The present patent application claims the priority of European patent application 22 167 168.8 filed on Apr. 7, 2022, the disclosure of which is incorporated by reference in the present patent application in its entirety.
The disclosure relates to a method and a device for examining the environment of a vehicles by analyzing echo signals of transmitted ultrasonic signals, generated by reflection at an object in the environment of the vehicle.
Ultrasonic measuring systems for examining of the environment of a vehicle, e.g. during a parking process, are generally known (see e.g. WO 02/45998 A2 and WO 2014/180609 A1). In these measuring systems, an ultrasonic transmitter transmits ultrasonic burst signals which have a defined number of ultrasonic pulses following each other at a frequency. If objects are present in the environment of the vehicle into which the ultrasonic burst signal has been transmitted, echo signals are generated by the same because of reflections, which echo signals are received by an ultrasonic receiver. Typically, transmitting and receiving ultrasonic signals is performed by one and the same element, namely an ultrasonic transmitter.
With the known systems, it is possible, e.g., to determine the distance of an object from the vehicle.
However, it is sometimes desired to be able to determine more information about the detected object, namely, for example, the speed thereof relative to the vehicle.
It is an object of the disclosure to provide a method and a device for examining the environment of the vehicle for the existence of potential objects, it being possible to determine a plurality of parameters characterizing the object.
In order to achieve the object, the disclosure proposes a method for examining the environment of a vehicle by analyzing echo signals of transmitted ultrasonic signals, generated by reflection at an object in the environment of the vehicle, wherein in the method
According to the disclosure, at least two different ultrasonic burst signals are respectively transmitted in repeatedly occurring measuring cycles. These signals differ at least with respect to their lengths, i.e. with respect to their number of pulses, for example. Here, a comparatively short ultrasonic burst signal is used, so as to be able to determine the location at which an object was detected in the environment of the vehicle and the distance of the object from the vehicle based on the echo of said signal. With a certain time offset from the time of transmission of the short ultrasonic burst signal a signal peak occurs in the demodulated echo signal (envelope), wherein the distance of the object from the vehicle can then be calculated from the speed of sound. The longer ultrasonic burst signal is used to be able to calculate the velocity of the object relative to the vehicle in the propagation direction of the ultrasonic burst signal based on the analysis of a Doppler frequency shift in the echo signal. Thus, the spectral (Doppler) shift of this signal in the environment of the object is determined using the second ultrasonic burst signal.
Dividing a measuring cycle into two measuring phases (one measuring phase for the short ultrasonic burst signal and the second measuring phase for the long ultrasonic burst signal) has the advantage that now objects can also be detected in close proximity, if, as is typically the case nowadays, one unit, namely an ultrasonic transducer is used for the ultrasonic transmitter and the ultrasonic receiver.
Phase shifts which can be caused by a plurality of reflectors (for example, swinging arms of a pedestrian), can basically simulate any velocity. However, these are averaged out, as it were, over the length of the long ultrasonic burst signal.
The order in which the two ultrasonic burst signals of different length are transmitted and evaluated, is interchangeable. The measuring phases advantageously follow each other immediately. The time offset determined between the transmission of the short ultrasonic burst signal and the reception of the echo signal peak indicating the existence of an object, can be used in the longer measuring phase to define the position in the echo signal of the longer ultrasonic burst signal at which the echo signal section is to be examined that results from the Doppler shift caused by a movement of the object. The time between the reception of both echo signals is sufficiently short, so that it can be assumed that the object has barely moved on between both measurements.
The advantages of the disclosure can be summarized as follows:
In practical tests, the disclosure was extensively tested for its suitability for everyday use. In this context, it has shown that the ultrasonic burst signal with the lower number of pulses advantageously comprises 10 to 20 pulses, in particular 16 pulses, and/or a length of 190 μs to 380 μs, in particular 300 μs, and the ultrasonic burst signal with the higher number of pulses advantageously comprises 170 to 220 pulses, in particular 190 pulses, and/or a length of 3.2 ms to 4.0 ms, in particular 3.6 μs. In the practical tests, it has shown that the two ultrasonic burst signals should differ with respect to their length and pulse number by the factor 8 to 15 and preferably by the factor 10.
Typically, the analysis of the echo signals is performed using a signal processing unit.
Thus, according to the disclosure, different ultrasonic burst signals are transmitted. However, this does not necessarily mean that the different signals are necessarily transmitted separately. It is also possible to transmit a single ultrasonic burst signal, but to divide the same into, e.g., two or even more sections and to consider each of these sections as an ultrasonic burst signal in the sense of the disclosure, as it were.
The above object is further achieved, according to the disclosure, with a device for examining the environment of a vehicle by analyzing echo signals of transmitted ultrasonic signals, generated by reflection at an object in the environment of the vehicle, the device comprising:
The disclosure is explained in more detail below by means of an example and with reference to the drawing. In the Figures:
In order to clarify the method, the demodulated signals 22, 26 and 24, 28, i.e. the envelopes. are superposed in the diagram in
Hereinafter, an example of the evaluation of both echo signals 26, 28 will be described.
First, the echo peaks of the short echo signal 26 which are above the specified threshold value 30 are determined. In a second step, the portion (plateau 34) in the long echo signal 28 is determined, in which the Doppler calculation is to be performed.
Due to various considerations, it is advantageous to directly calculate the Doppler calculation from the complex time signals, based on the calculation of the center of gravity of the spectrum (first spectral moment).
The method starts from the complex envelope signal which is present in the sensor in a time-discrete form:
V
k
=I
k
+jQ
k.
For the evaluation portion, the following sum is formed:
The velocity results from the angle of R, as well as the wavelength λ and the sampling frequency Tsample:
If the calculation of R is performed not only for the duration of the long signal upon exceeding the threshold, but is performed across all values for the entire duration of the measurement, this corresponds to the center of the Doppler shift in the volume sensed by the sensor. Since, even without a clear obstacle, a significant signal portion above the threshold value is reflected by the ground (clutter), the velocity of the vehicle can be determined in this manner. If a plurality of obstacles is present, the one with the highest amplitude will be dominant. For a more detailed explanation thereof and of the entire method, V will be represented as polar coordinates.
V=|V|e
jΦ
For R, this results in (for simplicity, without correction term):
The phase difference in the exponent approximately describes the frequency at the position k:
The frequency components are thus weighted by the square of their amplitudes.
Number | Date | Country | Kind |
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22167168.8 | Apr 2022 | EP | regional |