CN2168235Y - Photoelecto receiving device of second-imaging - Google Patents

Photoelecto receiving device of second-imaging Download PDF

Info

Publication number
CN2168235Y
CN2168235Y CN 93216877 CN93216877U CN2168235Y CN 2168235 Y CN2168235 Y CN 2168235Y CN 93216877 CN93216877 CN 93216877 CN 93216877 U CN93216877 U CN 93216877U CN 2168235 Y CN2168235 Y CN 2168235Y
Authority
CN
China
Prior art keywords
photoelectric
utility
model
light target
imaging
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.)
Expired - Fee Related
Application number
CN 93216877
Other languages
Chinese (zh)
Inventor
王广志
丁海曙
董德康
丁辉
宋华
刘明哲
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.)
Tsinghua University
Original Assignee
Tsinghua University
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 Tsinghua University filed Critical Tsinghua University
Priority to CN 93216877 priority Critical patent/CN2168235Y/en
Application granted granted Critical
Publication of CN2168235Y publication Critical patent/CN2168235Y/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Images

Landscapes

  • Length Measuring Devices By Optical Means (AREA)

Abstract

The utility model belongs to the technical field of photoelectric detection. The utility model works out a photoelectric receiving device of second-imaging, which is composed of a scattered light target, an optical imaging lens and a photoelectric position sensor in sequence of cross spread on the same axial line. The device can use the present small-scale photoelectric sensing device to work out a large size light target for meeting the actual needs and the utility model can meet a variety of needs of the photoelectric detection field. The utility model has the advantages of simple structure, low cost, favorable optical switching efficiency and favorable capability of resisting disturbance. Continuous high-precision detection of the displacement change of measured objects can be realized.

Description

Photoelecto receiving device of second-imaging
The utility model belongs to photoelectric detection technology field, particularly the Photoelectric Detection receiving trap.
Photoelectric detecting technology has been widely used in various fields at present, and for example in athletic training, military training and a lot of engineering survey work, (or displacement) situation that need collimate measurand is accurately measured.Be that beam launcher and measurand are fixed together, can launch parallel beam continuously through focusing on, this light beam irradiates forms hot spot to the light target of receiving trap, and convert the position of hot spot to the electric signal relevant with the position, can obtain change in location (displacement) situation of measurand again through signal Processing.
Prior art receives mainly in the following ways the photoelectricity of measurand displacement detecting: thus the hot spot that (a) adopts TV camera that the light beam that is sent by emitter is formed on target is taken and is write down this point and rock situation, isolate the position from TV signal then, the equipment complexity of this method, can not in time feed back measurement result, and precision is relatively poor; (b) directly form light target with photoelectric device, the facula position that light beam is formed on target carries out record.It can be divided into two kinds of continous way and arrays according to the photoelectric device difference of use again, and continous way is to adopt planar photoelectric device to constitute light target, therefore requires the area of photoelectric device bigger; Array is to adopt a plurality of point-like photoelectric device dense arrangement to constitute light target, by encoded recording hot spot rocking on target, needs a lot of devices in order to obtain bigger light target like this.
The purpose of this utility model is to overcome the deficiency of prior art photoelectric receiving arrangement, design a kind of photoelectric receiving arrangement of secondary imaging, utilize less photoelectric receiving device to receive the situation of change of inner light beam position in a big way, make device have advantages such as volume is little, cost is low, and is applied widely.
The utility model is designed a kind of photoelectric receiving arrangement, it is characterized in that by the scattering light target 1 of perpendicular array, optical imaging lens 2 and photoelectrical position sensor 3 are formed successively on same axis, distance between said light target, lens, the sensor is respectively u, v, and satisfied with focal length of lens f:
1/ (u)+1/ (v)=1/ (f), and establish u>2f.
By rationally choosing u, v, the value of f can utilize existing small size optoelectronic sensor to design the large scale light target that corresponds to actual needs, and realizes that the small size photoelectric sensor receives the situation of change of measurand position in a big way.
The utility model is designed a kind of ABSORPTION AND SCATTERING formula optical imaging screen as light target, has high conversion rate and good accuracy to satisfy receiving beam.
Light target described in the utility model is coated with anti-reflection surface layer 13 by optical glass substrate 12 at this substrate front surface, and its rear surface is made scattering surface layer 14 and constituted.In order to guarantee its conversion efficiency, substrate should be selected the optical glass high to the specific wavelength transmitance of used light source for use, for example, when light source selects for use centre wavelength to be the infrared laser of 930mm, can select near infrared cut-off type glass, as HB820 etc.If select for use the red laser pipe do light source then should select the penetrating characteristic of ruddiness good and to the glass of other wavelength attenuation.Like this, guaranteed high conversion rate on the one hand, also made light target have the ability of anti-interference of stray light preferably simultaneously.In order further to improve the conversion efficiency and the antijamming capability of target surface, be coated with suitable film system in the place ahead of optical glass substrate, its effect has two; Being anti-reflection on the one hand, is that parasitic light is decayed on the other hand, and these two effects are to reach by material and thickness that the choose reasonable film is.Above-mentioned two layers of material makes target surface possess good absorption characteristic, can be for incident light is converted to by the pointolite of optical lens imaging, incident light need be carried out scattering, prepare the scattering surface layer at the rear of optical glass for this reason, can adopt general glass frosting technology or laser frosted to make frosting.The characteristic of desirable scattering surface layer is can be with the complete scattering of incident light, forms pointolite, and therefore CONTROL PROCESS subtly when preparation scattering surface layer makes the scattering surface layer have fully thin stochastic distribution structure.
Photoelectric receiving device described in the utility model adopts any photoelectric device that can detect the hot spot coordinate, as the CCD device, and four-quadrant device or photovoltaic array etc.For further improving the precision of photodetector system, preferably adopt the photoelectric sensor of continuous type, as the semiconductor silicon optical device.Photoelectric receiving device should be placed on the position that its photosurface just in time overlaps with the imaging surface of light target scattering hot spot.
The utility model has realized utilizing existing less photoelectric receiving device to be received in the change in location situation of interior tested light beam in a big way.The light target of this device has good conversion efficiency and antijamming capability, and the continuous type optoelectronic sensor of selecting for use can guarantee the accuracy of detection of whole photodetector system to the measurand displacement.This apparatus structure is simple, and is with low cost, can be used among the photoelectric displacement detection system in various fields.
Brief Description Of Drawings:
Fig. 1 forms synoptic diagram for the utility model
Fig. 2 is a light target structural drawing of the present utility model
Fig. 3 is an embodiment overall construction drawing of the present utility model
The utility model is designed a kind of secondary imaging photoelectric receiving arrangement embodiment, and general structure is made up of trumpet type receiving basin 34 and support 35 as shown in Figure 3.The big end of receiving basin is installed light target 31, small end is installed a continuous type photoelectric sensor 33, on the axis of light target and the formation of photoelectric sensor photosurface, an optical lens 32 is installed, light target is u=10v with the photoelectric sensor photosurface to lens distance v ratio to lens distance u, photoelectric sensor photosurface diameter is 10mm, the light target diameter is 100mm, and focal length of lens f is 25mm.

Claims (2)

1, a kind of photoelectric receiving arrangement, it is characterized in that by the scattering light target 1 of perpendicular array, optical imaging lens 2 and photoelectrical position sensor 3 are formed successively on same axis, distance between said light target, lens, the sensor is respectively u, v, and satisfied with focal length of lens f:
1/ (u)+1/ (v)=1/ (f), and establish u>2f;
2, photoelectric receiving arrangement according to claim 1 is characterized in that described light target by the optical glass substrate, is coated with anti-reflection surface layer at this substrate front surface, and its rear surface is made the scattering surface layer and constituted.
CN 93216877 1993-06-30 1993-06-30 Photoelecto receiving device of second-imaging Expired - Fee Related CN2168235Y (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN 93216877 CN2168235Y (en) 1993-06-30 1993-06-30 Photoelecto receiving device of second-imaging

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN 93216877 CN2168235Y (en) 1993-06-30 1993-06-30 Photoelecto receiving device of second-imaging

Publications (1)

Publication Number Publication Date
CN2168235Y true CN2168235Y (en) 1994-06-08

Family

ID=33796935

Family Applications (1)

Application Number Title Priority Date Filing Date
CN 93216877 Expired - Fee Related CN2168235Y (en) 1993-06-30 1993-06-30 Photoelecto receiving device of second-imaging

Country Status (1)

Country Link
CN (1) CN2168235Y (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2004106850A1 (en) * 2003-06-01 2004-12-09 Zhiyong Xie Photoelectric sensor
CN106595478A (en) * 2016-12-09 2017-04-26 北京无线电计量测试研究所 Light spot position detector

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2004106850A1 (en) * 2003-06-01 2004-12-09 Zhiyong Xie Photoelectric sensor
CN106595478A (en) * 2016-12-09 2017-04-26 北京无线电计量测试研究所 Light spot position detector

Similar Documents

Publication Publication Date Title
CN108490419A (en) A kind of vehicle-mounted multi-line laser radar system of automatic Pilot
CN109983312A (en) Optical system for the range information in collecting field
CN108291968A (en) Three-dimensional LIDAR system with field of regard
CN117872318A (en) Lidar receiver using waveguide and aperture
WO2021056668A1 (en) Dynamic distance measurement system and method
CN101427203A (en) Detection circuit for detecting movements of a movable object
CN102135393A (en) Measurement system for motion parameters of high-speed motion object
CN101013030A (en) Microlen array based laser beam divegence angle testing method
CN101738243A (en) Method for detecting reflective liquid level displacement based on angular displacement tracking
CN207833020U (en) A kind of laser radar scanning imaging system
US9395296B1 (en) Two-dimensional optical spot location using a one-dimensional detector array
Beraldin et al. Optimized position sensors for flying-spot active triangulation systems
CN108051005A (en) The single PSD detection methods of Target space position and posture
EP0041146A1 (en) Method and apparatus for determination of angle incidence of electromagnetic energy
US6985239B2 (en) Position-sensing device for 3-D profilometers
CN1297823C (en) Portable meter scattering laser radar concurrently used for day and night and detection method thereof
CN110297228A (en) A kind of laser radar reception camera lens
CN106768874A (en) X-ray focusing optical focusing performance measuring device
CN105973073B (en) Automatic scoring round target device
CN2168235Y (en) Photoelecto receiving device of second-imaging
CN208421217U (en) A kind of optical receiving system
CN110879385A (en) Non-scanning laser radar receiving optical system
CN102706444B (en) Method for measuring topological charges of optical vortex
WO2010148389A2 (en) Light funnel
JP2001201369A (en) Photoelectron system

Legal Events

Date Code Title Description
C14 Grant of patent or utility model
GR01 Patent grant
C19 Lapse of patent right due to non-payment of the annual fee
CF01 Termination of patent right due to non-payment of annual fee