WO2013044950A1 - Mfpw radar level gauging with distance approximation - Google Patents
Mfpw radar level gauging with distance approximation Download PDFInfo
- Publication number
- WO2013044950A1 WO2013044950A1 PCT/EP2011/066875 EP2011066875W WO2013044950A1 WO 2013044950 A1 WO2013044950 A1 WO 2013044950A1 EP 2011066875 W EP2011066875 W EP 2011066875W WO 2013044950 A1 WO2013044950 A1 WO 2013044950A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- frequency
- distance
- modulation
- pulse
- channel
- Prior art date
Links
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S13/00—Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
- G01S13/02—Systems using reflection of radio waves, e.g. primary radar systems; Analogous systems
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S13/00—Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
- G01S13/88—Radar or analogous systems specially adapted for specific applications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01F—MEASURING VOLUME, VOLUME FLOW, MASS FLOW OR LIQUID LEVEL; METERING BY VOLUME
- G01F23/00—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm
- G01F23/22—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water
- G01F23/28—Indicating or measuring liquid level or level of fluent solid material, e.g. indicating in terms of volume or indicating by means of an alarm by measuring physical variables, other than linear dimensions, pressure or weight, dependent on the level to be measured, e.g. by difference of heat transfer of steam or water by measuring the variations of parameters of electromagnetic or acoustic waves applied directly to the liquid or fluent solid material
- G01F23/284—Electromagnetic waves
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S13/00—Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
- G01S13/02—Systems using reflection of radio waves, e.g. primary radar systems; Analogous systems
- G01S13/06—Systems determining position data of a target
- G01S13/08—Systems for measuring distance only
- G01S13/10—Systems for measuring distance only using transmission of interrupted, pulse modulated waves
- G01S13/26—Systems for measuring distance only using transmission of interrupted, pulse modulated waves wherein the transmitted pulses use a frequency- or phase-modulated carrier wave
Definitions
- the present invention relates to a radar level gauge using
- electromagnetic waves to determine a distance to a surface of a product in a tank.
- FMCW frequency modulated continuous wave
- An FMCW measurement comprises transmitting into the tank a signal which is swept over a frequency range in the order of a few GHz.
- the signal can be in the range 25-27 GHz, or 9.5-1 1 GHz.
- the transmitted signal is reflected by the surface of the contents in the tank (or by any other impedance transition) and an echo signal, which has been delayed a certain time, is returned to the gauge.
- the echo signal is mixed with the transmitted signal to generate a mixer signal, having a frequency equal to the frequency change of the transmitted signal that has taken place during the time delay. Due to the linear sweep, this difference frequency, also referred to as an intermediate frequency (IF), is proportional to the distance to the reflecting surface.
- IF intermediate frequency
- the mixer signal is often referred to as an IF signal.
- FMCW systems are relatively power hungry, making them less suitable for applications where power is limited.
- Examples of such applications include field devices powered by a two-wire interface, such as a 4-20 mA loop, and wireless devices powered by an internal power source (e.g. a battery or a solar cell).
- an internal power source e.g. a battery or a solar cell.
- Various methods are available to decrease power consumption.
- the number of different carrier wave frequencies in a measurement cycle is insufficient to provide a continuous IF signal, or even an
- the small set of frequencies is chosen according to a specified frequency scheme, and a phase shift in the received pulse is determined for each frequency.
- the process of determining the distance to the surface involves establishing a change of phase with emitted frequency (see figure 1 ).
- the line A represents an initial distance estimation
- line B represents an updated estimation.
- points x are required to determine the rate of change (slope of line B)
- a larger number e.g. a 5-20 samples
- a few hundred may be required.
- One way to increase accuracy without requiring many samples is to determine a "rough approximation" of the distance to the surface, and to use this estimate as a starting point when determining an accurate distance measure.
- a method for determining a distance to a surface of a product kept in a tank comprising forming a transmit signal as a pulse train of distinct carrier wave pulses having a duration greater than 1 microsecond and shorter than 100 milliseconds, each pulse being frequency modulated around a defined center frequency, transmitting the transmit signal towards the surface, receiving an electromagnetic return signal reflected at the surface, mixing the return signal with the transmit signal in a first channel (l-channel) and mixing the return signal with a 90° phase shifted transmit signal in a second channel (Q-channel), to provide two IF
- step S5 actual phase properties of each distinct pulse received in relation to each corresponding distinct pulse transmitted, based on the primary amplitude values and determining a distance measure based on the actual phase properties, filtering the IF signals to provide a filtered signal corresponding to a second selected harmonic of the modulation frequency, mixing the filtered signals of each channel with the second selected harmonic of the modulation frequency, to provide two secondary amplitude values (I and Q), and providing an approximation of the distance based on a
- a radar level gauging system for determining a distance to a surface of a product kept in a tank, the system comprising a transceiver for transmitting electromagnetic transmit signals formed by a pulse train of distinct carrier wave pulses having a duration greater than 1 microsecond and shorter than 100 milliseconds, each pulse being frequency modulated around a defined center frequency, and receiving electromagnetic return signals reflected at the surface, a set of RF mixers for mixing the return signal with the transmit signal in a first channel (l-channel) and mixing the return signal with a 90° phase shifted transmit signal in a second channel (Q- channel), to provide two IF (intermediate frequency) signals, a first set of filters for filtering the IF signals to provide a filtered signal corresponding to a first selected harmonic of the modulation frequency, a first set of IF mixers for mixing the filtered signals of each channel with the first selected harmonic of the modulation frequency, to provide two primary amplitude values (I
- the level gauging thus includes an approxiamtion of a distance to the surface.
- the approxiamtion is determined by relating an amplitude of a first harmonic of an IF signal with an amplitude of a second harmonic of the IF signal.
- the frequency modulation of the transmit signal introduces a distance dependence.
- Two different harmonics of the modulated signal are used in two separate signal paths (sequential or parallel) to provide two different values representing different distance dependencies. By comparing these two values, e.g. dividing one with the other and forming a quotient between them, a rough approximation of the distance to the surface can be provided.
- each harmonics represents a given distance range.
- the distance may be estimated.
- the distance dependence may be very different, and may be selected to suit the application.
- the actual phase of the IF-signal of a plurality of pulses may be used in the process of providing a more exact distance measure, e.g. as disclosed in US application 12/981 995, herewith incorporated by reference.
- the approximated distance is used as input in the accurate distance determination, e.g. to improve the statistical analysis applied to a plurality of phase properties, thereby enabling a more sensitive and reliable distance measurement.
- the rough approximation can be used as a post processing verification of the accurate measurement. If the rough approximation is significantly different than the accurate distance measure, then a new accurate distance measurement should be obtained.
- Figure 1 is a diagram showing phase versus transmitted frequencies.
- Figure 2 is a schematic block diagram of a radar level gauge mounted on a tank.
- Figure 3 is a more detailed block diagram of the transceiver in figure 1 , according to a first embodiment of the present invention.
- Figure 4 illustrates frequency modulation of a carrier wave.
- Figure 5 is a flow chart of a method according to an embodiment of the present invention.
- Figure 6 shows the first five harmonics for sinusoidal modulation.
- Figure 7 shows Fourier coefficients for even tones for triangular modulation.
- embodiments of the present invention are mainly described with reference to a radar level gauge system having a free propagating antenna for radiating and capturing electromagnetic signals. It should be noted that this by no means limits the scope of the invention, which is equally applicable to other signal propagating devices, including other free propagating antennas such as a rod antenna, a patch antenna, a fixed or movable parabolic antenna or a conical antenna, and wave guides, such as a still pipe, a transmission line or a probe, such as a single-line probe (including a so-called Goubau probe), a twin-line probe or a coaxial probe.
- free propagating antennas such as a rod antenna, a patch antenna, a fixed or movable parabolic antenna or a conical antenna
- wave guides such as a still pipe, a transmission line or a probe, such as a single-line probe (including a so-called Goubau probe), a twin-line probe or a coaxial probe.
- Fig 2 schematically illustrates a radar level gauge system 1 according to an embodiment of the present invention, comprising a measurement electronics unit 2, and a signal propagating device, here a horn antenna 3.
- the radar level gauge system 1 is provided on a tank 5, which is partly filled with a product 6 to be gauged.
- the product 6 is a solid, such as grain or plastic pellets, which is well-known to represent a difficult application requiring a relatively high measurement sensitivity of the radar level gauge system.
- the measurement electronics unit 2 can determine the distance between a reference position and the surface 7 of the product 6, whereby the filling level L can be deduced. It should be noted that, although a tank 5 containing a single product 6 is discussed herein, the distance to any material interface present in the tank 5 can be measured in a similar manner.
- the electronics unit 2 comprises a transceiver 10 for transmitting and receiving electromagnetic signals, which is connected to the antenna 3 via a wave guide 9.
- the unit 2 further comprises a processing circuitry 1 1 , which is connected to the transceiver 10 for control of the transceiver and processing of signals received by the transceiver to determine the filling level of the product 6 in the tank 5.
- the processing circuitry 1 1 is also connected to a memory 12, storing any software required for the operation of the gauge 1 , and also providing RAM used during operation.
- the processing circuitry 1 1 is further connectable to external communication lines 13 for analog and/or digital communication via an interface 14.
- the communication between the communication interface 14 and an external control station can be provided by a two-wire interface, which has a combined function of both transmitting the measurement result to the control station and receiving power for operation of the gauge 1 .
- the current in the lines is regulated in accordance with a measurement result determined by the processing circuitry 1 1 .
- the gauge may communicate wirelessly with the control station using e.g. a Wireless HART protocol, and use a local power supply with batteries or other means of scavenging energy for autonomous operation.
- the processing circuitry 1 1 and the interface 12 may be provided on the same circuit board.
- Fig 3 schematically shows an exemplary transceiver 10 suitable for implementing an embodiment of the present invention.
- a signal generator 20 is arranged to generate carrier wave pulses with a well defined and accurately controlled carrier frequency.
- the accuracy deviation should be less than 1/1000, and preferably less than 1/10000 or better. This may be achieved with a feed back control system, and the signal generator may for example include a phase locked loop, PLL.
- the pulse duration will be assumed to be about 2 ms, but significantly shorter pulses, e.g. in the order of s are also possible. It should be noted that in a tank gauging context, pulses of a duration in the order s or ms, as mentioned here, are much too long to enable pulsed distance measurement with time domain reflectometry, i.e. to receive a reflected pulse and determine its time of flight. The pulses according to the present invention are thus longer than pulses in conventional pulsed radar level gauges, where a typical pulse duration is in the order of ns.
- the average power of the pulses can be in the nW or ⁇ / area.
- the duty cycle i.e. the relationship between the pulses and the intervals there between, should be limited to less than 50%, and is preferably significantly lower, e.g. 5% or even 1 % or less. Compared to conventional FMCW, this means that the pulses may be emitted with a relatively high power, without increasing the average power of the measurement cycle.
- the pulses are typically radar pulses, with a carrier wave frequency in the GHz area.
- the frequency range may be in the order of 10% of the operating frequency, and may be e.g. between 25 and 27 GHz, or between 9,5 and 1 1 GHz.
- the number of frequencies N may preferably be determined based on the conditions prevalent in the tank.
- the duration of the pulses, the duty cycle, and the frequency of the PLL are controlled by the processor 1 1 (see fig 2).
- the PLL 20 is connected to a modulator 21 , arranged to frequency modulate the pulses from the PLL 20.
- the modulation can be of various types, including periodical (such as triangular or sinusoidal) or random (noise like). With a periodic modulation, an integer number of modulation periods is preferably contained within each emitted pulse, and the modulation preferably starts at a locked position (such as start at zero for each pulse).
- a random modulation is preferably pseudo-random.
- the modulation is assumed to be periodic, with a modulating frequency f m .
- the frequency variation of the modulated carrier wave is shown in figure 6.
- the modulation frequency should be chosen with respect to the pulse duration to ensure that a complete number of modulation periods (P m0d ) are included in each pulse.
- the modulating frequency should be in the order of kHz, and may for example be 10 kHz.
- the modulating frequency may be in the order of a few kHz to one MHz.
- the modulation has an amplitude selected to introduce a variation of the carrier wave frequency (modulation width) of 6f, which is significantly smaller than the predetermined frequency range of the measurement.
- the predetermined range of carrier wave frequencies used in the frequency scheme may be in the order of 1 GHz, and the modulation width 6f can then suitably be in the order of MHz.
- a circulator 22 or a power divider such as a Wilkinson Power Divider
- WPD is provided to direct the signal from the signal modulator 21 to the antenna 3 in the tank 5 and to direct a return signal from the antenna 3 to a receiver section of the transceiver 10.
- the receiver section comprises one or several RF mixers, for mixing the return signal with the transmit signal.
- the RF mixing may be homodyne mixing, i.e. the return signal is mixed directly with the transmit signal, but it may also be useful to apply mixing with a delayed transmit signal.
- the receiver section includes two channels, an in-phase channel (I) and a quadrature channel (Q), each comprising a mixer 23a, 23b.
- the first mixer 23a is provided with the transmitted pulses directly from the PLL 20 (l-channel).
- the second mixer 23b is provided with the transmitted pulses from the PLL 20 via a 90 degrees phase shifter 24 (Q- channel) arranged between the modulator 21 and the mixer 23b.
- the output from the mixers 23a, 23b will not be DC level signals, but instead be IF (intermediate frequency) signals including the modulation frequency f m and harmonics thereof.
- the receiver further comprises two sets of band pass filters 25a, 25b and 26a, 26b, respectively, each set being arranged to filter out a desired frequency content.
- the output from each RF mixer 23a, 23b is connected to one filter in each set, so that two different frequency contents (primary and secondary) are filtered out from each channel (I and Q).
- the desired content may be one of the first harmonics of f m .
- the filtered signals are amplified by amplifiers 27.
- Each set of filters is then connected to a set of IF mixers 28a, 28b, and 29a, 29b, respectively. These mixers also receive as input the modulation frequency f m from modulator 21 , via two multipliers 31 and 32.
- the filters 25a, 25b, 26a, 26b and multipliers 31 , 32 are variable, to enable selection of desired frequency content.
- the filters 25a, 25b, 26a, 26b are variable, to enable selection of desired frequency content.
- the filters 25a, 25b, 26a, 26b are variable, to enable selection of desired frequency content.
- the modulator frequency f m the modulator frequency f m , modulating width 6f, and factor N that are varied in order to achieve the desired filtering.
- the practical implementation of the filters may in most cases be digital and may be combined with the mixers.
- the output from the mixers 25a, 25b, 26a, 26b will be DC level signals, representing primary and secondary phase values for each channel. These values are each fed to a sequence of processing elements including a low pass filter 33, an amplifier 34, an integrator 35 and an A/D converter 36.
- the filters 33 and amplifiers 34 improve the signal-to-noise ratio of the radar level gauge system.
- the low pass filters 33 preferably have a
- the integrators 35 are adapted to integrate the signals over the length of the pulse.
- the order of these elements will be governed by the choice of components, i.e. if they are analogue or digital components.
- the digital output is supplied to the processor 1 1 for storage and processing which will be described below.
- an equally useful alternative may be to provide the primary and secondary phase values in a sequential fashion, i.e. having only one filter path for each channel, and alternating the settings of this path.
- figure 3 that would mean that there would be only two sets of filters 25, 26, amplifiers 26, 27, mixers 28, 29, and processing elements 33-36, instead of four.
- the IF signals output by mixers 23a, 23b will have a distance dependence and will be spread over different harmonics. If the transmitted signal has a sinusoidal modulation with modulation width 6f, the received signal after the homodyne mixing can be described by Bessel functions as harmonics of f m as illustrated in figure 6.
- the distance dependence of J1 (X) (for X smaller than 2) has the same feature as the high-pass filtering in conventional FMCW-systems, i.e. to reduce the dynamic range ⁇ 20 dB by having an amplitude distance dependence counteracting the 1/h-dependence. If a fixed 6f is used it will be limited to 8-10 MHz to measure up to 20-25 m without losing too much amplitude by spreading power to too many other harmonics.
- the modulation width is adjustable depending on the used distance interval. Depending on the type of modulation it can either be different for different installations or be adjusted during the measurement.
- sinusoidal modulation is triangular frequency modulation which has different properties, and may be more efficient than sinusoidal modulation.
- the spectral density corresponds to 0-30 m distance.
- the spectral density can be reduced 17 dB without reducing the received signal. This reduction will remain also for long pulses.
- the lower spectral density for the same power may be used to increase the power.
- a rough estimation of the distance may be provided. For example, in figure 6, it is clear that when the amplitude of the first two harmonics are the same (i.e. a quotient of 1 ) then X is slightly greater than 2. From a known value of X, the distance h can be calculated using the relationship above.
- step S1 a pulse of a determined duration, e.g. 2 ms, is generated by the PLL 20 and transmitted as signals ST into the tank by the antenna 3.
- step S2 the transmitted electromagnetic signals ST are reflected at impedance transitions in the tank 5, including the surface 7 of the product 6 contained in the tank 5, and are returned to the transceiver 10 as echo signals SR by the antenna 3.
- the return signal SR is received by the two channels (I and Q) in the receiver side of the transceiver 10.
- step S3 the return signal SR is mixed with the transmit signal in mixers 23a and/or 23b, to form an IF signals.
- step S4-S5 amplitudes of two different harmonics of the IF signal are determined (in the illustrated example the processed output from mixers 28a and 29a, or alternatively from mixers 28b and 29b). Finally, in step S6 these two amplitudes are compared to each other to determine a rough distance approximation.
- one useful relationship is simply the quotient between the two amplitudes. Such a quotient may indicate a specific distance, based on knowledge of the distance dependence of the two harmonics.
- amplitudes for two or more different harmonics in each channel may be determined for two channel, and amplitudfes for the second and fourth harmonics for the second channel. This may enable an even more robust approximation.
- the distance approximation method outlined herein may
- the primary (or secondary) phase values discussed above are recorded in memory 13 for all frequencies in a predetermined frequency scheme.
- Each phase difference value (which is in the range 0-2 ⁇ ) is correlated to an expected phase difference value, calculated based on a previously detected distance.
- the difference between the expected phase and the actual, detected phase corresponds to a distance offset.
- one such offset, resulting from a single frequency is sufficient to provide an updated distance detection.
- the uncertainty in such a detection will normally be too significant to provide satisfactory reliability, and some kind of statistical analysis will normally be required.
- a rough approximation provided by the present invention, for each transmitted pulse, can be very advantageous to make such analysis more robust and reliable. Under certain conditions, this approximation may eliminate the need for an initial distance detection as discussed in
- the approximation discussed herein may be used to verify a more accurate distance determination, e.g. obtained according to US 12/981 995.
Landscapes
- Engineering & Computer Science (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Electromagnetism (AREA)
- Computer Networks & Wireless Communication (AREA)
- Thermal Sciences (AREA)
- Fluid Mechanics (AREA)
- Radar Systems Or Details Thereof (AREA)
Abstract
Description
Claims
Priority Applications (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
BR112014007179A BR112014007179A2 (en) | 2011-09-27 | 2011-09-28 | mfpw radar level measurement with distance approach |
EP11763649.8A EP2748629B1 (en) | 2011-09-27 | 2011-09-28 | Mfpw radar level gauging with distance approximation |
RU2014110278/07A RU2603126C2 (en) | 2011-09-27 | 2011-09-28 | Mfpw radar level gauging with distance approximation |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US13/246,265 US8730093B2 (en) | 2011-09-27 | 2011-09-27 | MFPW radar level gauging with distance approximation |
US13/246,265 | 2011-09-27 |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2013044950A1 true WO2013044950A1 (en) | 2013-04-04 |
Family
ID=44719945
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/EP2011/066875 WO2013044950A1 (en) | 2011-09-27 | 2011-09-28 | Mfpw radar level gauging with distance approximation |
Country Status (6)
Country | Link |
---|---|
US (1) | US8730093B2 (en) |
EP (1) | EP2748629B1 (en) |
CN (2) | CN202501902U (en) |
BR (1) | BR112014007179A2 (en) |
RU (1) | RU2603126C2 (en) |
WO (1) | WO2013044950A1 (en) |
Families Citing this family (19)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US9513153B2 (en) | 2010-12-30 | 2016-12-06 | Rosemount Tank Radar Ab | Radar level gauging using frequency modulated pulsed wave |
US8872694B2 (en) | 2010-12-30 | 2014-10-28 | Rosemount Tank Radar Ab | Radar level gauging using frequency modulated pulsed wave |
US8730093B2 (en) * | 2011-09-27 | 2014-05-20 | Rosemount Tank Radar Ab | MFPW radar level gauging with distance approximation |
US8854253B2 (en) | 2011-09-27 | 2014-10-07 | Rosemount Tank Radar Ab | Radar level gauging with detection of moving surface |
US9121942B2 (en) * | 2012-11-05 | 2015-09-01 | Magnetrol International, Inc. | Guided wave radar delay lock loop circuit |
US9234784B2 (en) * | 2013-10-25 | 2016-01-12 | Rosemount Tank Radar Ab | Frequency modulated radar level gauging |
GB2521136B (en) * | 2013-12-10 | 2021-04-07 | Dynamic Flow Tech Limited | Waste water flow quantifying apparatus, method and computer program |
US9541444B2 (en) * | 2014-04-01 | 2017-01-10 | Rosemount Tank Radar Ab | Self-diagnosing FMCW radar level gauge |
US9709433B2 (en) * | 2014-06-30 | 2017-07-18 | Rosemount Tank Radar Ab | Pulsed radar level gauging with efficient start-up |
RU2601283C2 (en) * | 2014-09-23 | 2016-10-27 | Федеральное государственное бюджетное учреждение науки Институт проблем управления им. В.А. Трапезникова Российской академии наук | Contactless radiowave method of measuring liquid level in reservoir |
US9618617B2 (en) * | 2015-03-20 | 2017-04-11 | Honeywell International Inc. | Level measurement using correlation between a pair of secondary reference signals |
DE102015109463A1 (en) * | 2015-06-15 | 2016-12-15 | Endress + Hauser Gmbh + Co. Kg | Method for checking the functionality of a radar-based level gauge |
US10641866B2 (en) * | 2016-08-05 | 2020-05-05 | Texas Instruments Incorporated | Failure detection in a radar system |
RU2626386C1 (en) * | 2016-10-07 | 2017-07-26 | Федеральное государственное бюджетное учреждение науки Институт проблем управления им. В.А. Трапезникова Российской академии наук | Method of measuring liquid level and loose medium in capacity |
ES2792043T3 (en) * | 2017-12-04 | 2020-11-06 | Grieshaber Vega Kg | Printed circuit board for a radar fill level measuring device with a waveguide coupling |
CN108195443B (en) * | 2017-12-29 | 2020-10-02 | 北京奥特美克科技股份有限公司 | Water level measuring method, system and equipment |
CN108692792B (en) * | 2018-03-27 | 2020-11-10 | 招商局金陵船舶(江苏)有限公司 | Radar type monitoring device for platform liquid level remote measuring system |
EP3657206A1 (en) * | 2018-11-20 | 2020-05-27 | ams AG | Method of detecting a time-of-flight, a time-of-flight converter, an ultrasound flow meter and an optical device |
CN110763302A (en) * | 2019-11-20 | 2020-02-07 | 北京航空航天大学 | FMCW high-precision liquid level measurement method based on iterative frequency estimation |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5406842A (en) * | 1993-10-07 | 1995-04-18 | Motorola, Inc. | Method and apparatus for material level measurement using stepped frequency microwave signals |
JP2004301617A (en) * | 2003-03-31 | 2004-10-28 | Nohken:Kk | Microwave type level meter |
US20080143583A1 (en) * | 2006-12-13 | 2008-06-19 | Roland Welle | Method and Device for Correcting Non-Ideal Intermediate-Frequency Signals in Distance Sensing Device According to the FMCW Principle |
Family Cites Families (38)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3216010A (en) | 1952-11-04 | 1965-11-02 | Conrad W Roeschke | Range indicating system |
US3623097A (en) | 1969-07-17 | 1971-11-23 | Us Army | Modulation correlated fm ranging system |
US3725924A (en) | 1970-07-22 | 1973-04-03 | Us Navy | Intermittent cw system for satellite surveillance |
US4293934A (en) | 1979-06-18 | 1981-10-06 | Shell Oil Company | Circumferential acoustic device |
GB2123237A (en) | 1982-06-28 | 1984-01-25 | Davy Mckee | Surface detector |
NO152108C (en) * | 1983-04-05 | 1985-08-14 | Autronica As | NIVAAMAALER |
US4914441A (en) | 1988-08-29 | 1990-04-03 | Raytheon Company | Method of processing in a pulse doppler radar |
US5130714A (en) | 1991-05-23 | 1992-07-14 | Hughes Aircraft Company | Stretch and chirp waveform format for reduced generating and receiving hardware complexity |
DE4334079C2 (en) | 1993-10-06 | 1997-02-13 | Daimler Benz Aerospace Ag | Highly accurate radar range finder |
US5440310A (en) | 1994-02-14 | 1995-08-08 | Motorola, Inc. | Bandwidth synthesized radar level measurement method and apparatus |
FR2718249B1 (en) * | 1994-04-05 | 1996-04-26 | Thomson Csf | Radar distance measuring method and device. |
RU2115137C1 (en) * | 1994-05-11 | 1998-07-10 | Николай Егорович Армизонов | Range-finding method of location and components of vector of velocity of objects by radio signals of spacecraft of satellite radio navigation systems |
US6137438A (en) * | 1998-07-22 | 2000-10-24 | Thomas E. McEwan | Precision short-range pulse-echo systems with automatic pulse detectors |
DE19925216C1 (en) | 1999-06-01 | 2001-01-04 | Siemens Ag | Process for the interference-free evaluation of radar signals |
EP1069438A1 (en) * | 1999-07-15 | 2001-01-17 | Endress + Hauser Gmbh + Co. | Method and device for highly accurate determination of the level of a product in a container |
DE19961855B4 (en) | 1999-12-22 | 2007-11-29 | Endress + Hauser Gmbh + Co. Kg | Method and device for determining the fill level of a product in a container |
US6362775B1 (en) * | 2000-04-25 | 2002-03-26 | Mcdonnell Douglas Corporation | Precision all-weather target location system |
US6642884B2 (en) | 2000-05-08 | 2003-11-04 | Sigtec Navigation Pty Ltd. | Satellite-based positioning system receiver for weak signal operation |
US6684696B2 (en) * | 2000-08-17 | 2004-02-03 | Vega Grieshaber, Kg | Filling-level measuring device that evaluates echo signals |
US7230980B2 (en) | 2001-09-17 | 2007-06-12 | Time Domain Corporation | Method and apparatus for impulse radio transceiver calibration |
US7053630B2 (en) | 2002-07-08 | 2006-05-30 | Saab Rosemount Tank Radar Ab | Level gauging system |
US6680690B1 (en) | 2003-02-28 | 2004-01-20 | Saab Marine Electronics Ab | Power efficiency circuit |
US20050270228A1 (en) * | 2003-07-03 | 2005-12-08 | Stephens Scott A | Radar system for local positioning |
RU2255352C2 (en) * | 2003-07-07 | 2005-06-27 | Кошуринов Евгений Иванович | Method and system for radar measurement of object speeds and coordinates (modifications) |
CN1282866C (en) * | 2004-12-23 | 2006-11-01 | 太原理工大学 | Digitized radar levelmeter |
DE102005057094B4 (en) | 2005-11-30 | 2013-02-14 | Vega Grieshaber Kg | Level radar with variable transmission power |
CN101322016B (en) * | 2005-12-05 | 2013-04-24 | Vega格里沙贝两合公司 | Filling level radar frequency converter |
DE102006006572A1 (en) | 2006-02-13 | 2007-08-16 | Vega Grieshaber Kg | Method of measuring fill level in a container with a pulse propagation time level sensor using intermediate frequency sampling |
US7482818B2 (en) | 2006-04-17 | 2009-01-27 | Greenwald Technologies, Llc | Systems and methods for detecting the presence and/or absence of a solid liquid or gas |
US7823446B2 (en) | 2006-11-06 | 2010-11-02 | Rosemount Tank Radar Ab | Pulsed radar level gauging with relative phase detection |
DE102007037105A1 (en) | 2007-05-09 | 2008-11-13 | Rohde & Schwarz Gmbh & Co. Kg | Method and device for detecting simultaneous double transmission of AM signals |
DE102007060579B4 (en) * | 2007-12-13 | 2019-04-25 | Endress+Hauser SE+Co. KG | Method for determining and / or assessing the filling state of a container filled with at least one medium |
US8659472B2 (en) | 2008-09-18 | 2014-02-25 | Enraf B.V. | Method and apparatus for highly accurate higher frequency signal generation and related level gauge |
DE102008048582A1 (en) * | 2008-09-23 | 2010-03-25 | Endress + Hauser Gmbh + Co. Kg | Microwave level gauge |
RU2416807C2 (en) * | 2009-01-23 | 2011-04-20 | Общество с ограниченной ответственностью "Конструкторское бюро радиосистем" | Method for radar measurement of velocity and coordinates of objects and system for implementing said method |
US8872694B2 (en) | 2010-12-30 | 2014-10-28 | Rosemount Tank Radar Ab | Radar level gauging using frequency modulated pulsed wave |
US8854253B2 (en) | 2011-09-27 | 2014-10-07 | Rosemount Tank Radar Ab | Radar level gauging with detection of moving surface |
US8730093B2 (en) * | 2011-09-27 | 2014-05-20 | Rosemount Tank Radar Ab | MFPW radar level gauging with distance approximation |
-
2011
- 2011-09-27 US US13/246,265 patent/US8730093B2/en active Active
- 2011-09-28 EP EP11763649.8A patent/EP2748629B1/en active Active
- 2011-09-28 WO PCT/EP2011/066875 patent/WO2013044950A1/en active Application Filing
- 2011-09-28 BR BR112014007179A patent/BR112014007179A2/en not_active Application Discontinuation
- 2011-09-28 RU RU2014110278/07A patent/RU2603126C2/en active
- 2011-11-10 CN CN2011204658303U patent/CN202501902U/en not_active Expired - Fee Related
- 2011-11-10 CN CN201110371876.3A patent/CN103017866B/en active Active
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5406842A (en) * | 1993-10-07 | 1995-04-18 | Motorola, Inc. | Method and apparatus for material level measurement using stepped frequency microwave signals |
JP2004301617A (en) * | 2003-03-31 | 2004-10-28 | Nohken:Kk | Microwave type level meter |
US20080143583A1 (en) * | 2006-12-13 | 2008-06-19 | Roland Welle | Method and Device for Correcting Non-Ideal Intermediate-Frequency Signals in Distance Sensing Device According to the FMCW Principle |
Non-Patent Citations (2)
Title |
---|
MERRILL SKOLNIK: "Introduction to Radar Systems, passage", 1 January 1980, INTRODUCTION TO RADAR SYSTEMS (SECOND EDITION), MCGRAW-HILL, SG, PAGE(S) 88 - 91, ISBN: 978-0-07-057909-5, XP002548186 * |
SAUNDERS W K: "Post-War Developments in Continuous-Wave and Frequency-Modulated Radar", IRE TRANSACTIONS ON AERONAUTICAL AND NAVIGATIONAL ELECTRONICS, IEEE, USA, vol. ANE-2, no. 1, 1 March 1961 (1961-03-01), pages 7 - 19, XP011245965, ISSN: 0096-1639 * |
Also Published As
Publication number | Publication date |
---|---|
EP2748629B1 (en) | 2017-11-08 |
CN103017866B (en) | 2017-03-01 |
RU2603126C2 (en) | 2016-11-20 |
CN202501902U (en) | 2012-10-24 |
US8730093B2 (en) | 2014-05-20 |
US20130076560A1 (en) | 2013-03-28 |
EP2748629A1 (en) | 2014-07-02 |
BR112014007179A2 (en) | 2017-04-04 |
CN103017866A (en) | 2013-04-03 |
RU2014110278A (en) | 2015-11-10 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
EP2748629B1 (en) | Mfpw radar level gauging with distance approximation | |
US8872694B2 (en) | Radar level gauging using frequency modulated pulsed wave | |
US9513153B2 (en) | Radar level gauging using frequency modulated pulsed wave | |
US8854253B2 (en) | Radar level gauging with detection of moving surface | |
US11022475B2 (en) | Fill level radar device having automated frequency adjustment | |
US9612147B2 (en) | Radar level gauge system with multiple receiver branches | |
CN105987739B (en) | Radar level gauge amount | |
KR20160074526A (en) | Frequency modulated radar level gauging | |
US20080129583A1 (en) | Radar level detector | |
US9671488B2 (en) | Radar level gauge with signal division | |
RU2649665C1 (en) | Non-contacting radio wave level gauge |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
121 | Ep: the epo has been informed by wipo that ep was designated in this application |
Ref document number: 11763649 Country of ref document: EP Kind code of ref document: A1 |
|
REEP | Request for entry into the european phase |
Ref document number: 2011763649 Country of ref document: EP |
|
NENP | Non-entry into the national phase |
Ref country code: DE |
|
ENP | Entry into the national phase |
Ref document number: 2014110278 Country of ref document: RU Kind code of ref document: A |
|
REG | Reference to national code |
Ref country code: BR Ref legal event code: B01A Ref document number: 112014007179 Country of ref document: BR |
|
ENP | Entry into the national phase |
Ref document number: 112014007179 Country of ref document: BR Kind code of ref document: A2 Effective date: 20140326 |