157203A (en) 1983-09-19
FR2522164A1 (en) 1983-08-26

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Legal Events

Date Code Title Description
732 Registration of transactions, instruments or events in the register (sect. 32/1977)
PCNP Patent ceased through non-payment of renewal fee

Effective date: 19940225