초록 ▼

A non-contact probe for determining the conductivity of coating materials is disclosed. The probe includes a free running oscillator operating at a selected frequency, a sensor made up of an LC circuit, a detector for detecting a change in the LC circuit in response to change in the sensor coil indu

A non-contact probe for determining the conductivity of coating materials is disclosed. The probe includes a free running oscillator operating at a selected frequency, a sensor made up of an LC circuit, a detector for detecting a change in the LC circuit in response to change in the sensor coil induction, and a processor for converting the detected changes in the signal to surface conductivity data. The detector may be a frequency detector that detects changes in the resonant frequency of the LC circuit or the detector may be a magnitude detector that detects changes in the signal magnitude of the LC oscillator. The sensor is the coil inductor of the LC circuit. Inductance of the sensor coil is variable depending on conductivity of the material near the sensor coil.

대표청구항 ▼

1. A non-contact surface conductivity measurement probe for conductivity measurement of a material having a conductive surface, the probe comprising:(a) an oscillator operating at a selected oscillator frequency;(b) a sensor comprising an LC circuit that is an integral part of the oscillator, the LC

1. A non-contact surface conductivity measurement probe for conductivity measurement of a material having a conductive surface, the probe comprising:(a) an oscillator operating at a selected oscillator frequency;(b) a sensor comprising an LC circuit that is an integral part of the oscillator, the LC circuit including a sensor coil (L), inductance of the sensor coil being variable depending on conductivity of the material near the sensor coil;(c) a frequency detector for detecting a change in the resonant frequency of the LC circuit in response to change in the sensor coil induction;(d) a processor for converting detected changes in the resonant frequency to surface conductivity data; and(e) a spacer for maintaining the sensor coil at a fixed distance from the conductive surface. 2. The probe of claim 1, wherein the oscillator is a free running oscillator. 3. The probe of claim 2, wherein the free running oscillator is a Colpitts oscillator circuit. 4. The probe of claim 1, wherein the oscillator frequency is a radio frequency. 5. The probe of claim 4, wherein the oscillator frequency is about 21 MHz. 6. The probe of claim 1, wherein the probe is maintained at the fixed distance from the conductive surface-in order to determine a surface resistance measurement based on a shift in the resonant frequency. 7. The probe of claim 1, further comprising a display device for displaying output representative of the conductivity measurement. 8. A non-contact surface conductivity measurement probe for conductivity measurement of a material having a conductive surface, the probe comprising:(a) an oscillator operating at a selected oscillator frequency;(b) a sensor comprising an LC circuit that is an integral part of the oscillator, the LC circuit including a sensor coil (L), inductance of the sensor coil being variable depending on conductivity of the material near the sensor coil;(c) a frequency detector for detecting a change in the resonant frequency of the LC circuit in response to change in the sensor coil induction; and(d) a processor for converting detected changes in the resonant frequency to surface conductivity data;wherein the sensor coil is maintained at a fixed distance from the conductive surface—in order to determine a surface resistance measurement based on a shift in the resonant frequency, the shift in the resonant frequency being mapped to a set of known thin film resistance standards to yield the surface resistance measurement as an equivalent reading in Ω/sq. 9. The probe of claim 8, wherein the set of known thin film resistance standards is stored in the processor. 10. The probe of claim 8, wherein the probe has a surface resistance range of about 0.01Ωsq to about 30Ω/sq. 11. The probe of claim 8, wherein the material is a non-magnetic conductive material. 12. The probe of claim 8, wherein the material is a ferromagnetic material. 13. A non-contact surface conductivity measurement probe for conductivity measurement of a material, the probe comprising:(a) an oscillator operating at a selected oscillator frequency;(b) a sensor comprising an LC circuit that is an integral part of the oscillator, the LC circuit including a sensor coil (L), inductance of the sensor coil being variable depending on conductivity of the material near the sensor coil;(c) a frequency detector for detecting a change in the resonant frequency of the LC circuit in response to change in the sensor coil induction; and(d) a processor for converting detected changes in the resonant frequency to surface conductivity data;wherein a MagRAM coating is applied on top of the material and the conductivity measurement is used to determine a thickness of the MagRAM coating by magnetic induction. 14. The probe of claim 13, wherein the material has a conductive substrate. 15. The probe of claim 13, wherein the material has non-conductive substrate. 16. The probe of claim 13, wherein the MagRAM coating is covered by a non-conductive pain t coat. 17. A non-contact surface conductivity measurement probe for conductivity measurement of a material having a conductive surface, the probe comprising:(a) an oscillator operating at a selected oscillator frequency;(b) a sensor comprising an LC circuit that is an integral part of the oscillator, the LC circuit including a sensor coil (L), inductance of the sensor coil being variable depending on conductivity of the material near the sensor coil;(c) a signal magnitude detector for detecting a change in the signal magnitude of the LC circuit in response to change in the sensor coil induction;(d) a processor for converting detected changes in the signal magnitude to surface conductivity data; and(e) a spacer for maintaining the sensor coil at a fixed distance from the conductive surface. 18. The probe of claim 17, wherein the oscillator is a free running oscillator. 19. The probe of claim 18, wherein the free running oscillator is a Colpitts oscillator circuit. 20. The probe of claim 17, wherein the oscillator frequency is a radio frequency. 21. The probe of claim 20, wherein the oscillator frequency is about 21 MHz. 22. The probe of claim 17, wherein the probe is maintained at the fixed distance from the conductive surface in order to determine a surface resistance measurement based on a shift in the signal magnitude. 23. The probe of claim 17, further comprising a display device for displaying output representative of the conductivity measurement. 24. A non-contact surface conductivity measurement probe for conductivity measurement of a material having a conductive surface, the probe comprising:(a) an oscillator operating at a selected oscillator frequency;(b) a sensor comprising an LC circuit that is an integral part of the oscillator, the LC circuit including a sensor coil (L), inductance of the sensor coil being variable depending on conductivity of the material near the sensor coil;(c) a signal magnitude detector for detecting a change in the signal magnitude of the LC circuit in response to change in the sensor coil induction; and(d) a processor for converting detected changes in the signal magnitude to surface conductivity data;wherein the material has a conductive surface and the sensor coil is maintained at a fixed distance from the conductive surface in order to determine a surface resistance measurement based on a shift in the signal magnitude, the shift in the signal magnitude being mapped to a set of known thin film resistance standards to yield the surface resistance measurement as an equivalent reading in Ω/sq. 25. The probe of claim 24, wherein the set of known thin film resistance standards is stored in the processor. 26. The probe of claim 24, wherein the probe has a surface resistance range of about 0.01Ω/sq to about 30Ω/sq. 27. The probe of claim 24, wherein the material is a non-magnetic conductive material. 28. The probe of claim 24, wherein the material is a ferromagnetic material. 29. A non-contact surface conductivity measurement probe for conductivity measurement of a material, the probe comprising:(a) an oscillator operating at a selected oscillator frequency;(b) a sensor comprising an LC circuit that is an integral part of the oscillator, the LC circuit including a sensor coil (L), inductance of the sensor coil being variable depending on conductivity of the material near the sensor coil;(c) a signal magnitude detector for detecting a change in the signal magnitude of the LC circuit in response to change in the sensor coil induction; and(d) a processor for converting detected changes in the signal magnitude to surface conductivity data;wherein a MagRAM coating is applied on top of the material and the conductivity measurement is used to determine a thickness of the MagRAM coating by using magnetic induction to measure dissipation of energy stored in the LC circuit. 30. The probe of claim 29, wherein the material has a non-conductive surface. 31. The probe of claim 29, wherein t he MagRAM coating is covered by a non-conductive paint coat. 32. A non-contact surface conductivity measurement probe for conductivity measurement of a material having a test surface, the probe comprising:(a) an oscillator operating at a selected oscillator frequency;(b) a sensor comprising an LC circuit that is an integral part of the oscillator, the LC circuit including a generally planar sensor coil (L), inductance of the sensor coil being variable depending on conductivity of the material near the sensor coil, the sensor coil being etched on a printed circuit (PC) board such that the sensor coil is maintained at a fixed distance from the test surface by the printed circuit board;(c) a frequency detector for detecting a change in the resonant frequency of the LC circuit in response to change in the sensor coil induction; and(d) a processor for converting detected changes in the resonant frequency to surface conductivity data. 33. The probe of claim 32 wherein the thickness of the PC board is a proximately 0.03 inch and having a blank surface that interfaces with the test surface. 34. The probe of claim 32 wherein the sensor coil is an 8-turn coil tuned to a resonant frequency of about 15 MHz. 35. The probe of claim 32 wherein the etched sensor coil is copper trace. 36. The probe of claim 32 wherein the etched sensor coil has an outer diameter of about 0.5 inch. 37. The probe of claim 32 wherein the etched sensor coil has a generally spiral configuration on the PC board. 38. The probe of claim 32, wherein the oscillator is a free running oscillator. 39. The probe of claim 38, wherein the free running oscillator is a Colpitts oscillator circuit. 40. The probe of claim 32, wherein the oscillator frequency is a radio frequency. 41. The probe of claim 40, wherein the oscillator frequency is about 21 MHz. 42. The probe of claim 32, wherein the sensor coil is maintained at a fixed distance from the test surface in order to determine a surface resistance measurement based on a shift in the resonant frequency. 43. The probe of claim 42, wherein the shift in the signal magnitude is mapped to a set of known thin film resistance standards to yield the surface resistance measurement as an equivalent reading in Ω/sq. 44. The probe of claim 43, wherein the set of known thin film resistance standards is stored in the processor. 45. The probe of claim 43, wherein the probe has a surface resistance range of about 0.01Ω/sq to about 30Ω/sq. 46. The probe of claim 43, wherein the material is a non-magnetic conductive material. 47. The probe of claim 43, wherein the material is a ferromagnetic material. 48. The probe of claim 32, further comprising a display device for displaying output representative of the conductivity measurement. 49. The probe of claim 32, wherein a MagRAM coating is applied on top of the material and the conductivity measurement is used to determine a thickness of the MagRAM coating by using magnetic induction to measure dissipation of energy stored in the LC circuit. 50. The probe of claim 49, wherein the material has a non-conductive surface. 51. The probe of claim 49, wherein the MagRAM coating covered by a non-conductive paint coat.