GB1308957A - Methods and apparatus for determining the distance of an object - Google Patents
Methods and apparatus for determining the distance of an objectInfo
- Publication number
- GB1308957A GB1308957A GB1348470A GB1348470A GB1308957A GB 1308957 A GB1308957 A GB 1308957A GB 1348470 A GB1348470 A GB 1348470A GB 1348470 A GB1348470 A GB 1348470A GB 1308957 A GB1308957 A GB 1308957A
- Authority
- GB
- United Kingdom
- Prior art keywords
- light
- incident
- frequency
- varied
- beams
- 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
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B9/00—Measuring instruments characterised by the use of optical techniques
- G01B9/02—Interferometers
- G01B9/02055—Reduction or prevention of errors; Testing; Calibration
- G01B9/02075—Reduction or prevention of errors; Testing; Calibration of particular errors
- G01B9/02078—Caused by ambiguity
- G01B9/02079—Quadrature detection, i.e. detecting relatively phase-shifted signals
- G01B9/02081—Quadrature detection, i.e. detecting relatively phase-shifted signals simultaneous quadrature detection, e.g. by spatial phase shifting
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO 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
- G01S17/00—Systems using the reflection or reradiation of electromagnetic waves other than radio waves, e.g. lidar systems
- G01S17/02—Systems using the reflection of electromagnetic waves other than radio waves
- G01S17/06—Systems determining position data of a target
- G01S17/08—Systems determining position data of a target for measuring distance only
- G01S17/32—Systems determining position data of a target for measuring distance only using transmission of continuous waves, whether amplitude-, frequency-, or phase-modulated, or unmodulated
- G01S17/34—Systems determining position data of a target for measuring distance only using transmission of continuous waves, whether amplitude-, frequency-, or phase-modulated, or unmodulated using transmission of continuous, frequency-modulated waves while heterodyning the received signal, or a signal derived therefrom, with a locally-generated signal related to the contemporaneously transmitted signal
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01B—MEASURING LENGTH, THICKNESS OR SIMILAR LINEAR DIMENSIONS; MEASURING ANGLES; MEASURING AREAS; MEASURING IRREGULARITIES OF SURFACES OR CONTOURS
- G01B2290/00—Aspects of interferometers not specifically covered by any group under G01B9/02
- G01B2290/70—Using polarization in the interferometer
Landscapes
- Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- General Physics & Mathematics (AREA)
- Computer Networks & Wireless Communication (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Instruments For Measurement Of Length By Optical Means (AREA)
Abstract
1308957 Measuring displacements PHILIPS ELECTRONIC & ASSOCIATED INDUSTRIES Ltd 20 March 1970 [25 March 1969] 13484/70 Heading G4H If in a Michelson type interferometer the frequency or other parameter of the incident light is varied about an average value, the number of zero crossings of the intensity during a fixed time period is proportional to the displacement of one mirror with the respect to the other, and to the modulating frequency. Thus by counting the number of zero crossings the distance between the two mirrors may be measured. Light incident from a source 1 on a Michelson type interferometer passes via beam splitter 3, through quarter-wave plates 21 and 28. In this way the light passing through 28 comprises two beams of circularly polarized light which combine to form a single beam of linearly polarized light whose plane polarization is rotated with respect to that of the incident light, the angle of rotation being proportional to the displacement of the mirror 7. The light may be monitored by means of polarizer 23 and photodetechtor 25 whose output feeds into counter 26, and polarizer 24 whose angle is at 90 degrees to that of 23, and photo-electric detector 27 which also feeds into counter 26. The light incident at 1 may comprise two linearly polarized beams with planes of polarization at 90 degrees. The frequency of the incident light may be varied, or the frequencies of the two incident beams may be different, and the difference frequency may be varied.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
NL6904621A NL6904621A (en) | 1969-03-25 | 1969-03-25 |
Publications (1)
Publication Number | Publication Date |
---|---|
GB1308957A true GB1308957A (en) | 1973-03-07 |
Family
ID=19806529
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB1348470A Expired GB1308957A (en) | 1969-03-25 | 1970-03-20 | Methods and apparatus for determining the distance of an object |
Country Status (5)
Country | Link |
---|---|
BE (1) | BE747836A (en) |
CH (1) | CH520319A (en) |
FR (1) | FR2035878B1 (en) |
GB (1) | GB1308957A (en) |
NL (1) | NL6904621A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2129124A (en) * | 1982-10-16 | 1984-05-10 | Ferranti Plc | Aligning mask with body |
GB2256480A (en) * | 1991-06-05 | 1992-12-09 | Marconi Gec Ltd | Optical sensor |
Families Citing this family (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR2468099A1 (en) * | 1979-10-17 | 1981-04-30 | Anvar | METHOD AND APPARATUS FOR LASER INTERFEROMETRY WITH TWO WAVE LENGTHS |
DD201191B1 (en) * | 1981-09-24 | 1987-07-15 | Ilmenau Tech Hochschule | KIPPINVARIANT INTERFEROMETER WITH LEVELS MIRROR |
GB2127960B (en) * | 1982-09-29 | 1985-12-11 | British Aerospace | Ring laser gyroscope readout arrangements |
Family Cites Families (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
FR1086053A (en) * | 1953-07-02 | 1955-02-09 | Csf | Improvements to frequency-modulated telemetry systems |
US3366954A (en) * | 1966-11-04 | 1968-01-30 | Air Force Usa | Spectrographical range finder |
AU409380B2 (en) * | 1966-12-06 | 1971-01-07 | Improvements in or relating to optical mixing devices |
-
1969
- 1969-03-25 NL NL6904621A patent/NL6904621A/xx unknown
-
1970
- 1970-03-20 GB GB1348470A patent/GB1308957A/en not_active Expired
- 1970-03-23 CH CH435870A patent/CH520319A/en not_active IP Right Cessation
- 1970-03-23 BE BE747836D patent/BE747836A/en unknown
- 1970-03-24 FR FR7010533A patent/FR2035878B1/fr not_active Expired
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2129124A (en) * | 1982-10-16 | 1984-05-10 | Ferranti Plc | Aligning mask with body |
GB2256480A (en) * | 1991-06-05 | 1992-12-09 | Marconi Gec Ltd | Optical sensor |
GB2256480B (en) * | 1991-06-05 | 1995-02-01 | Marconi Gec Ltd | Improvements to optical sensors |
Also Published As
Publication number | Publication date |
---|---|
NL6904621A (en) | 1970-09-29 |
FR2035878B1 (en) | 1974-09-20 |
CH520319A (en) | 1972-03-15 |
BE747836A (en) | 1970-09-23 |
DE2012946A1 (en) | 1970-10-01 |
DE2012946B2 (en) | 1975-07-24 |
FR2035878A1 (en) | 1970-12-24 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
PS | Patent sealed [section 19, patents act 1949] | ||
PCNP | Patent ceased through non-payment of renewal fee |