Single coil conductance measuring apparatus

• US 6,359,449 B1
• Filed: 06/29/1999
• Issued: 03/19/2002
• Est. Priority Date: 06/29/1999
• Status: Expired due to Fees

• Current Assignee: INTELLECTUAL PROPERTY LLC
• Original Assignee: INTELLECTUAL PROPERTY LLC
• Inventors: Bell, Marshall J., Reining, William N.
• Primary Examiner(s): Metjahic, Safet
• Assistant Examiner(s): LEROUX, ETIENNE PIERRE
• Application Number:
  US09/343,166
• Time in Patent Office: 994 Days
• Field of Search: 324/445, 324/248, 324/117.R, 324/633, 324/634, 324/635, 324/652, 324/691, 324/692, 324/707, 324/708, 331/8, 331/11, 331/14, 331/137, 600/484, 600/481, 600/534, 600/538
• US Class Current: 324/692
• CPC Class Codes: G01R 27/08 Measuring resistance by measuring both voltage and current

Abstract

A conductance sensor uses a high impedance feedback oscillator to drive a single coil at the natural resonant frequency of the coil coupled to a measured material. The amplitude of the driving signal is also feedback controlled. The error signal of the amplitude control yields a measurement of resistance of the measured material. The combination of frequency adjustment and amplitude control eliminates non-resistance impedance effects and amplitude-dependent effects allowing high precision, high sensitivity measurement.

Claims

1. A method of quantitative measurement of the resistance of a remote substance using a single coil comprising the steps of:

(a) exciting the coil with an electrical signal to produce an electromagnetic field enveloping the remote substance;

(b) allowing the frequency of the electric signal to be at the resonant frequency of the coil as affected by the remote substance;

(c) adjusting a control signal controlling the amplitude of the electrical signal so that the electric signal at the coil substantially equals a predetermined standard level; and

(d) deriving a resistance value of the remote substance based on the adjusted control signal independent of any deformation of the coil, wherein the resistance value of the remote substance is only substantially indicative of a real portion of an impedance of the remote substance and is not substantially indicative of any reactance or inductance of the remote substance or the coil.

2. The method of claim 1 wherein the remote substance is a liquid and including the step of flowing the liquid through a tube positioned in the electromagnetic field.

3. The method of claim 1 wherein step (b) is performed by an amplifier having positive feedback from the coil.

4. The method of claim 1 wherein step (c) is performed using a rectifier receiving the electric signal from the coil and rectifying the electric signal synchronously with the phase of the electric signal.

5. The method of claim 4 wherein step (c) is performed by multiplying the electric signal by itself.

6. A sensor for remote measurement of resistance of a sample material comprising:

a conductive coil;

an oscillator connected to the conductive coil to;

(1) drive the conductive coil with an oscillating current;

(2) to receive feedback from the conductive coil to allow the frequency of the oscillating current to be at a varying resonant frequency of the conductive coil as coupled to the sample; and

an amplitude control circuit connected to the oscillator to adjust the oscillating current; and

an output providing an error signal indicating the adjustment of the amplitude control circuit, the error signal providing a measure of the effective resistance of the sample,

wherein the measure of the effective resistance of the sample can be determined independent of any deformation of the conductive coil, and wherein the effective resistance of the sample is only substantially indicative of a real portion of an impedance of the sample and is not substantially indicative of any reactance or inductance of the sample or the conductive coil.

7. The sensor of claim 6 wherein the oscillator is an amplifier having an output connected to the coil and configured for positive feedback.

8. The sensor of claim 6 wherein the oscillator includes a gain controlled amplifier having a gain control input signal reflecting the voltage amplitude of the oscillating current;

and

wherein the error signal is the gain control input.

9. The sensor of claim 8 wherein the gain control input is provided by a rectifier, rectifying the oscillating current synchronously with the oscillating current.

10. The sensor of claim 9 wherein the rectifier is a multiplier multiplying the oscillating current by itself.

11. The sensor of claim 6 including a guide for positioning the measured material in a predetermined relationship with respect to the coil.

12. The sensor of claim 6 wherein the guide is a non-conductive tube through which a liquid may pass.