This invention relates to a technique for measuring the depth of water, e.g., in a river or stream; and more particularly, to a technique for measuring the depth of water using a pressure sensor.
Water pressure measurements performed with a pressure sensor in flowing water are affected by water velocity and this needs to be corrected to determine the correct water depth. Known techniques for measuring the depth of water, e.g., in a river or stream using a pressure sensor do not make a correction for the water velocity. In view of this, there is a need in the art for better way for measuring the depth of water, e.g., in a river or stream, especially using a pressure sensor.
In summary, the correction of water pressure measurements performed by an instrument equipped with an acoustic Doppler velocity meter and pressure sensor is directly related to the water velocity. There are two parameters, dynamic pressure and drag coefficient that need to be determined to properly correct the measured pressure by the instrument.
The present invention builds on technology previously developed by the assignee of the instant patent application, e.g., which is sold as a product in the marketplace known as the FlowTracker® Handheld ADV®. By way of example, the reader is referred to the FlowTracker® Technical Manual (March 2009), which is known in the art and sets forth technical details for firmware version 3.7 and software version 2.30, which is incorporated by reference in its entirety. The present invention builds upon this technology, e.g., by introducing and incorporating new technology for taking a water depth measurement by compensating for Venturi effects on pressure sensors in moving water, e.g., consistent with that disclosed herein. The present invention is implemented using this new technology in a product being sold by the assignee of the present invention, e.g., known as the FlowTracker2™.
According to some embodiments, the present invention may include, or take the form of, apparatus for taking a water depth measurement using a probe, featuring a signal processor configured to
The present invention may include one or more of the following features:
The signal processor may be configured to determine the velocity-dependent offset by compensating a dynamic pressure component based upon a pressure correction coefficient to account for the Bernoulli Effect of the water depth measurement, e.g., where the dynamic pressure component may be defined by the relationship:
pv
2/2,
where p represents the fluid density and v represents the fluid speed of the moving water.
The apparatus may include, or take the form of, the probe having the pressure sensor contained therein.
The pressure sensor may include a non-vented pressure sensor.
According to some embodiments, the apparatus may include, or take the form of, an acoustic Doppler velocimeter (ADV) with a built-in probe or pressure sensor for sensing pressure for taking the water depth measurement, e.g., which may take the form of the assignee's FlowTracker2, e.g., consistent with that set forth herein.
According to some embodiments, the present invention may include a method for taking a water depth measurement using a probe, featuring:
According to some embodiments of the present invention, the present invention may also take the form of a computer-readable storage medium having computer-executable components for performing the steps of the aforementioned method. The computer-readable storage medium may also include one or more of the features set forth above.
The drawing, which are not necessarily drawn to scale, includes
To reduce clutter in the drawing, each Figure in the drawing does not necessarily include every reference label for every element shown therein.
By way of example,
The signal processor 10a may be configured to provide the corresponding signaling containing information about the corrected water depth measurement of the flowing water, e.g., for further processing.
By way of example, and as one skilled in the art would appreciate, the functionality of the signal processor 10a may be implemented using hardware, software, firmware, or a combination thereof. In a typical software implementation, the signal processor 10a would include one or more microprocessor-based architectures having, e.g., at least one signal processor or microprocessor like element 10a. One skilled in the art would be able to program with suitable program code such a microcontroller-based, or microprocessor-based, implementation to perform the signal processing functionality disclosed herein without undue experimentation, e.g., using one or more of the methods or algorithms disclosed herein.
For example, the signal processor 10a may be configured, e.g., by one skilled in the art without undue experimentation, to receive the signaling containing information about the water depth measurement determined from the pressure sensed by the pressure sensor contained in the probe immersed in the flowing water, and also containing information about the velocity-dependent offset that is determined and depends on the velocity of the flowing water, consistent with that disclosed herein. By way of example, this signaling may be stored in a memory module device, circuit or component, e.g., like element 10b, as described below.
By way of further example, the signal processor 10a may be configured, e.g., by one skilled in the art without undue experimentation, to determine the corresponding signaling containing information about the corrected water depth measurement of the flowing water by correcting the water depth measurement by the velocity-dependent offset in order to compensate for the Venturi effects on the pressure sensor in the moving water, based upon the signaling received, and consistent with that disclosed herein.
The scope of the invention is not intended to be limited to any particular implementation using technology either now known or later developed in the future. The scope of the invention is intended to include implementing the functionality of the signal processor(s) 10a as stand-alone processor, signal processor, or signal processor module, as well as separate processor or processor modules, as well as some combination thereof. According to some embodiments, the signal processor 10a may be configured as part of the pressure sensor P, or as part of another processor or processing module that forms part of the apparatus 10. The scope of the invention is not intended to be limited to what circuit, component or other element that the signal processor 10a may form part of.
By way of example, the signal processor, or signal processing module 10a may also include, e.g., other signal processor circuits or components generally indicated 10b, including random access memory or memory module (RAM) and/or read only memory (ROM), input/output devices and control, and data and address buses connecting the same, and/or at least one input processor and at least one output processor, e.g., which would be appreciate by one skilled in the art.
By way of further example, the signal processor 10a and other signal processor circuits or components generally indicated 10b may include, or take the form of, some combination of a signal processor and at least one memory including a computer program code, where the signal processor and at least one memory are configured to cause the system to implement the functionality of the present invention, e.g., to respond to signaling received and to determine the corresponding signaling, based upon the signaling received.
By way of example, the basic methodology may include the following:
i) Correction of Dynamic Pressure
As one skilled in the art would appreciate, when measuring water pressure at a specific point within a water column, the water pressure or total pressure is the sum of the Hydrostatic Pressure (P) and Dynamic Pressure (Pd) given in Equation 3:1.
P
0
=P+P
d (Equation 3:1—Total Pressure)
When stagnant (water velocity is zero) water is present, the Dynamic Pressure (Pd) component can be excluded from Total Pressure (Po) and thus the Hydrostatic Pressure (P) is equal to the Total Pressure (Po). The Total Pressure in Equation 3:1 for Stagnant Water can be reworked in Equation 3:2,
P
0
=P (Equation 3:2—Total Pressure—Stagnant Water)
Consistent with that shown in
P=ρgh (Equation 3:3—Hydrostatic Pressure),
Where: ρ—water\liquid Density,
As one skilled in the art would also appreciate, when water is flowing the Dynamic Pressure is directly related to the water velocity and needs to be accounted for in calculating the Total Pressure (Po). Dynamic Pressure (Pd) is defined by the Water Density (ρ) and Water Velocity (V) given in Equation 3:4, as follows:
P
d=0.5ρV2 (Equation 3:4—Dynamic Pressure).
ii) Drag/Correction Coefficient
As one skilled in the art would appreciate, the effect of drag force on pressure measurements can be corrected by applying a drag\correction coefficient to the calculated Dynamic Pressure. The Total Pressure (Po) in Equation 3.1 may be reworked to devise a Corrected Pressure (Pc) that incorporates drag\correction coefficient, e.g., using Equation 3.5 that yields,
P
c
=P
m+0.5ρ(aV)2 (Equation 3:5—Corrected Pressure),
Where: Pm—pressure measured,
By way of example, the drag\correction coefficient can be computed from experimental data for particular head\instrument\probe. If one arranges the data pressure and velocity data, e.g., Equation 3.6 yields,
P
c
=P
m
+cV
2 (Equation 3:6—Corrected Pressure—Coefficient “c”),
Where: Pc—corrected pressure,
For the purpose of that calibration, one can devise a setup where the depth of the pressure sensor is kept constant and allow for varying the speed of the water/liquid around the sensor at the same time. The water/liquid temperature can also be controlled along with controlling the salinity, thus controlling the density.
Taking multiple measurements with varying the water/liquid speed in the setup described above and using linear regression, one can determine the best “c” fit. Solving the coefficient “c”, e.g., using Equation 3.7 yields,
Since the environment is controlled, one can compute “a” in Equation 3.8, as follows:
a=√{square root over (c/(0.5ρ))} (Equation 3:8—Drag\Correction Coefficient),
Where: c—the best fit c, and
The correction for dynamic pressure due to the effect of water velocity on the measured water pressure was investigated in a towing tank under control conditions. The water condition in the towing tank was stagnant before the tests commenced with no visible external influences. The instrument was mounted at a fixed position on the towing cart during the entire tests. The water pressure data collected during the towing tank test is graphically shown in
The methodology outlined under Drag\Correction Coefficient was verified by calculating the theoretical or computed pressure using Equation 3:9 below. Applying Equation 3.9, the measured pressure can be simulated by using the constant Pc and stepping through the velocity runs used during the tests. By way of example,
Equation 3.9 is as follows:
P
com
=P
c−0.5ρ(aV)2 (Equation 3:9—Computed Pressure)
Where: Pc—corrected pressure, and
The methodology outlined under Drag\Correction Coefficient was verified by calculating the corrected pressure using Equation 3:5 above, which is repeated below. The comparison between “Measured pressure” that is the raw pressure sensor readings against the “Corrected pressure” is shown and given in
P
c
=P
m+0.5ρ(aV)2 (Equation 3:5—Corrected Pressure).
1. By way of example, the method for compensating for Venturi effects on pressure sensors in moving water may include the following:
2) A method for compensating for Venturi effects on pressure sensors in moving water and computing a proper instrument depth may include the following:
3. A method for compensating for Venturi effects on pressure sensors in moving water, e.g., by computing a proper instrument depth and collecting a water profile, may include the following:
An example of an algorithm for a hardware/software implementation was developed in the apparatus 10, e.g., including the product sold in the marketplace under the name, FlowTracker2™ ADV®, e.g., as described above, to compensate pressure sensor measurements used to determine for water depth for dynamic pressure, e.g., consistent with that described below:
Dynamic pressure is the kinetic energy per unit volume of fluid and affects the pressure sensor measurements performed by the apparatus 10's internal pressure sensor in flowing water. The extent of the dynamic pressure affecting the pressure sensor measurements is directly related to the water velocity. The correction for dynamic pressure on the apparatus 10's pressure sensor measurements is described herein.
In fluid dynamics, the Total Pressure (P0) is defined as the sum of the Static Pressure (P) and the Dynamic Pressure (Pd), as follows:
P
0
=P+P
d (Equation 4:10—Total Pressure).
The internal pressure sensor implemented in the apparatus 10 provides an accurate measurement of the Total Pressure (P0). Calculating depth from pressure requires the Static Pressure (P) to be known. For still or slow moving water the Dynamic Pressure (Pd) is negligible and thus the Static Pressure (P) and the Total Pressure (P0) are very close. Using the Total Pressure (P0) as measured by the pressure sensor instead of the Static Pressure (P) in these cases provides a good conversion for all practical purposes.
However, for faster flowing water, ignoring the Dynamic Pressures (Pd) is not an option and would result in a significant error in the pressure-to-depth conversion. Correcting for Dynamic Pressure is essential to ensure a proper depth computation.
Dynamic Pressure (Pd) is defined as,
P
d=0.5×WaterDensity×WaterSpeed2 (Equation 4:11—Dynamic Pressure)
Parameters required in Equation 4:11 include the following:
Equation 4:12 may be used to determine corrected water speed, e.g., as follows:
WaterSpeed=AdvWaterSpeed×a (Equation 4:12—Corrected AdvWaterSpeed)
If one substitutes Equation 4:12 in Equation 4:11, then the dynamic pressure can be computed using (Equation 4:13, as follows:
P
d=0.5×WaterDensity×(AdvWaterSpeed×a)2 (Equation 4:13—Dynamic Pressure using AdvWaterSpeed)
Knowing the Dynamic Pressure (Pd) and the Total Pressure (P0)—the static pressure can then be computed, e.g., by using Equation 4:14, as follows:
P=P
0
−P
d (Equation 4:14—Static Pressure)
If one substitutes (Equation 4:13 in Equation 4:14 the final equation for correcting the pressure measured by the apparatus 10's internal pressure sensor may be defined in Equation 4:15, e.g., as follows:
P=P
0−0.5×WaterDensity×(AdvWaterSpeed×a)2 (Equation 4:15—Corrected Pressure)
The corrected pressure may be used, e.g., to compensate for Venturi effects on the pressure sensor by the moving water for taking the water depth measurement, according to the present invention.
While the invention has been described with reference to an exemplary embodiment, it will be understood by those skilled in the art that various changes may be made and equivalents may be substituted for elements thereof without departing from the scope of the invention. In addition, may modifications may be made to adapt a particular situation or material to the teachings of the invention without departing from the essential scope thereof. Therefore, it is intended that the invention not be limited to the particular embodiment(s) disclosed herein as the best mode contemplated for carrying out this invention.
This application claims benefit to provisional patent application Ser. No. 62/430,477 (911-023.7-1/N-YSI-0037US), filed 6 Dec. 2016, which is incorporated by reference in its entirety.
Number | Date | Country | |
---|---|---|---|
62430477 | Dec 2016 | US |