# US 2014/0360264 A1 · Method and Measuring Device for Fill Level Measurement

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- Number: US 2014/0360264 A1
- Document ID: US20140360264A1
- Status: Published application
- Kind: A1
- Application number: 14/366,310
- Filed: 2012-11-22
- Published: 2014-12-11
- Earliest claimed: 2011-12-20
- Assignees: Endress + Hauser GmbH + Co. KG
- Applicants: Endress + Hauser GmbH + Co. KG
- Inventors: Markus Vogel; Alexey Malinovskiy; Stefan Gorenflo; Dietmar Spanke
- Web page: https://patentgrep.com/patent/US20140360264A1

## CPC

- G01F 23/2962: Measuring transit time of reflected waves
- G01F 23/284: Electromagnetic waves
- G01F: MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME

## 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.

## Claims

### Claim at position 1

1-16. (canceled)

### Claim 17

A method for measuring fill level of a substance located in a container, in measuring cycles following one after the other, comprising the steps of:
signal pulses of predetermined frequency are sent 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
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.

### Claim 18 (depends on 17)

The method as claimed in claim 17, 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.

### Claim 19 (depends on 17)

The method as claimed in claim 17, 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.

### Claim 20 (depends on 17)

The method as claimed in claim 17, 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.

### Claim 21 (depends on 17)

The method as claimed in claim 17, 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.

### Claim 22 (depends on 17)

The method as claimed in claim 17, 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.

### Claim 23 (depends on 17)

The method as claimed in claim 17, wherein:
the phase appearance-frequency distribution is registered continuously and updated in each measuring cycle, by
multiplying in each measuring cycle the appearance-frequencies of the phase appearance-frequency distribution determined in the preceding measuring cycle with a predetermined decay factor; and
adding the travel times the zero crossings newly entering in the respective measuring cycle to the appearance-frequencies existing at the corresponding travel times, as reduced by the decay factor.

### Claim 24 (depends on 22)

The method as claimed in claim 22, 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.

### Claim 25 (depends on 17)

The method as claimed in claim 17, 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.

### Claim 26 (depends on 25)

The method as claimed in claim 25, 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.

### Claim 28 (depends on 26)

The method as claimed in claim 26, 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.

### Claim 29 (depends on 17)

The method as claimed in claim 17, 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 subceeds a predetermined threshold value.

### Claim 30 (depends on 29)

The method as claimed in claim 29, 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.

### Claim 31 (depends on 17)

The method as claimed in claim 17, 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, or
the signal pulses are ultrasonic pulses sent periodically with the repetition frequency.

### Claim 32 (depends on 17)

A fill-level measuring device for performing a method according to claim 17, comprising:
a transmitting and receiving system for sending the signal pulses and for receiving the received signals,
an input circuit for deriving the auxiliary signals; and
a measuring and evaluation unit,
which determines in each measuring cycle the travel times of the zero crossings of the auxiliary signal derived in the respective measuring cycle; and
which, based on the travel times of the zero crossings of the auxiliary signals of the current and plurality of preceding measuring cycles, determines the phase appearance-frequency distribution in each measuring cycle.

### Claim 33 (depends on 32)

The fill-level measuring device as claimed in claim 32, wherein:
said measuring and evaluation unit comprises:
a rectifier for rectifying the auxiliary signal,
a differentiating stage connected to said rectifier for determining a second derivative of the rectified auxiliary signal with respect to travel time;
a measuring system connected to said differentiating stage for registering peak and whose travel times arising in an output signal of said differentiating stage; and
an intelligent electronic unit, especially a microcontroller, connected after said measuring system.