Measuring and testing – Volume or rate of flow – Mass flow by imparting angular or transverse momentum to the...
Reexamination Certificate
2002-12-06
2004-10-05
Lefkowitz, Edward (Department: 2855)
Measuring and testing
Volume or rate of flow
Mass flow by imparting angular or transverse momentum to the...
Reexamination Certificate
active
06799476
ABSTRACT:
BACKGROUND OF THE INVENTION
1. Field of the Invention
This invention relates to a method for operating a mass flowmeter that employs the Coriolis principle and is equipped with a Coriolis-type measuring tube, an oscillator associated with and stimulating said Coriolis measuring tube, and a transducer dedicated to said Coriolis measuring tube for collecting the Coriolis forces and/or oscillations derived from Coriolis forces. The invention further relates to a mass flowmeter that operates by the Coriolis principle and incorporates a Coriolis measuring tube, an oscillator stimulating the Coriolis measuring tube, and a transducer dedicated to said Coriolis measuring tube for collecting Coriolis forces and/or oscillations derived from Coriolis forces.
2. Description of the Prior Art
Prior-art Coriolis-type mass flowmeters usually feature separate ports respectively for power input, i.e. for the supply of electric power, and for the output of the measuring signal, i.e. for data transfer. Such separation of power input and data output makes the power supply virtually independent of the type of data transfer, meaning that in any event the power input is not restricted in a way that would limit the amount of power that can be fed into the mass flowmeter. It follows that a power supply unit can be selected which will ensure adequate power for the mass flowmeter and any under all operating conditions. This prevents interruptions in the operation of the mass flowmeter in situations where the power consumption of its components would otherwise exceed the available amount of electric power.
On the other hand, it would be desirable to operate the mass flowmeter of the type described above via a two wire input/output interface, meaning a port that can feed the necessary electric power to the mass flowmeter and at the same time output the measuring data. Such a two wire interface typically serves for the connection of a two wire process control loop for both signal transmission and supply of electric power, typically limited by a 4-20 mA current at a 24 V DC voltage. The operation of the mass flowmeter via a two wire port may be desirable, for instance, for explosion-protection considerations, given that a two wire port permits intrinsically safe operation of the mass flowmeter in that the maximum power available to the mass flowmeter is limited to a point where no spark with an ignition potential could be generated.
When a two wire port of the above type is used, the measuring signal is usually output with a current value of between 4 mA and 20 mA, so that in any case a current maximum of 4 mA is available for powering the components of the mass flowmeter. Any current in excess of that value is usually of no consequence given the fact that the amount of power for operating the components of the mass flowmeter must be predefined and preset. As a result, the effective power available for operating a Coriolis-type mass flowmeter with a two wire port for electric power input and measuring signal output is severely limited to a point where its practical use is difficult at best.
SUMMARY OF THE INVENTION
It is therefore the objective of this invention to introduce a method for operating a mass flowmeter that employs the Coriolis principle, and a mass flowmeter based on the Coriolis principle, that permits operation even with a limited maximum of available electric power and subject to time variations.
Referring to the aforementioned method for operating a mass flowmeter, that objective is achieved by this invention whereby the electric power consumed within the mass flowmeter is controlled as a function of the electric power actually available.
The method according to the invention thus prevents the electric power consumption by the components of the mass flowmeter from exceeding the available electric power, which does not necessarily have to involve an adjustment to the worst-case situation in which only the smallest amount of power is available. Instead, the control according to this invention of the electric power taken up and consumed within the mass flowmeter allows at any time the use of virtually all of the current as a function of the electric power available.
In this context it should be pointed out that, of course, the method according to the invention is not based on the simplistic realization that less available electric power necessarily leads to less power consumption. Rather, the method of this invention provides for the active control of the power consumption by the components of the mass flowmeter.
According to a preferred embodiment of the invention, such specific control of the power consumed in the mass flowmeter is provided by controlling the mean value of the oscillatory energy of the Coriolis measuring tube in adaptation to the electric power available. In a preferred implementation of the invention, this is accomplished by energizing the oscillator within the limits of the available electric power, preferably by controlling its amplitude. The desired adaptation to the available electric power can be achieved in that, whenever less electric power is available, the oscillator is activated with a lower amplitude. In other words, less available electric power will reduce the oscillation amplitude and thus the oscillating energy of the Coriolis measuring tube. If and when the available electric power rises again, the oscillating amplitude of the Coriolis measuring tube can rise as well. The fact that, within the constraints of harmonic oscillations, a higher oscillating amplitude of the Coriolis measuring tube is preferred over a lower amplitude is obviously attributable to the better signal-to-noise ratio obtainable with higher oscillating amplitudes in the Coriolis measuring tube.
Yet the mean-value oscillatory energy of the Coriolis measuring tube can be varied in other ways as well. For example, another preferred implementation of the invention, employed as an alternative or in addition to the above method, provides for the oscillator to be activated at time intervals as a function of the available electric power. Energizing the oscillator with interstitial time gaps means that, in contrast to conventional operation, the activation of the oscillator no longer takes place at the excitation frequency which usually corresponds to the resonance frequency of the Coriolis measuring tube within the excitation oscillation. Instead, in this preferred implementation of the invention, the oscillator, while still stimulated in a manner whereby the oscillation of the Coriolis measuring tube remains unchanged in terms of the aforementioned excitation oscillation, there is no activation of the oscillator during predefined oscillation cycles. For example, the oscillator may only be energized at certain time intervals, i.e. it is activated at the excitation frequency within a predefined periods while merely co-resonating with the Coriolis measuring tube during the passive intervals that follow.
For measuring operations it is important, however, that the oscillation of the Coriolis measuring tube is not stopped, meaning that the passive intervals in which no excitation takes place are preferably short enough to prevent the ever-present attenuation from causing a complete decay of the oscillation of the Coriolis measuring tube. As an alternative to the excitation of the Coriolis measuring tube at time intervals, one could conceivably stimulate the Coriolis measuring tube via the oscillator only during every nth cycle of the excitation oscillation, where n is an integer.
As an alternative or in addition to controlling the electric energy taken up and consumed in the mass flowmeter by means of the oscillatory energy of the Coriolis measuring tube, it is entirely possible within the scope of this invention to control all separate power-consuming components of the mass flowmeter. For example, a preferred implementation of the invention provides for an analog-to-digital converter (A/D converter) to accomplish the conversion of the measuring signal emanating from the transducer by controlling the
Cesari and McKenna LLP
Krohne A.G.
Lefkowitz Edward
Thompson Jewel V.
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