GB2107897A - Optical automatic critical focusing device - Google Patents

Optical automatic critical focusing device Download PDF

Info

Publication number
GB2107897A
GB2107897A GB08219994A GB8219994A GB2107897A GB 2107897 A GB2107897 A GB 2107897A GB 08219994 A GB08219994 A GB 08219994A GB 8219994 A GB8219994 A GB 8219994A GB 2107897 A GB2107897 A GB 2107897A
Authority
GB
United Kingdom
Prior art keywords
receiver
transmitter
mirror
optics
optical arrangement
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
GB08219994A
Other versions
GB2107897B (en
Inventor
Rolf Jurenz
Michael Lenk
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.)
Pentacon GmbH Foto und Feinwerktechnik
Original Assignee
Pentacon Dresden VEB
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 Pentacon Dresden VEB filed Critical Pentacon Dresden VEB
Publication of GB2107897A publication Critical patent/GB2107897A/en
Application granted granted Critical
Publication of GB2107897B publication Critical patent/GB2107897B/en
Expired legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B17/00Systems with reflecting surfaces, with or without refracting elements
    • G02B17/08Catadioptric systems
    • G02B17/0896Catadioptric systems with variable magnification or multiple imaging planes, including multispectral systems
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/48Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S17/00
    • G01S7/481Constructional features, e.g. arrangements of optical elements
    • G01S7/4811Constructional features, e.g. arrangements of optical elements common to transmitter and receiver
    • G01S7/4812Constructional features, e.g. arrangements of optical elements common to transmitter and receiver transmitted and received beams following a coaxial path
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B17/00Systems with reflecting surfaces, with or without refracting elements
    • G02B17/08Catadioptric systems
    • G02B17/0804Catadioptric systems using two curved mirrors
    • G02B17/0808Catadioptric systems using two curved mirrors on-axis systems with at least one of the mirrors having a central aperture
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B17/00Systems with reflecting surfaces, with or without refracting elements
    • G02B17/08Catadioptric systems
    • G02B17/0856Catadioptric systems comprising a refractive element with a reflective surface, the reflection taking place inside the element, e.g. Mangin mirrors
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B17/00Systems with reflecting surfaces, with or without refracting elements
    • G02B17/08Catadioptric systems
    • G02B17/0884Catadioptric systems having a pupil corrector
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B7/00Mountings, adjusting means, or light-tight connections, for optical elements
    • G02B7/28Systems for automatic generation of focusing signals
    • G02B7/30Systems for automatic generation of focusing signals using parallactic triangle with a base line
    • G02B7/32Systems for automatic generation of focusing signals using parallactic triangle with a base line using active means, e.g. light emitter

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Optics & Photonics (AREA)
  • Engineering & Computer Science (AREA)
  • Spectroscopy & Molecular Physics (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Radar, Positioning & Navigation (AREA)
  • Remote Sensing (AREA)
  • Measurement Of Optical Distance (AREA)
  • Lenses (AREA)
  • Focusing (AREA)

Abstract

An optical automatic critical focusing arrangement for photographic cameras comprises a transmitting diode 1 and a receiver 5. A small concave mirror 2 is provided on the optical axis between the transmitting diode 1 and the receiver 5, which mirror is irradiated by the transmitting diode 1 arranged at its focal point, and additionally has, as a component of the transmitter optics, a rear surface which is provided with a reflecting coating. The small mirror together with a larger concave mirror 3 arranged on the optical axis, forms a mirror lens as the receiver optics. 6a is an optional cover disc or lens. <IMAGE>

Description

SPECIFICATION Optical automatic critical focussing device The invention relates to an optical automatic critical focusing arrangement, preferably for photographic cameras which operate with infrared transmitting and receiving units.
In connection with photographic cameras, it is known to use the rays emitted by an infra-red radiator provided on the camera for measuring the distance of the object. The distance is determined from the proportion of the radiation reflected on the object, and according to this distance the automatic critical focusing of the taking lens is effected. The radiation is so focused that it can be directed at specific parts of the image field covered by the camere. The disadvantage of this prior art (DE OS 1 965 064) is the large expenditure of optical components since it is necessary to use two separate systems for the transmitting and receiving units, namely two optically collecting members which are symmetrical about the infra-red radiator. In addition, further reflecting means are necessary for the generation of the partial ray bundles.
It is furthermore known (DE AS 1 953 849) to arrange the infra-red radiator in the focal point of a reflector so that parallel light is emitted. Herein, the transmitter and receiver optics are separately arranged on the optical axis one behind the other.
In the centre of the receiver optics, there is provided an opening for the accommodation of the transmitter optics. In accordance with the focal length of the receiver optics, the whole system is very long in construction. Also, focus setting is only possible by selected zones, that is to say in steps.
Another automatic critics' focusing arrangement (DE AS 2 126 1 18) also necessitates a very large expenditure of optical and opto-electronic components, due to the separate arrangement of the transmitting and receiving units in such a way that there is no cooperative combination of the components.
It is the object of the invention to reduce the expenditure of optical and opto-electronic components for the automatic critical focusing of photographic camera and lenses.
The task underlying the invention is to provide a space-saving combined, preferably infra-red radiation transmitter and receiver unit for automatic critical focusing.
According to the invention, the problem is solved in that a small concave mirror, which is irradiated by a transmitting diode arranged in its focus, additionally has as a component of the transmitter optics a rear surface of wi n a reflecting coating has been applied and which, with a larger concave mirror arranged alignedly in the optical axis, simultaneously forms a mirror lens as the receiver optics. According to a constructional form of the invention, the optically active surfaces of the transmitter and receiver optics components have different spherical or aspherical curvatures. Expediently, the larger concave mirror has in its centre a free opening which is simultaneously designed as a socket for the receiver.It is furthermore proposed according to the invention that there should be provided in front of the transmitting diode a cover disc which may be designed as a lens. This lens in front of the transmitter and receiver optics is advantageously so designed that it has different curvatures for the respective ray path. For the performance of the automatic critical focusing, it is necessary that either the transmitter optics or the concave mirror of the receiver optics is displaceable in the longitudinal direction and can be coupled with the focusing control of the taking lens. The transmitter and receiver optics are therefore preferably arranged in the mount housing of the taking lens or in the camera housing. As the material for the mirror parent substances there may be used glass, ceramics, plastics and/or metal materials.In addition, provision is made for the mirror surfaces to be designed as first surface and/or second surface mirrors.
The invention will be explained in more detail hereinafter. In the accompanying drawings Figure 1 a shows a lateral view of the transmitter and receiver according to the invention, including the infra-red radiator, Figures 1 b, c show variants of the lens to be arranged in front of the IR transmitter and receiver, Figure 2 shows the IR transmitter and receiver with the displaceable concave mirror of the receiver optics, Figure 3 shows the IR transmitter and receiver optics, with the transmitter optics displaceable.
In known measuring principles of automatic critical focusing, it is necessary to transmit modulated IR rays on the object to be critically focused. For example, in the phase measurement method, an IR transmitting diode is modulated at a specific frequency. The energy is projected on the object via a transmitter optics and the reflected radiation is imaged on the IR receiving diode by a receiver optics. The phase difference between the alternating current energy emitted by the transmitting diode and the energy recollected by the receiving diode serves as a signal for critical focusing. The sharpness external measurement for the automatic critical focusing of optical systems is characterised in that the taking lens is not part of the measuring principle.
Therefore, the proposed optical system is particularly suitable for the phase measurement method because here a fixed optical arrangement that is independent of the object distance is sufficient and only approximate conditions of sharpness have to be observed for the projection on the object as well as the imaging of the radiation reflected by the object. However, if position-sensitive receivers are used for the method, then a coupling of the transmitter or receiver optics with the taking lens is necessary for realising the conditions of sharpness which are required.
As shown in Fig. 1 a, an IR transmitting diode 1 is arranged in the focus of a small concave mirror 2. So as to be aligned in the optical axis, there is provided behind the small concave mirror 2 a larger concave mirror 3 with a free opening 4, through which a light current can be applied to an IR receiver 5 located therebehind. In front of the IR transmitting and receiving system, including the transmitting diode 1, there is arranged a cover disc 6a, in which there lu located, for example, the socket of the transmitting diode 1. This cover disc 6a may be constructed as a lens 6b (Fig. 1 b). In this connection, it is possible for the optical effect of the lens 6c shown in Fig. 1 c to be different in the transmitting and receiving zones. By this means, optimisation of the concave mirrors 2, 3 can be achieved.For example, the mirror diameters can be kept in smaller dimensions.
The light current emitted by the transmitting diode 1 is preferably guided to an object as a -parallel light beam. The beam cross-section bounds the field of measurement. An Image of the ray proportion reflected by the object is formed on the IR receiver 5 which is in the "fixed focus" setting, via the spherical and/or aspherical surfaces of the concave mirrors 3 and 2, which In all represent a mirror lens, through the free opening 4. It is also possible to transmit the light current from the transmitter at a fixedly set distance as a convergent beam and to set the receiver optics to the same distance. The phase difference between the transmitted and received signals of the modulated IR radiation, which is proportional to the object distance, serves as the criterion of measurement for focusing the taking lens not shown.
The described optical arrangement may be accommodated beside the taking lens either directly in the housing of this lens or in the camera. As regards the electrical signal processing, reference is made to the known prior art.
Fig. 2 shows a variant of the IR transmitter and receiver according to the invention. Herein, the concave mirror 3 of the receiver optics is coupled with the taking lens so as to run in the opposite direction during its movement, and the arrangement is thus usable, for example, for the mentioned method using position-sensitive receivers. In order to observe specific conditions of correction, it is possible to use second surface mirrors having differently curved front and rear surfaces. The variant shown in Fig. 3 allows a displacement of the transmitter optical 2, including the transmittiri 1 diode 1, and during its movement is coupled with the taking lens so as to run in the same direction. The application thereof is also possible in the method given in Fig. 2.
Here, an additional feature is the fact that the free opening 4 in the concave mirror 3 of the receiver optics is simultaneously designed as a mounting part and can accommodate the receiver 5.
If the transmitter is fixed, the concave mirror 3 carrying the receiver 5 can again be coupled with the taking lens so as to run in the opposite direction during its movement.
It is within the scope of the invention that the proposed arrangement can be used not only in the infra-red range but also in other ranges of radiation. Over and above this, the twofold utilisation of the optical components, both for transmitting and for receiving, is of great advantage. In addition to a reduction in components, a minimum of space is required for the installation thereof. The arrangement according to the invention furthermore operates irrespective of the type of taking lens used.

Claims (9)

Claims
1. An optical automatic critical focusing arrangement comprising a transmitter, a receiver, a small concave mirror, which is irradiated by a transmitting diode arranged at its focal point, additionally has as a component of the transmitter optics a rear surface which is provided with a reflecting coating, said small mirror together with a larger concave mirror being alignedly arranged in the optical axis, forms a mirror lens as the receiver optics.
2. An optical arrangement as claimed in Claim 1, wherein the optically active surfaces of the components of the transmitter and receiver optics have different spherical or aspherical curvatures.
3. An optical arrangement as claimed in Claim 2, wherein the concave mirror has in its centre a free opening which is simultaneously designed as a socket for the receiver.
4. An optical arrangement as claimed in Claim 3, wherein in front of the transmitting diode there is provided a cover disc which may be constructed as a lens.
5. An optical arrangement as claimed in Claim 4, wherein the curvatures of the lens in front of the transmitter and receiver optics are different.
6. An optical arrangement as claimed in Claim 5, wherein the transmitter optics or the concave mirror of the receiver optics is displaceable in the longitudinal direction and can be coupled with the focusing control of the taking lens.
7. An optical arrangement as claimed in Claim 2, wherein the mirror parent substances consist of glass, ceramics, plastics and/or metal materials, and in that the mirror surfaces are designed as first surface and/or second surface mirrors.
8. An optical arrangement as claimed in Claim 7, wherein the transmitter and receiver optics are arranged in the mount housing of the taking lens or in the camera housing.
9. An optical arrangement substantially as described with reference to the accompanying drawings.
GB08219994A 1981-10-16 1982-07-09 Optical automatic critical focussing device Expired GB2107897B (en)

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
DD23412981A DD201245A1 (en) 1981-10-16 1981-10-16 OPTICAL ARRANGEMENT FOR AUTOMATIC SHARPENING

Publications (2)

Publication Number Publication Date
GB2107897A true GB2107897A (en) 1983-05-05
GB2107897B GB2107897B (en) 1985-08-21

Family

ID=5534150

Family Applications (1)

Application Number Title Priority Date Filing Date
GB08219994A Expired GB2107897B (en) 1981-10-16 1982-07-09 Optical automatic critical focussing device

Country Status (3)

Country Link
DD (1) DD201245A1 (en)
DE (1) DE3227980A1 (en)
GB (1) GB2107897B (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2122835A (en) * 1982-06-30 1984-01-18 Eastman Kodak Co Rangefinder
WO2009070203A1 (en) * 2007-11-27 2009-06-04 Eastman Kodak Company Dual focal length lens system

Families Citing this family (30)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE102006031580A1 (en) 2006-07-03 2008-01-17 Faro Technologies, Inc., Lake Mary Method and device for the three-dimensional detection of a spatial area
DE102009010465B3 (en) 2009-02-13 2010-05-27 Faro Technologies, Inc., Lake Mary laser scanner
US9551575B2 (en) 2009-03-25 2017-01-24 Faro Technologies, Inc. Laser scanner having a multi-color light source and real-time color receiver
DE102009015920B4 (en) 2009-03-25 2014-11-20 Faro Technologies, Inc. Device for optically scanning and measuring an environment
DE102009035336B3 (en) 2009-07-22 2010-11-18 Faro Technologies, Inc., Lake Mary Device for optical scanning and measuring of environment, has optical measuring device for collection of ways as ensemble between different centers returning from laser scanner
DE102009035337A1 (en) 2009-07-22 2011-01-27 Faro Technologies, Inc., Lake Mary Method for optically scanning and measuring an object
DE102009055989B4 (en) * 2009-11-20 2017-02-16 Faro Technologies, Inc. Device for optically scanning and measuring an environment
US9113023B2 (en) 2009-11-20 2015-08-18 Faro Technologies, Inc. Three-dimensional scanner with spectroscopic energy detector
US9210288B2 (en) 2009-11-20 2015-12-08 Faro Technologies, Inc. Three-dimensional scanner with dichroic beam splitters to capture a variety of signals
US9529083B2 (en) 2009-11-20 2016-12-27 Faro Technologies, Inc. Three-dimensional scanner with enhanced spectroscopic energy detector
DE102009057101A1 (en) 2009-11-20 2011-05-26 Faro Technologies, Inc., Lake Mary Device for optically scanning and measuring an environment
DE102009055988B3 (en) 2009-11-20 2011-03-17 Faro Technologies, Inc., Lake Mary Device, particularly laser scanner, for optical scanning and measuring surrounding area, has light transmitter that transmits transmission light ray by rotor mirror
US9607239B2 (en) 2010-01-20 2017-03-28 Faro Technologies, Inc. Articulated arm coordinate measurement machine having a 2D camera and method of obtaining 3D representations
US9628775B2 (en) 2010-01-20 2017-04-18 Faro Technologies, Inc. Articulated arm coordinate measurement machine having a 2D camera and method of obtaining 3D representations
US9879976B2 (en) 2010-01-20 2018-01-30 Faro Technologies, Inc. Articulated arm coordinate measurement machine that uses a 2D camera to determine 3D coordinates of smoothly continuous edge features
CN102687433A (en) 2010-01-20 2012-09-19 法罗技术股份有限公司 Portable articulated arm coordinate measuring machine and integrated electronic data processing system
DE102010020925B4 (en) 2010-05-10 2014-02-27 Faro Technologies, Inc. Method for optically scanning and measuring an environment
DE102010032726B3 (en) 2010-07-26 2011-11-24 Faro Technologies, Inc. Device for optically scanning and measuring an environment
DE102010032725B4 (en) 2010-07-26 2012-04-26 Faro Technologies, Inc. Device for optically scanning and measuring an environment
DE102010032723B3 (en) 2010-07-26 2011-11-24 Faro Technologies, Inc. Device for optically scanning and measuring an environment
DE102010033561B3 (en) 2010-07-29 2011-12-15 Faro Technologies, Inc. Device for optically scanning and measuring an environment
DE102012100609A1 (en) 2012-01-25 2013-07-25 Faro Technologies, Inc. Device for optically scanning and measuring an environment
DE102012107544B3 (en) 2012-08-17 2013-05-23 Faro Technologies, Inc. Optical scanning device i.e. laser scanner, for evaluating environment, has planetary gears driven by motor over vertical motor shaft and rotating measuring head relative to foot, where motor shaft is arranged coaxial to vertical axle
DE112013004369T5 (en) 2012-09-06 2015-06-11 Faro Technologies, Inc. Laser scanner with additional detection device
CN104620129A (en) 2012-09-14 2015-05-13 法罗技术股份有限公司 Laser scanner with dynamical adjustment of angular scan velocity
US9513107B2 (en) 2012-10-05 2016-12-06 Faro Technologies, Inc. Registration calculation between three-dimensional (3D) scans based on two-dimensional (2D) scan data from a 3D scanner
DE102012109481A1 (en) 2012-10-05 2014-04-10 Faro Technologies, Inc. Device for optically scanning and measuring an environment
US10067231B2 (en) 2012-10-05 2018-09-04 Faro Technologies, Inc. Registration calculation of three-dimensional scanner data performed between scans based on measurements by two-dimensional scanner
DE102015122844A1 (en) 2015-12-27 2017-06-29 Faro Technologies, Inc. 3D measuring device with battery pack
CN109814084B (en) * 2019-03-11 2021-02-12 上海禾赛科技股份有限公司 Laser radar system

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB2122835A (en) * 1982-06-30 1984-01-18 Eastman Kodak Co Rangefinder
WO2009070203A1 (en) * 2007-11-27 2009-06-04 Eastman Kodak Company Dual focal length lens system
US7573654B2 (en) 2007-11-27 2009-08-11 Eastman Kodak Company Dual focal length lens system
CN101874218A (en) * 2007-11-27 2010-10-27 伊斯曼柯达公司 Dual focal length lens system
CN101874218B (en) * 2007-11-27 2012-09-26 伊斯曼柯达公司 Dual focal length lens system

Also Published As

Publication number Publication date
DE3227980A1 (en) 1983-05-05
GB2107897B (en) 1985-08-21
DD201245A1 (en) 1983-07-13

Similar Documents

Publication Publication Date Title
GB2107897A (en) Optical automatic critical focusing device
KR100258710B1 (en) Solid catadioptric lens
EP0152418B1 (en) A night vision instrument with electronic image converter
US5288987A (en) Autofocusing arrangement for a stereomicroscope which permits automatic focusing on objects on which reflections occur
EP0768542B2 (en) Optical distance measuring apparatus
US4087689A (en) Boresighting system for infrared optical receiver and transmitter
US4664515A (en) Optical system of a radiation thermometer
ES8704271A1 (en) Airborne optoelectrical target detection, localisation and omnidirectional tracking system.
US4634255A (en) Focus detection apparatus
US3745347A (en) Telescope including an imaging system for radiation in the visible range
WO2002075348A3 (en) Omni-directional radiation source and object locator
US4370551A (en) Focus detecting device
EP0201036A2 (en) Automatic focusing apparatus
US4188102A (en) Mirror reflex camera with electronic rangefinder
US6388738B1 (en) Rangefinder optical system
US5069549A (en) Moire contouring camera
US4549802A (en) Focus detection apparatus
US4533226A (en) Still or motion picture camera
JPS57154206A (en) Focusing device
US4618762A (en) In-focus position detecting apparatus
JPS6342761B2 (en)
DE69630997T2 (en) Autofocus device
JP2001027704A (en) Prism optical system
JPH0714835Y2 (en) Radiation thermometer
US4389107A (en) Focusing device for cameras

Legal Events

Date Code Title Description
PCNP Patent ceased through non-payment of renewal fee