Dielectric constant monitor

• US 5,148,125 A
• Filed: 06/21/1991
• Issued: 09/15/1992
• Est. Priority Date: 03/03/1989
• Status: Expired due to Term

• Current Assignee: Lincoln Ventures Limited
• Original Assignee: Lincoln County
• Inventors: Woodhead, Ian M., Hirsch, Stephen J. J.
• Primary Examiner(s): Pascal, Robert J.
• Application Number:
  US07/721,921
• Time in Patent Office: 452 Days
• Field of Search: 331/135, 331/136, 331/65, 324/633, 324/634, 324/682, 324/690
• US Class Current: 331/135
• CPC Class Codes: G01N 27/223 for determining moisture content, e.g. humidity rain detectors on vehicle windows B60S1/0825
• CPC Class Codes: G01N 33/246 for water content for control of watering A01G25/167
• CPC Class Codes: G01R 27/2664 Transmission line, wave guide (closed or open-ended) or strip - or microstrip line arrangements

Abstract

Monitoring of the average dielectric constant in an extended volume of a medium such as soil is achieved using an oscillator incorporating a transmission line to be embedded in the medium. The transmission line is connected as the feedback loop of an amplifier, for one-way propagation of an electrical signal with a delay determined largely by the dielectric properties of the medium, such as its moisture content. The oscillation frequency is indicative of the dielectric constant of the medium.

Claims

1. Apparatus for monitoring the dielectric constant of a material comprising:

an amplifier having input and output ports,

a transmission line connected at one end to the amplifier input and at the other end to the amplifier output forming a feedback loop, and

output means connected to the loop;

wherein

the transmission line is embedded at least partly in the material when monitoring takes place,

an electrical signal propagates one-way along the transmission line and through the amplifier in passing around the loop,

the signal is inverted on each passage around the loop to sustain an electrical oscillation at a frequency determined in part by the propagation delay of the transmission line, and

the oscillation frequency is used by the output means to provide a measure of the dielectric constant of the material.

2. Apparatus according to claim 1 wherein the transmission line comprises a twin lead cable.

3. Apparatus according to claim 1 wherein the amplifier comprises an inverter connected to one lead of the transmission line, and a comparator.

4. Apparatus according to claim 1 wherein the electrical signal is inverted by the amplifier.

5. Apparatus according to claim 2 wherein the electrical signal is inverted by crossing the leads of the cable between connection of the transmission line to the amplifier input and the amplifier output.

6. Apparatus according to claim 1 wherein the transmission line is unbalanced with respect to ground.

7. Apparatus according to claim 1 further comprising:

a comparison amplifier having input and output ports,

a relatively-short length transmission line connected at one end to the comparison amplifier input and at the other end to the comparison amplifier output comprising a second feedback loop, and

second output means connected to the second feedback loop;

wherein an electrical signal propagating around the second feedback loop will be inverted and a comparison electrical oscillation will be sustained at a frequency determined largely by the propagation delay of the comparison amplifier, and

the comparison oscillation frequency is used by the second output means for correction of the measure of the dielectric constant of the material.

8. A method of monitoring the dielectric constant of a material comprising:

embedding a transmission line in the material as part of an amplifier feedback loop,

propagating an electrical signal one-way along the transmission line and through the amplifier,

inverting the signal on each passage around the loop to create an electrical oscillation at a frequency determined in part by the propagation delay of the transmission line, and

using the frequency to provide a measure of the dielectric constant of the material.

9. A method according to claim 8 further comprising correcting the measure of the dielectric constant by comparison of the frequency with a second frequency output from a second amplifier and feedback loop having a relatively-short transmission line not embedded in the material but otherwise substantially identical to the first amplifier and feedback loop.