Method and apparatus for electrooptical distance measurement

• US 4,274,736 A
• Filed: 09/26/1979
• Issued: 06/23/1981
• Est. Priority Date: 10/11/1978
• Status: Expired due to Term

• Current Assignee: Kern AG
• Original Assignee: Kern AG
• Inventors: Balmer, Beat
• Primary Examiner(s): Buczinski, Stephen C.
• Application Number:
  US06/079,102
• Time in Patent Office: 636 Days
• Field of Search: 343/12 R, 343/7 A, 356/5
• US Class Current: 356/5.13
• CPC Class Codes: G01S 17/36 with phase comparison between the received signal and the contemporaneously transmitted signal
• CPC Class Codes: G01S 7/4915 Time delay measurement, e.g. operational details for pixel components signal extraction and conditioning G01S7/493; Phase measurement
• CPC Class Codes: G01S 7/497 Means for monitoring or calibrating

Abstract

With an electrooptical distance meter a reference signal is timeshifted by means of an electronic phase shifter (20), until it has a given phase relation to the measurement signal. Both signals are compared in phase by a double balanced mixer (22), the output of which directs the electronic phase shifter (20) by a control loop (20, 22, 23). The phase shift is measured after frequency conversion by two additional double balanced mixers (24, 25). Thus handy precision distance meters with measurement frequencies about 500 MHz may be built, comprising control loops for laser diode transmitter (1), avalanche diode receiver (13), phase shifter (20) and intermediate frequency, as well as a processor (5, 29) control for automatic function of the instrument.

Claims

1. A method for electrooptical distance measurement, whereby a beam of modulated light is transmitted over the distance and after reception is converted into an electrical signal corresponding to the modulation of light, said signal being compared with respect to time with reference signal used for modulating the light beam, at least one of said signals being shifted with respect to the other one until a given time relation between the signals is reached, and the distance being found from the extent of said signal shift, comprising the steps

(a) mixing for temporal comparison the signal converted from the modulated light and the reference signal used for modulating the light beam,

(b) time-shifting the reference signal by means of a control circuit and a driving signal obtained from said mixing step, until a given time relation with respect to the converted signal is reached,

(c) frequency converting to a lower frequency the shifted as well as the unshifted reference signals, and

(d) measuring the temporal difference of the frequency-converted reference signals to determine the temporal shift of the reference signal obtained in said time-shifting step.

2. A method as claimed in claim 1, wherein from the strength of the received modulated light a regulating signal is derived for regulating, by means of a control circuit (2), the strength of the transmitted modulated light in such a way that the strength of the received light is convenient for signal processing.

3. An apparatus for electrooptical distance measurement with a means for transmitting continuously modulated light, a receiving means for converting said modulated light into an electrical signal corresponding to the modulation of light, as well as a means for comparing, with respect to time, said converted signal with a reference signal used for modulating said light transmitting means, means for changing by a measurable amount the temporal shift between said converted signal and reference signal including means for obtaining the distance from said measured temporal signal shift, the apparatus comprising a first double balanced mixer (22) for temporal comparison of converted signal and reference signal, an electronic phase shifter (20) for time-shifting the reference signal, a local oscillator (27) and two double balanced mixers (24, 25) for frequency-converting respectively the shifted and the unshifted reference signals, as well as a phase meter (28) for the frequency-converted reference signals.

4. An apparatus as claimed in claim 3, comprising a control circuit (20, 22, 23) wherein the electronic phase shifter (20) is driven by the output of the first double balanced mixer (22).

5. An apparatus as claimed in claim 3, comprising an optical means (6 to 12) for directing the modulated light from the transmitting means (1) over the distance to the receiving means (13), an optical means (6, 7, 11, 12) for directing the modulated light from the transmitting means (1) over a known reference distance to the receiving means (13), and an optical switching means (15, 16) for respectively opening and closing the measured distance and the reference distance alternately.

6. An apparatus as claimed in claim 3, with the receiving means comprising a silica-avalanche-photodiode (13) and a temperature sensing means (14) for generating a diode bias voltage depending on temperature.

7. An apparatus as claimed in claim 3, with the receiving means comprising a silica-avalanche-photodiode (13) and a control means (14) for regulating a diode bias voltage in order to maintain a given amount of intrinsic noise in the diode output.

8. An apparatus as claimed in claim 3, with the transmitting means comprising a laser diode (1) as well as a means (2) for stabilizing, limiting and regulating in dependence on temperature the DC bias current of the laser diode (1).

9. An apparatus as claimed in claim 8, comprising a power detector (56) for the received modulated light and a sample-hold stage switched to the power detector for regulating the DC bias current of the laser diode (1).

10. An apparatus as claimed in claim 4, wherein the control circuit (20, 22, 23) comprises an integrator (33) switched to the output of the first double balanced mixer (22) and a means (34) for forming the absolute value of the integrated signal in order to match it to the regulating range of the electronic phase shifter (20).

11. An apparatus as claimed in claim 8, comprising an interference filter (12) arranged in the optical ray path in front of the receiving means (13) and matched to the spectral width of the laser diode (1).

12. An apparatus as claimed in claim 3, comprising a grey wedge (6) arranged in the optical ray path in front of the transmitting means (1) for setting a convenient optical signal strength for the receiving means (13).

13. An apparatus as claimed in claim 3, comprising a frequency synthesizer (3) and a filter network selecting from the output of the synthesizer a harmonic component with respect to the fundamental frequency for modulating the transmitting means (1).

14. An apparatus as claimed in claim 13, wherein the frequency synthesizer (3) and the filter network may produce each one of a series of different modulating frequencies within the microwave range.

15. An apparatus as claimed in claim 14, wherein said local oscillator (27) for frequency converting is controlled and arranged within a controlling loop in such a way that for each modulating frequency the frequency-converted reference signals all have one and the same frequency.

16. An apparatus as claimed in claim 14, wherein said means for obtaining the distance comprise a processor means (29) for computing the distance from the output of said phase meter (28) for the series of modulating frequencies and from measured data of temperature, air pressure and partial water pressure.

17. An apparatus as claimed in claim 5 or 14 or 16, wherein said means (5, 29) for obtaining the distance may be used to direct the modulated light over the known optical reference path by means of the optical switching means (15, 16), to set a modulating frequency by means of the frequency synthesizer (3), to register the time-shift between converted signal and reference signal by means of the phase meter (28), to repeat this process for the optical measurement path and for both reference and measurement paths for the remaining modulating frequencies, and to compute the distance from the registered time-shifts by means of the processor means (29).