Electrodeless conductivity measuring system

• US 4,220,920 A
• Filed: 03/28/1979
• Issued: 09/02/1980
• Est. Priority Date: 03/28/1979
• Status: Expired due to Term

• Current Assignee: The Foxboro Company (Schneider Electric SE)
• Original Assignee: The Foxboro Company (Schneider Electric SE)
• Inventors: Gross, Thomas A. O.
• Primary Examiner(s): Smith, Alfred E.
• Assistant Examiner(s): Roberts, Charles F.
• Application Number:
  US06/024,554
• Time in Patent Office: 524 Days
• Field of Search: 324/442, 324/445, 336/84 C
• US Class Current: 324/442
• CPC Class Codes: G01N 27/023 where the material is placed in the field of a coil
• CPC Class Codes: G01R 27/02 Measuring real or complex resistance, reactance, impedance, or other two-pole characteristics derived therefrom, e.g. time constant by measuring phase angle only G01R25/00
• CPC Class Codes: G01R 27/22 Measuring resistance of fluids

Abstract

An electrodeless conductivity measuring system of the type employing a spaced pair of toroidal ferromagnetic cores, in which anomalies in the permeance of the cores is alleviated by the use of non-permeable shields of conductive material.

Claims

1. An electrodeless conductivity probe, comprising first and second toroidal ferromagnetic cores, means mounting said cores in spaced relationship, a first and a second shield of electrically conductive, non-permeable material partially surrounding said first and said second cores, respectively, a first winding over said first shield and linking said first core, and a second winding over said second shield and linking said second core.

2. The apparatus of claim 1, in which said shields each comprise a partial toroidal core box extending around the associated core at least 180°

, leaving an unshielded region not exceeding 180°

, and a non-conductive element completing said core box and secured to said shield, and in which the shielded regions of said cores are in confronting relationship.

3. The apparatus of claim 1, further comprising means for applying a voltage at a predetermined frequency across said first winding, and means connected to said second winding for detecting a signal induced in said secondary winding by a conductive medium linking said cores.

4. The apparatus of claim 1, further comprising an oscillator connected to said first winding to apply an alternating voltage at a predetermined frequency to said first winding, and synchronous detection means connected to said oscillator and said second winding for producing an output signal in response to voltage induced in said second winding at said predetermined frequency and in a predetermined phase relative to said voltage applied to said first winding, said synchronous detecting means being non-responsive to voltages induced in said second winding at said predetermined frequency and displaced in phase by nπ

/2, where n is an odd positive integer, from said predetermined phase;

said shields having a combined thickness such that flux passing through both shields at said predetermined frequency is shifted in phase by nπ

/2.

7. The conductivity probe of claim 3, in which the total thickness of said shields is at least δ

cm., where δ

=5033√

π

/μ

f, where π

is the resistivity of said shields in ohm·

cm, μ

is the relative permeability of said shields, and f is said predetermined frequency in Hertz.

5. An electrodeless conductivity probe, comprising first and second toroidal ferromagnetic cores, means mounting said cores in adjacent spaced relationship, at least one shield of electrically conductive, non-permeable material partially surrounding at least a first of said cores and surrounding at least 180°

of said first core on the side facing the other of said cores, and a winding on each of said cores.

6. The conductivity probe of claim 5, in which the total shield thickness is at least δ

, where δ

=5033√

ρ

/μ

f, one of said cores is adapted to be excited at a frequency f Hertz, μ

is the relative permeability of said material, and ρ

is the resistivity of said material in ohm·

cm.