DEVICES AND METHODS OF SENSING PROPERTIES OF FLUIDS

Abstract

The invention discloses methods for simultaneously measuring various properties of a fluid using a waveguide. The method includes transmitting a plurality of wave modes into the fluid using an ultrasonic shear wave transducer from one end of a waveguide. Further, the wave modes are reflected from the other end of the waveguide. The reflected wave modes are processed simultaneously. The time of flight and the amplitude of the received wave modes are determined. Further, one or more properties of the fluid are measured using determined time of flight and amplitude of the received wave modes. The disclosed method is used to accurately measure the properties of fluid such as level, density, viscosity or flow rate in a short period of time.

Claims

1. A method of measuring various properties of a fluid using a waveguide having a first end and a second end and a body of substantially uniform cross section therebetween, at least one transducer affixed to the first end of the waveguide configured to send acoustic waves and to receive reflected acoustic signals, comprising: a. transmitting a plurality of wave modes into the fluid using an ultrasonic shear wave transducer from the first end of a waveguide; b. receiving the reflected plurality of wave modes from the second end of the waveguide, wherein the reflections contain information characteristic of the properties of the fluid; c. processing simultaneously the plurality of received wave modes; d. determining time of flight and amplitude ratio of the received wave modes; and e. measuring one or more properties of the fluid using determined time of flight and amplitude of the received wave modes.

2. The method as claimed in claim 1, wherein the plurality of wave modes are selected from longitudinal (L(m,n)), torsional (T(m,n), flexural (F(m,n)).

3. The method as claimed in claim 1, wherein the transmitting is done at an angle of 45-90° inclination to an axis of the waveguide.

4. The method as claimed in claim 1, wherein the one or more properties measured include viscosity, density, flow rate, level or temperature of the fluid.

5. The method as claimed in claim 1, wherein the properties of the fluid are measured using at least two wave modes.

6. The method as claimed in claim 1, comprising measuring a first property of the fluid, measuring a second property of the fluid and applying a correction to the first property using the second property measurement.

7. The method as claimed in claim 6, wherein the first property is fluid level and the second property is density, viscosity or temperature of the fluid.

8. The method as claimed in claim 7, wherein the fluid level is measured to an accuracy of 2.5% or better in the range 10-100 mm.

9. The method as claimed in claim 1, wherein the second end is provided with an axisymmetric notch, a non-axisymmetric notch, a bend, a polygonal section, or an elliptical section.

10. The method as claimed in claim 4, wherein the method comprises measuring the density or viscosity using flexural wave mode, torsional wave mode or both.

11. The method of claim 9, wherein the second end comprises an elliptical section and the property measured is density.

12. The method of claim 9, wherein the second end comprises a cylindrical or a flat section and the property measured is fluid level.

13. The method of claim 9, wherein the second end comprises a cylindrical section and the property measured is flow rate of the fluid.

14. The method as claimed in claim 1, wherein the fluid properties are measured using at least two different frequencies.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0014] The invention has other advantages and features which will be more readily apparent from the following detailed description of the invention and the appended claims, when taken in conjunction with the accompanying drawings, in which:

[0015] FIG. 1A illustrates a system for measuring the properties of fluid.

[0016] FIG. 1B illustrates a configuration of shear transducer with respect to the waveguide.

[0017] FIG. 1C illustrates a waveguide with an excitation transducer and a reception transducer.

[0018] FIG. 1D shows the changes in the cross-section of second end of the waveguide.

[0019] FIG. 2 illustrates a method for measuring the properties of fluid.

[0020] FIG. 3 shows the schematic of the experimental setup for fluid property measurement using a waveguide sensor.

[0021] FIG. 4A, and 4B show reflected A-scan signals in L(0,1), T(0,1) and F(1,1) modes at different fluid levels.

[0022] FIG. 5A shows the change in time of flight (δTOF) of the L(0,1), T(0,1) and F(1,1) wave modes at different fluid levels.

[0023] FIG. 5B shows the change in peak amplitude of the L(0,1), T(0,1) and F(1,1) wave modes at different fluid levels.

[0024] FIG. 5C shows validation of liquid level measurement in the 10-100 mm range, illustrating error <2.5%.

[0025] FIG. 6A shows the reflected L(0,1), T(0,1) and F(1,1) modes in the A-scan signals observed at different fluid densities.

[0026] FIG. 6B shows comparison between standard and measured values of fluid densities using shift in TOF.

[0027] FIG. 7 shows viscosity measurements using ultrasonic method compared to Cannon standard values at different temperatures.

[0028] FIG. 8A shows experimental setup for intrusive flow measurement.

[0029] FIG. 8B shows L(0,1), T(0,1) and F(1,1) wave modes in A scan for intrusive flow measurement.

[0030] FIG. 8C shows variation in TOF with flow rate for L, T and F modes.

[0031] FIG. 8D shows change in amplitude with flow rate for L, T and F modes.

[0032] FIG. 8E shows comparison between standard rotameter measurements and ultrasonic measurements using waveguide for different flow rates.

DETAILED DESCRIPTION

[0033] While the invention has been disclosed with reference to certain embodiments, it will be understood by those skilled in the art that various changes may be made and equivalents may be substituted without departing from the scope of the invention. In addition, many modifications may be made to adapt to a particular situation or material to the teachings of the invention without departing from its scope.

[0034] Throughout the specification and claims, the following terms take the meanings explicitly associated herein unless the context clearly dictates otherwise. The meaning of “a”, “an”, and “the” include plural references. The meaning of “in” includes “in” and “on.” Referring to the drawings, like numbers indicate like parts throughout the views. Additionally, a reference to the singular includes a reference to the plural unless otherwise stated or inconsistent with the disclosure herein.

[0035] The invention in its various embodiments discloses a system and a method for simultaneously measuring various properties of a fluid using a waveguide. The disclosed method is used to measure the properties of a fluid accurately in a short period of time.

[0036] In various embodiments, provided herein are systems and methods for simultaneously measuring various properties of a fluid. The system 100 as shown in FIG. 1A includes a computing device 101, an analog to digital converter 103, an ultrasonic pulser-receiver 105 and a waveguide sensor device 110. The computing device 101 is configured for data acquisition, processing and calculation of properties of fluid. The analog to digital converter 103 is configured to convert the analog signal to digital signal. The ultrasonic pulser-receiver 105 is configured to generate electric pulses. The pulses generated by pulser-receiver 105 are sent to the device 110. The device 110 includes a first end 102, a body 106 and a second end 104. The body 106 has substantially uniform cross section. The cross section in some embodiments may be circular, square, polygonal or other section. The device 110 includes at least one transducer 107 affixed to the first end 102 of the waveguide. The transducer 107 is configured to convert the electric pulses into acoustic pulses. The transducer 107 is configured to send acoustic waves and to receive reflected acoustic signals.

[0037] In one embodiment, the measurement device 110 may have a shear wave transducer 107 oriented at an angle θ to the axis of the waveguide, as shown in FIG. 1B. In various embodiments, the angle θ may vary between 45-90 degrees with reference to the axis of the waveguide. In various embodiments, the transducer is configured to produce waveforms 103a corresponding to longitudinal L(0,1), 103b corresponding to torsional T(0,1), or flexural F(1,1) modes of vibration simultaneously.

[0038] In one embodiment, device 120 includes one excitation transducer 107-1 and one reception transducer 107-2 as shown in FIG. 1C. In some embodiments, the device 110 includes more than one transducer for transmitting or receiving the signals in more than one frequency zone or wave mode. The zones may include low attenuation, increasing attenuation and high attenuation zones. The second end 104 of the device 110 in some embodiments is provided with a change in cross section. In various embodiments, the change in cross-section may include a circular section 104a, a flat or polygonal section 104b, an elliptical section 104c, a bend 104d, axisymmetric notch 104e, or a non-axisymmetric notch 104f, as shown in FIG.1D. In some embodiments a waveguide with circular cross section and with unchanged cross section at the second end may be used. In some embodiments, the waveguide may have a circular cross section with non-circular second end.

[0039] In various embodiments, the method 200 for simultaneously measuring various properties of a fluid, as shown in FIG. 2 includes the steps of transmitting a plurality of wave modes into the fluid using an ultrasonic shear wave transducer from the first end of a waveguide in step 201. In some embodiments, the plurality of wave modes are selected from longitudinal (L(m,n)), torsional (T(m,n), or flexural (F(m,n)) modes. In step 202, the reflected plurality of wave modes are received from the second end of the waveguide. The reflections contain information characteristic of the properties of the fluid. The plurality of received wave modes are processed simultaneously in step 203. In step 204, time of flight and amplitude ratio of the received wave modes are determined. In step 205, one or more properties of the fluid are measured using determined time of flight and amplitude of the received wave modes. In various embodiments, the properties of the fluid are measured simultaneously using at least two wave modes. In some embodiments, the measured one or more properties of the fluid includes viscosity, density, flow rate, level or temperature of the fluid.

[0040] In some embodiments, the method 200 may involve measuring a first property of a fluid such as level, flow etc. and a second property such as temperature, density etc. The method may further involve applying a correction to the first property using the second property. In one embodiment, the simultaneous measurements performed using the method 200 may be fluid level and temperature, and the method may involve correcting the fluid level measurement using density, viscosity or temperature of the fluid. Temperature may be measured by a temperature dependent parameter such as density or viscosity. In one embodiment, the measurement error is less than or equal to 2.5% when measuring change in level between 10-100 mm.

[0041] In some embodiments, the method 200 in step 201 includes transmitting the wave modes at an angle θ of 45-90° inclination to an axis of the waveguide. In another embodiment, the transmitting is done at an angle of 90° and the property measured is a level of fluid.

[0042] In some embodiments, the density and viscosity are measured using flexural wave and torsional wave modes. In one embodiment, the flow rate is measured using longitudinal wave mode and the fluid level is measured using flexural wave mode. In various embodiments the temperature of a fluid may be measured using density or viscosity as primary measurement.

[0043] In some embodiments the method 200 may be used to measure flow rate. The waveguide may be employed for flow measurement using the same experimental setup as shown in FIG. 1A. In some embodiments a circular waveguide with circular end may be used and the second end of the waveguide may be placed in the flowing fluid. The tranducer orientation may be 45° to the axis of the waveguide to generate all three L, T and F wave modes. The method may further involve detecting drop in amplitude of the reflected signals, in all three wave modes shift in TOF in F(1,1) with increasing flow rate. The method may detect flow rate with error of 2% or less.

[0044] The methods disclosed here may be used to measure the physical properties of fluids. The disclosed methods may also be used to determine gradients in the properties of the fluid. The distributed physical properties of fluid may also be determined using the methods. Further, the methods disclosed here provide redundancy to improve accuracy in measurements of the fluid level/rheology. The methods have wide applications for example, inside critical enclosures of processing industries where access to other types of sensors is difficult.

EXAMPLES

Example 1

Method for Measuring Fluid Level

[0045] The experiment was conducted for the determination of fluid level in (a) water and (b) castor oil using thin wire like waveguide sensor. The cross section was uniformly cylindrical without a change in cross section at the end. The schematic of the experimental setup is shown in FIG. 3. Initially, the A-scan signal was obtained for air medium or zero water level (0-cm) as shown in FIG. 4A. Subsequently, the fluid (water) was filled gently in the cylindrical container at increments of 10 mm. The A-scan signals were acquired at each 10 mm interval while filling 90 mm depth of water in the test container are shown in FIG. 4B.

[0046] The sensor was placed inside a beaker and corresponding level scale were used for verification of level measurement. The change in δTOF's and amplitude for the L(0,1), T(0,1) and F(1,1) wave modes at different fluid levels are shown in FIG. 5A and FIG. 5B respectively. As shown in FIG. 5A, due to the dispersive nature of the F(1,1) mode, the δTOF's values are relatively higher in flexural wave mode as compared to the torsional and longitudinal wave modes. The time of flight indicates the fluid level. As shown in FIG. 5A, the time of flight is proportional to the fluid level. As shown in FIG. 5B, the amplitude ratio of flexural wave mode decreases with increase in fluid level. There is no substantial drop in the amplitude ratio of torsional and longitudinal wave mode, when the fluid to be measured is water whereas there is significant drop in the amplitude ratio of torsional and longitudinal wave mode, when the fluid to be measured is oil.

[0047] Multiple trials were conducted to validate the repeatability of this technique. The level Measurement experiments were repeated for non-viscous fluid and the obtained shift in peak frequency and δTOF at different fluid levels of F(1,1) are shown in FIG. 5C. The data of FIG. 5C was found to be consistent and repeatable with an error percentage less than 2.5%.

[0048] It was observed that the flexural wave mode F(1,1) was much more sensitive to the surrounding fluid as compared to the longitudinal L(0,1) and torsional T(0,1) wave modes on viscous and non-viscous fluids. L(0,1) is much more sensitive in water (non-viscous) level measurement compared to T(0,1), while T(0,1) is much more sensitive in oil (viscous) level measurement compared to L(0,1).

Example 2

Measurement of Density

[0049] For measuring density, the experimental setup as shown in FIG. 3 was used to transmit/ receive the signal, and temperature was recorded with a thermocouple. The obtained A-scan signals are shown in FIG.6A. This experiment was chosen to validate the inverse model for density prediction. An circular waveguide with non-circular elliptical end was used. Fluid samples with density from 800 kg/m.sup.3 (kerosene) to 1200 kg/m.sup.3 were used. Above 1000 kg/m.sup.3, the density variation was achieved by adding salt to water. The centre frequency of the tone burst signal was selected to be 500 kHz. The effect of density was measured by tracking the change in TOF of T(0,1) (i.e TOF changes with density changes) and temperature effects were tracked by monitoring the change in TOF of L(0,1) signal. The waveguide measured density values were compared with the standard values as shown in FIG. 6B. Based on the results the waveguide measurement are closely in agreement with the standard value

Example 3

Measurement of Viscosity

[0050] For measuring viscosity, the same equipment as in FIG. 3 was used, with thermocouple for temperature measurement. Experiments were carried out using F(1,1) wave mode on Cannon viscosity standards from room temperature to 48° C. The dynamic viscosity was measured using a uniformly cylindrical waveguide and compared with the standard values. The effect of viscosity was measured by tracking the change in amplitude and also calculating the reflection coefficient of the reflected L(0,1) wave mode. Also the effect of temperature was monitored by tracking the change in TOF of the other wavemode, as shown in FIG. 7. Based on the results it was observed that the waveguide measurement are closely in agreement with the standard values.

Example 4

Intrusive Flow Measurement

[0051] The waveguide was employed for flow measurement using the same experimental setup as shown in FIG. 8A. A circular waveguide with circular end was selected for this experiment and the waveguide was placed inside the pipeline. The tranducer was oriented at 45° to the axis of the waveguide to generate all three wave modes. The centre frequency of the tone burst signal was 500 kHz. The flow was gradually varied in the range 0-2 LPM and the flow was measured using a rotameter. The obtained A-scan signals are shown in FIG. 8B. Significant drop in amplitude of the reflected signals in all three wave modes and shift in TOF is observed in F(1,1) wave mode compared to L(0,1) and T(0,1), with increasing flow rate, as illustrated in FIG. 8C and 8D. The comparison of rotameter vs. waveguide measurement shows that the waveguide measurements are closely in agreement with the standard values.