Method and apparatus for electrooptical distance measurement

• US 4,553,836 A
• Filed: 08/30/1982
• Issued: 11/19/1985
• Est. Priority Date: 09/29/1981
• Status: Expired due to Fees

• Current Assignee: Kern & Company AG Ch-5001 Aarau Switzerland
• Original Assignee: Kern AG
• Inventors: Meier, Dietrich, Minder, Hans-Ulrich
• Primary Examiner(s): Buczinski, S. C.
• Assistant Examiner(s): Sotomayor, John B.
• Application Number:
  US06/412,496
• Time in Patent Office: 1,177 Days
• Field of Search: 356/5, 343/17.1 R, 343/13 R
• US Class Current: 356/5.03
• CPC Class Codes: G01S 17/14 wherein a voltage or current pulse is initiated and terminated in accordance with the pulse transmission and echo reception respectively, e.g. using counters
• CPC Class Codes: G01S 7/497 Means for monitoring or calibrating
• CPC Class Codes: G04F 10/00 Apparatus for measuring unknown time intervals by electric means
• CPC Class Codes: G04F 10/04 by counting pulses or half-cycles of an ac G04F10/005 takes precedence

Abstract

With an electrooptical distance meter impulses of light are transmitted over the distance. The distance is found by counting the duration of gating signals which last between transmission and reception of the light impulses. 10,000 times of travel generated by a first digital circuit (16, 17, 18) are communicated to a second digital circuit (1, 19, 20) for storing and processing. The distance is computed by the second circuit (1, 19, 20) by forming a mean value from the more frequent counts. By evaluation of artificial gating signals of various durations and by generation of gating signals from the light impulses by means of various threshold levels an improved accuracy of distance measurement is achieved, even when measuring on natural, non cooperative objects.

Claims

1. A method for electrooptical measurement of the distance between an object (22) and a reference point (5,10), whereby impulses of light are transmitted from a transmitter (3) to the object (22) and back to a photoelectric receiver (12) near to the transmitter (3) and whereby pairs of electrical signal impulses (45, 49) corresponding to the instants of transmission and of reception of the light impulses are generated by means of said photoelectric receiver (12) to obtain the time of travel of said light impulses for computing said distance, comprising the steps

(a) generating signals (46) which last between the occurrence of at least two different threshold values at mutually corresponding edges of said pairs of signal impulses (45, 49),

(b) gating, by means of said gating signals (46) for each threshold value, a gate (18), said gate (18) passing the output of a frequency stabilized clock-oscillator (17) on to a frequency-counter (18), while the switching instants of the gate (18) and the impulses of the clock-oscillator (17) are uncorrelated,

(c) calculating, for each threshold value, a corresponding duration of gating signals by the weighted mean of the more frequent counts of said frequency-counter (18), and

(d) obtaining a characteristic time of travel of said light impulses for said distance from the dependence of said calculated duration of gating signals upon the threshold value.

2. A method as claimed in claim 1, further comprising the steps

(a) establishing a first threshold value with an order of magnitude equal to the maximum noise level of said photoelectric receiver (12),

(b) adjusting the noise level of said receiver (12) by changing its operating point until the frequency of occurrence of erroneous results for the time of travel of the light impulses due to noise impulses, is below a given level,

(c) calculating, from the counts for said first threshold value, a corresponding duration of gating signals,

(d) calculating, from the counts for a second threshold value equal to about twice the first threshold value, a second duration of gating signals, and

(e) obtaining a characteristic time of travel of the light impulses from a duration of gating signals corresponding to a threshold value zero by means of linear extrapolation from said first and second pairs of threshold values and gating signals.

3. A method as claimed in claim 2, wherein the characteristic time of travel is obtained from said first duration of gating signals by adding a fixed correction value to the duration, no gating signal being available for the second threshold value.

4. A method for electrooptical measurement of the distance between an object (22) and a reference point (5,10), whereby impulses of light are transmitted from a transmitter (3) to the object (22) and back to a photoelectric receiver (12) near to the transmitter (3), and whereby pairs of electrical signal impulses (45, 49) corresponding to the instants of transmission and of reception of the light impulses are generated by means of said photoelectric receiver (12) to obtain the time of travel of said light impulses for computing said distance and whereby the photoelectric receiver (12-18) is disabled after transmission of a light impulse by means of a disabling signal (43) of presetable duration to suppress noise and interfering signals, the time of travel of the light impulses being obtained from the duration of gating signals (46) occurring between each pair of signal impulses (45, 49), and additive constant error C occurring at the count of the duration of the gating signals (46) due to a gating characteristic differing leading and trailing edge of the gating signal, comprising the steps

(a) gating, by means of auxiliary impulses of constant period T, a gate (16,18) passing the output of a frequency stabilized clock-oscillator (17) on to a frequency-counter (18), while the switching instants of the gate (16,18) and the impulses of the clock-oscillator (17) are uncorrelated and the disabling signal (43) is preset to a duration mT (m>

0, integer),

(b) calculating by the weighted mean of the more frequent counts of said frequency counter (18) a duration mT+C,

(c) gating the gate (16,18) as in (a) but with the disabling signal (43) preset to a duration nT (n>

m, integer),

(d) calculating as in (b) a duration nT+C and

(e) calculating the constant error C by the difference ##EQU2##

5. An apparatus for electrooptical distance measurement with a means for transmitting impulses of light, a receiving means for converting said light impulses into corresponding electrical signal impulses as well as a first digital circuit (16, 17, 18) for generating a count of the time between pairs of said electrical signal impulses (45, 49), corresponding to the instants of transmission and of reception of the light impulses, at least two of said counts being used for computing said distance, the apparatus comprising a second digital circuit (1, 19, 20) for transmitting auxiliary signals to the first digital circuit (16, 17, 18), for receiving said counts from the first circuit, for storing, forming a mean value from correcting and generating a distance value from the counts, as well as for generating start-signals (42) for transmission of said impulses of light.

6. An apparatus as claimed in claim 5, comprising a second digital circuit (1, 19, 20) transmitting to the first digital circuit (16, 17, 18) calibrating impulses for measurement of time duration, at least two different threshold values for generating duration of gating signals from said pairs of signal impulses as well as disabling signals (43) to suppress undesired count-stop signals.

7. An apparatus as claimed in claim 5 or in claim 6, comprising a limiter circuit (34) in front of the first digital circuit (16, 17, 18), said limiter circuit (34) limiting the pairs of electrical signal impulses (45, 49) to a preset level prior to evaluation.