IP Library › Granted Patent US 10,725,155
Granted Patent B2
US 10,725,155 · App. 15/579,288 · Granted Jul 28, 2020

Method for measuring a distance

Inventors: Peter Rieger (Grossau, AT); Andreas Ullrich (Gablitz, AT)
Assignee: RIEGL LASER MEASUREMENT SYSTEMS GMBH
G01S7/484G01S7/497G01S13/20G01S13/227G01S17/06G01S17/10G01S17/42
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Quick Facts
Patent No.
US 10,725,155
App. No.
15/579,288
Granted
Jul 28, 2020
Kind
B2
Abstract

The present invention relates to a method for measuring the distance of targets in the surroundings by way of a time-of-flight measurement of pulses, in particular laser pulses, reflected at said targets, said pulses each being successively emitted at a transmission time in accordance with a predeterminable pulse repetition rate and said pulses, after the reflection thereof, each being received at a reception time, said method comprising the following steps: selecting a first pulse repetition rate from a set of at least two different pulse repetition rates and predetermining the selected pulse repetition rate for the emission, ascertaining a transmission time lying closest in time to the reception time of a reflected pulse and a time interval between these, and, if the ascertained time interval drops below a predetermined first threshold, selecting a second pulse repetition rate from the set and predetermining the second pulse repetition rate for the emission.

Claims (18)

1. A method for measuring the distance of a target by way of time-of-flight measurements on pulses reflected at said targets, said pulses being successively emitted in accordance with a predeterminable pulse repetition rate, each pulse being emitted at a transmission time and after reflection at said target, being received at a reception time, comprising:

selecting a first pulse repetition rate from a set of at least two different pulse repetition rates and predetermining the selected first pulse repetition rate as pulse repetition rate for the emission of the pulse;

for at least one of the reception times, ascertaining a transmission time lying closest in time to said reception time, and ascertaining a time interval between said reception time and the ascertained transmission time;

and, if the ascertained time interval is below a first threshold, selecting a second pulse repetition rate from the set and predetermining the selected second pulse repetition rate as the pulse repetition rate for the emission of the pulses;

wherein a reciprocal value of a greatest pulse repetition rate from the set and a reciprocal value of a smallest pulse repetition rate from the set differ from one another by at least twice the first threshold.

2. The method according to claim 1 , wherein, if the ascertained transmission time lies before reception time, a next-greatest pulse repetition rate or, if there is no such pulse repetition rate, a smallest pulse repetition rate from the set is selected as said second pulse repetition rate,

and, if the ascertained transmission time lies after said reception time, a next-smallest pulse repetition rate or, if there is no such pulse repetition rate, a largest pulse repetition rate from the set is selected as said second pulse repetition rate.

3. The method according to claim 2 , wherein, if the ascertained time interval exceeds a second threshold which is greater than the first threshold, a next-greatest or greatest pulse repetition rate from the set is selected as said second pulse repetition rate.

4. The method according to claim 1 , wherein, if the ascertained time interval exceeds a second threshold, which is greater than the first threshold, a next-greatest or greatest pulse repetition rate from the set is selected as said second pulse repetition rate.

5. The method according to claim 1 , wherein the pulses are laser pulses.

6. A method for measuring the distance of a target by way of time-of-flight measurements on pulses reflected at said target, said pulses being successively emitted in accordance with a predeterminable pulse repetition rate, each pulse being emitted at a transmission time and after reflection at said target, being received at a reception time, comprising:

selecting a first pulse repetition rate from a set of at least two different pulse repetition rates and predetermining the selected first pulse repetition rate as pulse repetition rate for the emission of the pulse;

for at least one of the reception times, ascertaining a transmission time lying closest in time to said reception time, and ascertaining a time interval between said reception time and the ascertained transmission time;

and, if the ascertained time interval is below a first threshold, selecting a second pulse repetition rate from the set and predetermining the selected second pulse repetition rate as the pulse repetition rate for the emission of the pulses;

wherein, if the ascertained time interval exceeds a second threshold, which is greater than the first threshold, a next-greatest or greatest pulse repetition rate from the set is selected as said second pulse repetition rate.

7. The method according to claim 6 , wherein, if the ascertained transmission time lies before reception time, a next-greatest pulse repetition rate or, if there is no such pulse repetition rate, a smallest pulse repetition rate from the set is selected as said second pulse repetition rate,

and, if the ascertained transmission time lies after said reception time, a next-smallest pulse repetition rate or, if there is no such pulse repetition rate, a largest pulse repetition rate from the set is selected as said second pulse repetition rate.

8. The method according to claim 6 , wherein the pulses are laser pulses.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Dec 4, 2017
From: RIEGER, PETER; ULLRICH, ANDREAS
To: RIEGL LASER MEASUREMENT SYSTEMS GMBH
Reel/Frame 044285/0755 →
Priority Claims (1)
AT 50491/2015 · Jun 15, 2015 · national
Continuity (1)
Related Publication 20180224528A1 · Aug 9, 2018
Cited By (1)
US 12,481,042