Measuring and testing – Volume or rate of flow – By measuring electrical or magnetic properties
Reexamination Certificate
2000-11-02
2002-10-15
Fuller, Benjamin R. (Department: 2855)
Measuring and testing
Volume or rate of flow
By measuring electrical or magnetic properties
Reexamination Certificate
active
06463807
ABSTRACT:
CROSS REFERENCE TO RELATED APPLICATIONS
Not Applicable
STATEMENT REGARDING FEDERALLY SPONSORED RESEARCH OR DEVELOPMENT
Not Applicable
BACKGROUND OF THE INVENTION
1. Background Information
This invention relates to apparatus and method for determining the rate of flow of a fluid by measuring an electrical potential difference developed in the fluid as the fluid moves through a magnetic field. The potential difference is sensed by at least one pair of electrodes contacting the liquid and spaced apart from each other along a line that is generally orthogonal to both the direction in which the flow is being measured and a magnetic field produced by a magnet. The measured potential difference has a magnitude proportional to the flow rate of the fluid. As is known to those skilled in the art, the overall potential difference between two such electrodes, usually termed a voltage difference, has two major components: a) a flow-related voltage due to the flow of the fluid when acted upon by the magnetic field; and b) a net ‘drift voltage’, which is the sum of voltages due to all other factors, such as electrode polarization.
In prior art flow sensors of this type, alternating magnetic fields from electromagnets have generally been used to provide an alternating magnetic field. The alternating magnetic field facilitates signal amplification and processing that accepts flow-related electrode signals while rejecting electrode drift signals which would otherwise introduce serious measurement errors. However, generating those fields and processing the measured voltage signals requires sophisticated circuits and techniques which raise the cost of such sensors and limit their application.
An example of a radical departure from the prior art is found in my U.S. Pat. No. 6,085,599 in which I teach mechanical means to alternate the polarity of the magnetic fields. Those techniques provide practical ways of simplifying magnetic flow sensors and reducing their costs. However, the use of mechanical means to alternate the field polarity, even though this may be performed with a high degree of ruggedness and reliability, reduces the marketability of such an instrument. The disclosure of U.S. Pat. No. 6,085,599 is incorporated herein by reference.
Another problem encountered in prior art magnetic flow sensors is that of entrapment of ferromagnetic debris. This is particularly true of arrangements using permanent magnets as in my U.S. Pat. No. 6,085,599. Such debris can change the magnetic flux distribution and thereby alter the calibration of the flow meter. Moreover, pieces of ferromagnetic debris can sometimes bridge the normally electrically isolated electrodes, producing a conductive path that may partially short out the electrode signals and thereby reduce the output voltage. Fine particles of debris can also form a film on normally insulating portions of the structure surrounding the electrodes and thereby shunt the electrode signals.
It is therefore an object of the invention to provide a practical magnetic flow sensor using stationary permanent magnets.
It has also been discovered that the methods of the present invention can be used with conventional magnetic flow sensors using electromagnets to improve their performance and such is therefore a further objective of the invention.
BRIEF SUMMARY OF THE INVENTION
The above and other objects are attained by magnetic flow sensors in accordance with various preferred embodiments of the present invention. In preferred embodiments the magnetic axis i.e., the line extending from the south to the north pole) of a permanent magnet is oriented generally perpendicular to a direction of flow of a fluid. As is known in the magnetic flow metering art, the flux from a magnet arranged in this fashion generates, in the fluid, a voltage difference proportional to the flow rate of the fluid. This voltage difference is sensed by a pair of electrodes (which preferably have the same size and shape and are made of the same material) and which are spaced apart from each other along a line that is generally orthogonal to both a direction of flow and the magnetic axis. The electrodes are preferably short circuited to each other most of the time so that polarization and other DC factors responsible for DC electrode drift are minimized over a period of time. Periodically, the short circuit is opened for a brief time interval so that the flow-generated voltage difference then appearing at the electrodes may be detected and processed to provide an output signal representative of the flow rate of the fluid. During the open circuit portion of this duty cycle, drift inducing factors do begin to cause drift signals to develop. However, they develop relatively slowly compared to the brief time interval required to detect the flow rate signal and thereby enable electronic processing to discriminate between the two. This method of flow rate detection thereby enables an extremely simple magnetic flow sensor to be made.
Several sensing heads of the general configuration recited above—i.e., one or more permanent magnets with an adjacent pair of electrodes—may be used at different locations to sense the flow rate of a fluid. For example, two sensing heads can be spaced out along a section of pipe or tubing. The flow rate voltages from the plural heads can be polarized to be additive in the associated signal processing circuitry. DC drift voltages at the various electrodes would, however, have a random distribution of magnitudes of polarities and would thus average out to zero when the overall electrode voltages were summed. The magnitude of the flow related signal can thus be made relatively high compared to the error related drifts, thereby improving sensor performance. The present invention is well adapted to such configurations because of the low cost of the components that are used.
In addition to improving the ratio of flow-related signals to drift signals, a two-headed sensing configuration comprising an upstream head and a downstream head can be used to detect the presence of ferromagnetic debris, most of which is likely to be trapped by the permanent magnet portion of the upstream sensing head. This debris can alter the magnetic flux distribution and shunt the flow-related voltage of the upstream head, thereby reducing the value of its flow-related voltage. Thus, if one compares the flow-related signals from identical upstream and downstream sensing heads and finds that those signals differ by more than some predetermined threshold value, one can conclude that at least the upstream head is contaminated with ferromagnetic debris and that cleaning of the wetted portions of the sensor is required.
Although various numbers of sensing heads can be used in the invention, in preferred methods of operation all of the paired electrodes of all the sensing heads are shorted together during a relatively long portion of an operating duty cycle. During a relatively short portion of the duty cycle a switching device can be used to sequentially open circuit pairs of electrodes and connect each open circuited pair to a common measurement circuit in order to measure its flow-related open circuit voltage. A switching device can also open circuit pairs of the electrodes and connect them to separate inputs of a common measurement circuit to measure the flow related voltages. Those skilled in the signal processing arts will realize that with these and other arrangements for aggregating open circuit voltages one can obtain a simple average of the output voltages, an average of the sum of the individual output voltages, or various other selected statistical measures.
Generally speaking, the flow-generated component of the open circuit voltage will appear quickly (i.e., it can be measured after a predictable rise time that depends primarily on the resistivity and dielectric constant of the flowing fluid) after an electrode pair is switched from a shorted to an open circuit state. Electrode pair drift voltages, by contrast, depend on electrode polarization and other generally much more slowly acting e
Fuller Benjamin R.
Kiewit David
Thompson Jewel V.
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