Fluid dielectric constant sensing device and method employing the same

• US 6,320,393 B1
• Filed: 03/18/1999
• Issued: 11/20/2001
• Est. Priority Date: 10/20/1998
• Status: Expired due to Fees

• Current Assignee: Mitsubishi Denki Kabushiki Kaisha (Mitsubishi Electric Corporation)
• Original Assignee: Mitsubishi Denki Kabushiki Kaisha (Mitsubishi Electric Corporation)
• Inventors: Ono, Mitsuhiro, Nagano, Susumu, Yasui, Katsuaki
• Primary Examiner(s): Metjahic, Safet
• Assistant Examiner(s): KERVEROS, DEMETRIOS C
• Application Number:
  US09/271,429
• Time in Patent Office: 978 Days
• Field of Search: 324/694, 324/654, 324/656, 324/663, 324/533, 324/534, 324/642, 324/643
• US Class Current: 324/663
• CPC Class Codes: F02D 19/0634 Determining a density, viscosity, composition or concentration F02D19/087 takes precedence
• CPC Class Codes: F02D 19/084 Blends of gasoline and alcohols, e.g. E85
• CPC Class Codes: F02D 2200/0611 Fuel type, fuel composition or fuel quality
• CPC Class Codes: F02D 41/0025 Controlling engines characterised by use of non-liquid fuels, pluralities of fuels, or non-fuel substances added to the combustible mixtures
• CPC Class Codes: G01N 27/221 by investigating the dielectric properties using microwaves G01N22/00; measuring loss factors or dielectric constants per se G01R27/26
• CPC Class Codes: G01N 27/226 Construction of measuring vessels; Electrodes therefor
• CPC Class Codes: Y02T 10/30 Use of alternative fuels, e.g. biofuels

Abstract

A dielectric constant sensing device of the present invention comprises a transmission line consisting of a first electrode formed of a conductor being wound like a longitudinal cylinder, a second electrode provided to be separated from the cylindrical surface of the first electrode at a predetermined distance, and a chamber for introducing a measured fluid between the first electrode and the second electrode, whereby a dielectric constant of the measured fluid can be sensed based on a rate of a pulse voltage wave propagated over the transmission line. Accordingly, the fluid dielectric constant sensing device which is able to attain high precision by a simple structure can be provided.

Claims

1. A fluid dielectric constant sensing device comprising:

a first electrode formed of a conductor being wound like a longitudinal cylinder;

a second electrode separated from the cylindrical surface of the first electrode at a predetermined distance;

an introducing portion for introducing a measured fluid between the first electrode and the second electrode;

a pulse signal generating means for applying a pulse signal to a transmission line which includes the first electrode, the second electrode, and the introducing portion;

a pulse signal sensing means for sensing the pulse signal after the pulse signal has propagated over the transmission line; and

a dielectric constant sensing means for sensing a dielectric constant of the measured fluid based on a period of time from generation of the pulse signal to detection of the pulse signal by the pulse signal sensing means.

2. The fluid dielectric constant sensing device of claim 1, wherein the first electrode is formed to have a longitudinal cylinder whose a ratio of length/diameter is more than 4.

3. The fluid dielectric constant sensing device of claim 1, wherein an input impedance of the pulse signal sensing means viewed from the transmission line side is set in a range of half to twice of a characteristic impedance of the transmission line.

4. The fluid dielectric constant sensing device of claim 3, wherein the pulse signal generating means and the pulse signal sensing means comprises one inverter.

5. The fluid dielectric constant sensing device of claim 1, wherein the first electrode has an insulating coating of predetermined thickness between the first electrode and the second electrode, and a thickness of the insulating coating is selected to such extent that reflection of the pulse signal is not substantially caused at the pulse signal sensing means.

6. The fluid dielectric constant sensing device of claim 1, wherein a filter means is provided to at least one of the pulse signal generating means and the pulse signal sensing means.

7. The fluid dielectric constant sensing device of claim 6, wherein the filter means is composed of second order filter or high order filter.

8. The fluid dielectric constant sensing device of claim 1, wherein a time required for propagation of the pulse signal over the transmission line is set large to such extent that the time is not affected substantially by variation in a propagation delay time when the pulse signal generating means receives an instruction signal and then responds to the instruction signal, or by variation in the propagation delay time when the pulse signal sensing means receives the pulse signal after the pulse signal has propagated over the transmission line and then responds to the pulse signal.

9. The fluid dielectric constant sensing device of claim 8, wherein a core or a yoke formed of magnetic material is provided to at least one of the first electrode and the second electrode.

10. The fluid dielectric constant sensing device of claim 8, wherein a temperature characteristic of permeability of the core or the yoke has a temperature characteristic which is opposite to that of the dielectric constant of the measure fluid.

11. The fluid dielectric constant sensing device of claim 1, wherein the second electrode has a protection member.

12. The fluid dielectric constant sensing device of claim 1, wherein one end of the first electrode is connected to the pulse signal generating means and other end of the first electrode is opened or connected to a constant voltage portion, and the dielectric sensing means senses the dielectric constant of the measured fluid based on a period of time during which the pulse signal being generated by the pulse signal generating means is input from a first end of the first electrode and then reflected at the other end of the first electrode to return to the first end of the first electrode.

13. The fluid dielectric constant sensing device of claim 1, wherein the pulse signal generating means and the pulse signal sensing means are composed of one Schmidt inverter.

14. The dielectric constant sensing device of claim 1, wherein one end of the first electrode is connected to the pulse signal generating means and the other end of the first electrode is connected to the pulse signal sensing means, and the dielectric constant sensing means senses the dielectric constant of the measured fluid based on a period or time during which the pulse signal being generated by the pulse signal generating means is input from one end of the first electrode and then reaches the other end of the first electrode.

15. A fluid dielectric constant sensing method comprising the steps of:

providing a first electrode formed of a conductor being wound as a longitudinal cylinder and a second electrode provided to be separated from a cylindrical surface of the first electrode at a predetermined distance;

forming a signal transmission line as a distributed constant circuit by the first electrode, the second electrode, and a measured fluid introduced between the first and second electrodes; and

sensing a dielectric constant of the measured fluid based on a change in propagation rate of the signal propagated over the transmission line caused by an affect of the dielectric constant of the measured fluid upon a constant of the distributed constant circuit.

16. The fluid dielectric constant sensing method of claim 15, wherein a sensing means for sensing a signal propagated over the transmission line is provided, and difference between a characteristic impedance of the transmission line and an input impedance of the sensing means is adjusted such that the signal is not substantially reflected at an input portion of the sensing means.

17. The dielectric constant sensing method of claim 15, wherein a passage width limiting means for a passage width of the measured fluid being introduced between the first electrode and the second electrode is provided, and the passage width limiting means limits change in the characteristic impedance of the transmission line caused by change in the dielectric constant of the measured fluid.

18. The fluid dielectric constant sensing method of claim 15, wherein a time required for propagation of the pulse signal over the transmission line is set large to such extent that the time is not affected substantially by variation in a propagation delay time when the pulse signal generating means receives an instruction signal and then responds to the instruction signal, or by variation in the propagation delay time when the pulse signal sensing means receives the pulse signal after the pulse signal has propagated over the transmission line and then responds to the pulse signal.

19. The fluid constant sensing method of claim 15, wherein a propagation rate of the signal propagated over the transmission line is calculated based on a period of time during which the pulse signal generated by the pulse signal generating means is input from a first end of the first electrode and then reflected at the other end to return to the first end of the first electrode.

20. The fluid dielectric constant sensing method of claim 15, wherein a propagation rate of the signal propagated over the transmission line is calculated based on a period of time during which the pulse signal being generated by the pulse signal generating means is input from one end of the first electrode and then reaches the other end of the first electrode.