The present invention relates generally to viscosity sensors.
The viscosity of certain fluids such as engine lubricating oil is an important parameter. Vehicle engines, for instance, are typically designed with an oil viscosity range in mind, and if the oil is too viscous or not viscous enough, engine damage can result. Accordingly, it is an object of the invention to provide a simple, elegant, inexpensive viscosity sensor that may be employed in, e.g., vehicle engines.
A viscosity sensor has one or more piezoelectric elements and a housing holding the piezoelectric element in a fluid chamber. An elongated amplification channel is formed in the housing and extends away from the chamber. The piezoelectric element can be excited to induce fluid movement that in turn induces the piezoelectric element to output a sensor signal representative of the viscosity of the fluid.
In one embodiment, two piezoelectric elements are provided in the housing and are closely spaced apart coaxially with each other with the channel being intermediate the piezoelectric elements in the transverse vertical plane of the sensor. The chamber may be a disk-shaped chamber that is between the piezoelectric elements and that communicates with the channel. The chamber holds the fluid. A computer such as a vehicle ECM may be provided for receiving the sensor signal.
In another aspect, a method for measuring the viscosity of a fluid includes disposing one or more piezoelectric elements in the fluid and applying an excitation signal to the piezoelectric element. An induced signal is sensed from the piezoelectric element and correlated to a viscosity. If desired, the induced signal can be processed with an exponential function characterized by exponential coefficients establishing a sensor output index.
In yet another aspect, a sensor system for outputting an induced signal representing the viscosity of a fluid inducing the signal includes piezoelectric means for creating motion in the fluid and, in response to the motion, generating the induced signal. Means are provided for correlating the induced signal to the viscosity.
The details of the present invention, both as to its structure and operation, can best be understood in reference to the accompanying drawings, in which like reference numerals refer to like parts, and in which:
The present invention is intended for application in automotive vehicle systems and will be described in that context. It is to be understood, however, that the present invention could also be successfully applied in many other applications including non-vehicle applications.
Referring initially to
The chamber 28 thus may be defined by a central through-hole in the central sensor plate 26 and may be further defined by disk-shaped depressions in the covers 22, 24, shown and described further below in reference to
The piezoelectric diaphragms 32, 34 may be made of any suitable material that exhibits the piezoelectric effect of mechanically deforming when an excitation signal (from, e.g., the ECM 16 shown in
The overall operation of the sensor 10 may now be understood. The diaphragms 32, 34 may be excited simultaneously with, e.g., one period of a sinusoidal excitation current. The excitation current preferably may be under one kiloHertz and more preferably may be around three hundred (300) Hertz. As understood herein, a low frequency excitation wave is preferred because otherwise the fluid wave generated by the diaphragms could dissipate before reaching the channel 30. Furthermore, higher frequencies can render the system unduly sensitive to small bubbles that may form in the fluid.
Owing to the excitation signal, the diaphragms commence a damped free vibration, deforming to induce waves in the fluid in the chamber 28. The channel 30 serves to amplify the effect in the fluid. In turn, the oscillations in the fluid cause mechanical deformations in the diaphragms 32, 34 which cause the diaphragms to generate electrical sensor signals. The sensor signals may be picked off one or both of the diaphragms and then correlated to viscosity as explained further below.
As shown in the non-limiting embodiment of
Rims “R” may extend slightly radially inwardly from the periphery of the chamber 28, circumscribing the chamber 28 of the central plate 26 to provide seating surfaces for the edges of the diaphragms 32, 34, respectively. The diaphragms 32, 34 preferably are tightly bonded to the rims “R” to ensure fluid tightness.
The sensor signal may be digitized and filtered to remove high frequency noise. The digitized filtered signal may then be processed with an exponential function to fit the straight line 46 shown in
In undertaking the above process, the peak points of the piezoelectric output signal can be fit to a curve from which an exponential function is obtained that contains the peak points. The coefficient of the exponent obtained from this function corresponds to the damping ratio factor, which is referred to herein as the sensor output index.
In
Thus, to calibrate the sensor, fluids of known viscosities and temperatures may be processed in the sensor 10 to establish correlations between the exponential coefficients that establish the sensor output index and the viscosity scale of the x-axis in
While the particular VISCOSITY SENSOR is herein shown and described in detail, it is to be understood that the subject matter which is encompassed by the present invention is limited only by the claims. For example, in addition to the above connection mechanisms, other quick connect/quick disconnect type of mechanisms may be used.