Optoelectronic distance measuring device

Radiant energy – Photocells; circuits and apparatus – Photocell controlled circuit

Reexamination Certificate

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Details

C250S2140LA, C250S559290, C250S2140RC, C330S308000, C330S059000, C356S004010, C356S005010

Reexamination Certificate

active

06710324

ABSTRACT:

BACKGROUND OF THE INVENTION
The invention relates to an optoelectronic distance measuring device comprising at least one transmitter unit to transmit pulsed electromagnetic radiation, at least one receiver unit associated with the transmitter unit to receive the reflected radiation and an evaluation unit to determine at least the distance of objects reflecting the transmitted radiation.
Such devices are generally known and are used, for example, in connection with vehicles to detect the surroundings of the vehicle during travel.
The occurrence of objects with very different reflectivity which result in amplitudes of the received pulses on the receiver unit which vary correspondingly strongly is problematic. A near object of high reflectivity such as a so-called cat's eye or a road boundary post, which is also termed a cooperative target, on the one hand, and a far object of low reflectivity such as a tree or a person in dark clothing, on the other hand, can differ from one another in practice with respect to the intensity, and thus to the received signal amplitude of the radiation reflected by them, by a factor of 10
6
or more.
A receiver unit which should cover such an extremely wide dynamic range will necessarily overmodulate at high intensities. The width of the received pulses decisive for a distance measurement using a pulse transit time process depends on the amplitude of the received radiation pulses. This relationship can be comparatively uncritical in the non-overmodulated or analog range, i.e. for radiation pulses not exceeding a specific intensity or amplitude, but can result in inaccuracies in the distance determination at high intensities, with such inaccuracies being able to lie in the range of some meters.
In connection with this problem it is know, for example, to use amplifiers with a logarithmic characteristic curve with which large amplitudes can be reproduced in a manner reduced in a logarithmic scale. The deformation of the pulse which takes place here and which can result in inaccuracies in the distance measurement is disadvantageous so that such amplifiers are only suitable for applications without a high accuracy requirement.
SUMMARY OF THE INVENTION
It is the object of the invention, starting from an optoelectronic distance measurement device of the kind initially named, to provide a possibility, in particular with distance determination, to at least reduce such inaccuracies to a minimum which occur due to different intensities of the reflected radiation, wherein this should in particular be possible over the total dynamic range occurring in practice.
This object is satisfied in that a series connection of load resistors is connected after the receiver unit and a separate amplifier is associated with each load resistor to amplify the subsidiary pulse produced at the respective load resistor from an incoming, successively attenuated received pulse.
In accordance with the invention, a plurality of signal pulses, termed subsidiary pulses here, with a reducing signal level are produced from each receiver pulse produced at the receiver unit, with these signal pulses being amplified by an arrangement of parallel amplifiers, with a separate amplifier being associated with each subsidiary pulse. Consequently, a plurality of parallel measuring channels are available at the same time which differ in that the received pulses, that is the subsidiary pulses, are of different signal levels.
Depending on the initial signal level of a received pulse produced at the receiver unit, a subsidiary pulse is produced at one of the load resistors which is not overmodulated subsequent to its amplification; that is, its signal level remains below an overmodulating threshold. The subsidiary pulses produced at the previous load resistors before this first, non-overmodulated, amplified subsidiary pulse are subjected to a pulse widening due to their amplification which results in overmodulation which would result in inaccuracies or at least in problems in a distance measurement taking place using a pulse transit time process. The invention allows these overmodulated amplified subsidiary pulses to be suppressed and to subject a non-overmodulated amplified subsidiary pulse to a subsequent evaluation.
Since, in accordance with the invention, a plurality of measuring channels are available, provision is automatically made for a measuring channel to exist for every signal level of an initial received pulse, that is, for every intensity of a reflected radiation pulse, in which an optimum evaluation of the received pulse is possible which is free of disturbing overmodulation effects, in that it is not the initial received pulse itself which is evaluated, but a subsidiary pulse produced from this which has a reduced signal level due to the attenuation by one or more load resistors, but which still contains the information required for a distance measurement using the transit time principle.
In accordance with the invention, the initial received pulse in a certain sense, and in dependence on its signal level, itself finds that measuring channel in which it can be evaluated without problem in the form of an attenuated subsidiary pulse which is, however, particularly not falsified with respect to the required information.
An extremely wide dynamic range can consequently be covered by the invention. Both near targets with a high reflectance and far targets of low reflectivity can be measured without problem and without compromises in the accuracy and speed of the distance measurement.
The measuring device in accordance with the invention can consequently be used to particular advantage in connection with laser scanners, for example in the areas of traffic engineering, automobile sensor technology and industrial surveying, and in particular anywhere special target marks of high reflectivity should be measured, on the one hand, and normal objects or the surroundings should be measured simultaneously, on the other hand, and are scanned for this purpose. Possible applications are, for example, navigation and safety with automatic transport vehicles when reflectors of known location have to be identified for the part task “navigation” and objects with low reflectance must also not be overlooked for the part task “safety”. Possible further applications are, for example, measurements on liquid metals where bare metal surfaces and dark ash regions alternate in rapid succession.
The invention moreover allows reflectivity measurements in that, with knowledge of the object distance, a conclusion is made on the intensity of the radiation pulse received, and thus on the reflectivity of the object in question, from the signal level of a non-overmodulated and therefore non-widened amplified subsidiary pulse, with the known properties of the measuring channel in question, that is, the degree of attenuation due to the respective load resistors and the characteristic values of the respective amplifier, allowing a conclusion on the signal level of the initial received pulse.
The invention can be advantageously combined with a double pulse evaluation in which received pulses successively incoming in a short time interval of the same transmitted pulse transmitted by the transmitter unit are evaluated with regard to the transit time in order, for example, to measure the upper edge of a container standing on the floor separately from the floor itself. Widenings of the received pulse due to overmodulation are avoided by the invention such that even received pulses lying close to one another in time can be separated from one another and no problems occur due to deformations or suppressions of the later received pulses by widened earlier received pulses.
Provision is preferably made for the resistance values of the load resistors to reduce in succession starting from the receiver unit.
Furthermore, the ratios of the resistance values of the load resistors to one another are preferably matched to the dynamic ranges of the amplifiers.
The matching of the resistance values to the properties, and in particular to th

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