ENLARGED PIPE SECTION FOR MICROWAVE-BASED FLOW MEASUREMENTS

Abstract

The present invention relates to a pipe section for flow measurements including measuring antennas configured to measure predetermined characteristics of fluid inside the pipe section. The pipe section includes an input end and an output end having a predetermined dimension, the pipe section comprising a section having a first cross section in a first direction extending beyond the input and output dimension by a predetermined amount and a cross section in the second direction being perpendicular to the first direction having a dimension B being less than the dimension A in the first direction.

Claims

1. A pipe section for flow measurements comprising: at least one measuring microwave antenna configured to measure predetermined characteristics of fluid inside the pipe section; wherein the pipe section comprises an input end and an output end having a cross section with a predetermined dimension and a section constituting a microwave resonator and having a cross section in a first direction having a dimension A extending beyond the input and output dimension by a predetermined amount and a second cross section in a second direction having an angle relative to the first direction and having a second dimension B being less than the dimension A, wherein the first and second directions are chosen so that B<A<2B, obtaining resonance modes reflected by opposing section surfaces each providing a different standing wave; and wherein the at least one antenna is mounted in the surfaces and configured to measure at least one resonance frequency indicating the characteristics of the fluid.

2. The pipe section according to claim 1, wherein the first dimension A is chosen to correspond to half the wavelength of the first resonance mode of the microwave signal.

3. The pipe section according to claim 1, wherein the pipe section constitutes an inverted venturi.

4. The pipe section according to claim 1, wherein the pipe section in at least one of the directions is constituted by two opposing curved pipe walls.

5. The pipe section according to claim 2, wherein the pipe section in the at least one of the directions is constituted by two opposing plane pipe walls.

6. The pipe section according to claim 3, wherein at least one of the antennas is mounted in the plane walls.

7. The pipe section according to claim 1, wherein the antennas are microwave measuring antennas configured to measure resonance and/or transmission characteristics of microwave signals in the pipe section.

8. The pipe section according to claim 1, wherein the cross section in the second direction has a dimension being between the cross section of the input and output and the dimension in the first direction.

9. A system for measuring characteristics of a fluid flow comprising a pipe section according to claim 1, wherein the at least one measuring antenna comprises a least one resonance measuring antenna configured to measure at least one electromagnetic resonance in the pipe section.

10. The system according to claim 9, wherein the at least one measuring antenna comprises at least one transmitter and one receiver, the system configured to measure the transmission time between the transmitter and receiver.

11. The pipe section according to claim 1, wherein the angle is 90 degrees.

Description

[0008] The invention will be discussed more in detail below with reference to the accompanying drawings, illustrating the invention by way of examples.

[0009] FIG. 1 illustrates a corrupt resonance peak measured in an inverted venturi according to the known art.

[0010] FIG. 2 Illustrates a preferred embodiment of the present invention with two opposite flat surfaces resulting in a clean resonance.

[0011] FIG. 3a-3c illustrates different alternative cross sections according to the invention.

[0012] FIG. 4 Illustrates the frequency response of the design in FIGS. 2 and 3a with a flat top and bottom.

[0013] As stated above, the inverted venturi solution is well known, e.g. from above-mentioned EP1451562B1 and U.S. Pat. No. 10,175,075, but the basic cylindrical geometry has the problem that the lowest waveguide mode to form resonances (TE11) is not circularly symmetrical, but does not have a predefined orientation. This means that two orthogonal modes can exist. They are independent, but they have the same resonant frequency. An inhomogeneity in the flow may shift the independent resonance frequencies and cause them to interfere with each other resulting in a corrupt combined resonance peak as illustrated in FIG. 1 as a split resonance peak 11. Even a simulation in HFSS (High Frequency Structure Simulator, a simulation program based on the finite element method) with an empty sensor shows that the peak is split in the middle.

[0014] Referring to FIG. 2 the present invention is related to a modification to the pipe section 1 constituting a modified inverted venturi with a larger cross section than the cross section at the input and output ends 2b of the pipe section 1, the term “cross section” in the present application being used indicating the dimensions perpendicular to the pipe and flow direction. The pipe section 1 is positioned between two pipe 2 sections conducting a fluid flow with a transition zone 2a having a predetermined length. Instead of a circular cross section, as is known in the prior art, the cross section of the illustrated embodiment is a combination of a circular and linear cross section parts so that there are two opposite flat surfaces 3, and two opposite arc-shaped surfaces 4, the latter having a larger separation than the former. This has several advantages, e.g.: [0015] The orthogonal resonances are separated in frequency so that each peak is clean. [0016] Three or more antennas 5 for measuring both transmission and resonance can be located on the flat surface 3, and exactly the same configuration can be used for several pipe diameters. Any desired configuration can be used, e.g. triangular, axial or transverse linear. [0017] A surface sensitive cavity resonator sensor, e.g. as described in EP2104837, can easily be integrated on one of the flat surfaces. [0018] The design has no theoretical flow velocity limitation. [0019] There is no dielectric pipe, sleeve, insert or filling in the cavity.

[0020] The frequency response resulting from the design shown in FIG. 2 shows two clearly separated clean peaks 12, 13 as is shown in FIG. 4, which also shows the split peak response 11 of the cylindrical design from FIG. 1 with broken lines for reference.

[0021] More in detail the frequency response of the design in FIG. 2, with a flat top 3 and bottom, has a clean first resonance peak with enough distance to the next peak to avoid confusion between peaks under highly dynamic flow conditions. This distance can be changed by changing the aspect ratios of the design. The two resonance peaks may be used for measuring the characteristics of the flow as disclosed in EP3286561B1.

[0022] As illustrated in FIG. 3a-3c, other shapes of the pipe section can be contemplated, e.g. having an elliptic (FIG. 3c) or rectangular cross section (FIG. 3b) or alternatively where the surface adapted to receive the antennas 5 has a standardized curvature suitable for the selected antennas while the curvature in the perpendicular direction is different. The main aspect being that the two peaks are clearly separated and the orientation of the resonating field relative to the cross section is defined.

[0023] The area of the cross section in the pipe section 1 according to the invention is preferably larger than the area of the cross section of the rest of the pipe 2 so as to be non-intrusive in the fluid flow, but a solution where the area is unchanged along the pipe and pipe section may also be contemplated for example if no pressure variations are wanted in the flow.

[0024] As an illustration, referring to FIG. 3b, a pipe section is illustrated defining a rectangular wave guide with dimensions A×B where A>B, A being the distance between the first two opposing surfaces 4 and B being the distance between the second two opposing surfaces 3. The cut-off frequency for the first mode where A corresponds to half the wavelength and the next will be when A corresponds to a full wavelength. The orthogonal mode has a cutoff frequency where B corresponds to half a wavelength. If A=2B the two next modes will have the same cutoff frequency, being twice the first mode. Therefore, waveguides often have this proportion and an octave is obtained where only one mode can exist. According to the present invention an intermediate solution is preferred where B<A<2B, obtaining resonance modes reflected by the opposing surfaces each providing a different standing wave. A longer distance, A>2B, will result in a long resonator where the resonances are too close. Thus, the dimensions should be chosen so as to obtain a reasonable separation between the resonance modes.

[0025] The multiphase flow measurement (MPFM) concept is thus based on measuring the water cut (WC) and the salinity under high-loss conditions in the liquid locally at the wall using probes or antennas 5 instead of trying to measure the effective permittivity of the whole flow, which is heavily affected by varying flow regimes. But if desired, additional receiver antenna(s) can be mounted on the opposite wall. However, tests with the surface sensitive salinity sensor indicate that the enlargement of the pipe will make the liquid flow close to the wall facilitating the measurement of the salinity and the local WC.

[0026] Two additional antennas 6 positioned in the flow direction may be used for cross correlation, e.g. as shown in FIG. 2. If they are located on opposite walls, the measured velocity represents the average velocity across the flow. If they are located on the same wall the measured velocity represents the velocity closer to the wall, but the received signal is stronger.

[0027] The position of the main antennas in FIG. 2 may be chosen as discussed in EP3308160B1 so that the transmission measuring antenna is positioned in a minimum of at least one of the higher resonance modes in the venturi to reduce the interference from the resonances while performing transmission measurements under moderately lossy conditions.

[0028] As is understood from the discussion above the present invention solves a fundamental problem related to exciting the lowest resonance in a basically cylindrical cavity without using any cone, fin, or other insert, while providing some extra advantages related to using the same geometrical antenna configuration on several pipe sizes, and allowing the combined use for measurement of resonance and differential transmission. The main advantage of being able to use the same antenna configuration on several pipe sizes is that the same models for extracting the watercut and the salinity can be used without extra pipe size related modifications. This reduces the need for testing and calibration, which is expensive and time consuming.

[0029] The invention requires no dielectric material (pipe, sleeve or filling) in the cavity which could absorb water, be affected by the fluids over time and have temperature dependent properties that needs to be compensated for. Neither does the invention have any velocity limit.

[0030] To summarize, the present invention relates to a pipe section for flow measurements including measuring antennas configured to measure predetermined characteristics of fluid inside the pipe section. The pipe section includes an input end and an output end having a predetermined dimension. The pipe section comprising a section having a first cross section in a first direction extending beyond the input and output dimension by a predetermined amount and a cross section in the second direction preferably being perpendicular to the first direction having a dimension B being less than the dimension A in the first direction.

[0031] While in the present invention two perpendicular directions in the resonator is discussed, providing two different resonance conditions, other solutions may be contemplated, where the shape of the cross section may be chosen so as to obtain more than two resonance frequencies or to adapt to other sypes of measurements and conditions.

[0032] According to one embodiment the pipe section is constituted in the first direction of two opposing curved pipe walls and may in the second direction be constituted by two opposing plane pipe walls. In the latter case at least one of said antennas are mounted in said plane walls.

[0033] The antennas are preferably microwave measuring antennas configured to measure resonance and/or transmission characteristics of microwave signals in said pipe section.

[0034] The cross section in the second direction may have a dimension being between the cross section of the input and output and the dimension in the first direction. The pipe section thus being larger than the input and output pipes in both directions, but where the dimensions in the first and second direction is not the same.

[0035] Preferably the first and second dimensions are chosen so as to provide an area of the cross section being at least the same as the area of the pipe cross section and preferably larger.