Method and measuring device for fill level measurement

Patent metadata

Field	Value
Publication number	US-10295394-B2
Application number	US-201214366310-A
Country	US
Kind code	B2
Filing date	Nov 22, 2012
Priority date	Dec 20, 2011
Publication date	May 21, 2019
Grant date	May 21, 2019

Abstract

A method for measuring fill level and a measuring device for performing the method, wherein, in measuring cycles following one after the other, signal pulses of predetermined frequency sent by means of a transmitting and receiving system with a predetermined repetition frequency into a container, and their signal components reflected back in the container in the direction of the transmitting and receiving system after a travel time dependent on their traveled path, are received as received signal. A fill level is measured taking into consideration a phase relationship between the transmitted and received signals related physically with the fill level to be measured. In each measuring cycle, based on the received signal, an auxiliary signal is derived reflecting amplitude and phase information in the received signal as a function of travel time, based on the auxiliary signal, a travel time of a signal fraction reflected on a surface of the substance is determined as fundamental travel time are determined, based on the travel times of the zero crossings of the auxiliary signals determined in the current and in a plurality of preceding measuring cycles, a phase appearance-frequency distribution is derived as a function of travel time, which gives appearance-frequencies, with which zero crossings were present on the respective travel times in the associated auxiliary signals, a travel time of a maximum of the frequency distribution lying nearest the fundamental travel time is determined as fill level travel time, and the fill level is determined based on the fill level travel time.

First claim

The invention claimed is:

1. A method for measuring fill level of a substance located in a container, in the case of which signal pulses of predetermined frequency are sent in measuring cycles following one after the other, comprising the steps of:
sending the signal pulses of predetermined frequency by means of a transmitting and receiving system with a predetermined repetition frequency into the container, and their signal components reflected back in the container in the direction of the transmitting and receiving system after a travel time dependent on their traveled path, are received as received signal;
based on the received signal, over a predetermined travel time range, an auxiliary signal is derived reflecting amplitude and phase information in the received signal as a function of travel time; based on the auxiliary signal, a travel time of a signal fraction reflected on a surface of the substance is determined as fundamental travel time;
travel times of zero crossings of the auxiliary signal are determined;
based on the travel times of the zero crossings of the auxiliary signals determined in the current and in a plurality of preceding measuring cycles, a phase appearance-frequency distribution is derived as a function of travel time, which gives appearance-frequencies, with which zero crossings were present at the respective travel times in the associated auxiliary signals;
a travel time of a maximum of the frequency distribution lying nearest the fundamental travel time is determined as fill level travel time;
and the fill level is determined based on a propagation velocity of the signal pulse, an installed height of the transmitting and receiving system above the container and the fill level travel time
wherein:
the fundamental travel time is determined in each measuring cycle based on the travel times of the zero crossings of the auxiliary signal derived in the respective measuring cycle; time periods between sequentially following zero crossings of the auxiliary signal, are determined;
a time window of predetermined length is shifted step-wise over the total travel time range; for each position of the time window, an appearance-frequency (#) is determined, with which there occur in the time window time periods, whose length corresponds to half of a period in the auxiliary signal corresponding to the frequency of the signal pulse;
a period appearance-frequency distribution (#(t)) of the appearance-frequencies (#) is determined as a function of travel times associated with the positions of the time window, a maximum of the period appearance-frequency distribution (#(t)) attributable to the reflection of the signal pulses on the surface of the substance is determined;
and the fundamental travel time is determined based on a travel time of the fill level maximum, especially that travel time, in the case of which the fill level maximum assumes its maximum value, or that travel time, in the case of which a rising or falling edge of the fill level maximum exceeds or undershoots a predetermined threshold value; and
wherein:
the travel time range for deriving the period envelope curve (#(t)) is divided into discrete segments, the length of the time window equals a length of a predetermined number of segments, the time window in the case of the stepwise shifting is shifted in each step by one segment;
and there is associated with the individual positions of the time window, in each case, that travel time, over which in the respective position a window center of the time window is located.

2. The method as claimed in claim 1 , wherein:
a cross correlation of the phase appearance-frequency distribution with a reference distribution is formed;
and the fill level travel time is determined based on a travel time of a maximum lying nearest the fundamental travel time in a distribution resulting from the cross correlation.

3. The method as claimed in claim 1 , wherein:
the frequency values of the phase appearance-frequency distribution are filtered by means of an average value filter; and
the fill level travel time is determined based on a travel time of a maximum lying nearest the fundamental travel time in the average value filtered, phase appearance-frequency distribution.

4. The method as claimed in claim 1 , wherein: an average value filtering is performed for travel times of the zero crossings of the auxiliary signals of measuring cycles following one after the other; and the phase appearance-frequency distribution is derived based on the filtered travel times obtained from this average value filtering for the individual measuring cycles.

5. The method as claimed in claim 1 , wherein:
the travel time range is divided into discrete segments of equal segment length;
in each auxiliary signal, those segments are determined, in which such auxiliary signal has zero crossings; and
the phase appearance-frequency distribution as is registered as a histogram, whose histogram classes each correspond to a segment.

6. The method as claimed in claim 1 , wherein:
the phase appearance-frequency distribution in each measuring cycle is determined based on the travel times of the zero crossings of the auxiliary functions derived in such measuring cycle and in a predetermined number of preceding measuring cycles.

7. The method as claimed in claim 6 , wherein: the number of measuring cycles considered in the phase appearance-frequency distribution is fixedly predetermined based on a predetermined fill level change rate to be expected, or the number is continuously matched to a current fill level change rate measured during the method.

8. The method as claimed in claim 1 , wherein:
the registering of the phase appearance-frequency distribution occurs exclusively within a travel time window surrounding the fundamental travel time determined in the respective measuring cycle;
which window extends to both sides of the fundamental travel time (tG) over a plurality of reference period lengths, wherein the reference period length equals half of a reciprocal of a frequency corresponding to the frequency of the signal pulses in the auxiliary signal; and
whose window width is smaller than a width of fill level-maxima the auxiliary functions attributable to reflections on the surface of the substance.

9. The method as claimed in claim 8 , wherein:
a fundamental travel time measured at the beginning of the method is stored as reference travel time;
based on this reference travel time, a position of the travel time window along a travel time axis is established; in each measuring cycle, it is checked whether a difference between the fundamental travel time measured in such measuring cycle and the stored reference travel time exceeds a predetermined threshold value; and
in each measuring cycle, in which the difference exceeds the threshold value, the stored reference travel time is replaced by an updated reference travel time, which equals the fundamental travel time measured in such measuring cycle, and the position of the travel time window is newly established based on the updated reference travel time.

10. The method as claimed in claim 9 , wherein:
the threshold value is dimensioned as a function of the travel time window width and the width of the fill level-maxima of the auxiliary function in such a manner, that the travel time window in each measuring cycle covers a travel time range of a plurality of reference period lengths on both sides of the current fundamental travel time.

11. The method as claimed in claim 1 , wherein:
the signal pulses are microwave pulses sent periodically with the repetition frequency; and the auxiliary signal is a time-expanded version of the received signal

Assignees

• Endress Hauser Gmbh Co Kg
• Endress Hauser Se Co Kg

Inventors

• Vogel Markus
• Malinovskiy Alexey
• Gorenflo Stefan
• Spanke Dietmar

Classifications

• G01F23/284 Primary

  Electromagnetic waves · CPC title

• G01F23/2962 Primary

  Measuring transit time of reflected waves · CPC title