Method and apparatus for testing conductivity using eddy currents

Claim 2

In the method of measuring conductivity of nonferrous metals which includes the steps of providing a periodic signal in proximity to a conductive non-ferrous test piece to induce eddy currents therein and developing a test signal which varies as a function of said eddy currents, the improvement comprising the steps of providing a first reference signal related in phase to said periodic signal said periodic signal, said reference signal and said test signal all being at the same frequency, measuring the period of one specific test frequency at which said test signal is at a predetermined phase relationship with respect to said reference signal and determining conductivity of said non-ferrous test piece as a direct linear function of said measured period at said one specific test frequency.

Claim 3

The method set forth in claim 1 wherein the step of measuring the period of said test frequency comprises the steps of dividing said test frequency by twice a preselected scaling factor to provide a scaled output signal, providing a second periodic signal and counting periods of said second signal during a half cycle of said scaled output signal, the count during said half cycle being equal to said scaling factor multiplied by the ratio of the frequency of said second signal divided by said test frequency.

Claim 4

The method set forth in claim 2 wherein said count is scaled to a percentage of a predetermined standard conductance at a selected test frequency.

Claim 5

The method set forth in claim 3 comprising the further step of displaying said count after each said half cycle of said scaled output signal.

Claim 8

The method set forth in claim 5 wherein eddy currents are induced in a second nonferrous test material by means of said coil carrying said periodic signal, a second field developed by eddy currents in said second test material is sensed to provide a second test signal which varies as a function of conductivity of said second nonferrous material, said second test signal is integrated to provide a second integrated signal, said second integrated signal is compared to said reference signal to provide a second difference signal which varies as a function of the phase difference between said second integrated signal and said reference signal, the frequency of said periodic signal is adjusted to a second frequency at which said reference signal and said second integrated signal have the same said preselected phase difference therebetween, and then conductivity of said second nonferrous material is determined as the same said inverse linear function of test frequency at said corresponding second frequency.

Claim 9

In the method of determining conductivity of test materials which includes the steps of providing a periodic signal to electromagnetically induce eddy currents in a first test material and developing a test signal which varies as a function of said eddy currents, the improvement comprising the steps of developing a reference signal as a preselected function of said periodic signal, said periodic signal, said test signal and said reference signal all being at a same test frequency, determining a relationship in phase between said test signal and said reference signal, varying said test frequency until said test frequency is at a first value at which said phase relationship is at a preselected value, and then determining conductivity of said first test material as an inverse linear function of said first value of said test frequency.

Claim 10

In the method of determining conductivity of test materials which includes the steps of providing a periodic signal to electromagnetically induce eddy currents in a first test material and developing a test signal which varies as a function of said eddy currents, the improvement comprising the steps of developing a reference signal as a preselected function of said periodic signal, said periodic signal, said test signal and said reference signal all being at a same test frequency, determining a relationship in phase between said test signal and said reference signal, varying said test frequency until said test frequency is at a first value at which said phase relationship is at a preselected value, and then determining conductivity of said first test material as an inverse linear function of said first value of said test frequency.

Claim 11

The method set forth in claim 7 wherein said periodic signal induces second eddy currents in a second test material and a second test signal which varies as a function of said second eddy currents is developed, and further comprising the steps of determining a second relationship in phase between said second test signal and said reference signal, varying said test frequency until said test frequency is at a second value at which said second phase relationship reaches the same said preselected value and then determining conductivity of said second test material as the same said inverse linear function of test frequency at the said corresponding second value of said test frequency.

Claim 12

The method set forth in claim 8 for determining conductivity of test materials having a predetermined minimum thickness, said test frequency being of sufficient magnitude that said induced eddy currents are substantially unrelated to material thickness.

Claim 13

The method set forth in claim 9 wherein said periodic signal is also said reference signal.

Claim 14

The method set forth in claim 7 wherein said step of determining said material conductivity comprises the steps of measuring the period of said periodic signal and displaying said measured period as a direct scaled function of said conductivity.

Claim 15

The method set forth in claim 11 wherein conductivity is displayed as a scaled percentage of a predetermined standard conductivity.

Claim 16

The method set forth in claim 7 wherein the step of determining said phase relationship comprises the steps of integrating said test signal and comparing said integrated test signal to said reference signal to develop a signal which varies as a function of a measured phase relationship therebetween.

Claim 17

The method set forth in claim 7 wherein said conductivity as so determined is digitally displayed as a direct linear function of the period of said one signal.

Claim 20

The method set forth in claim 15 wherein conductivity is measured as a direct linear function of the period of said test frequency at one specific test frequency at which said test signal is at said predetermined relationship with respect to said reference signal.

Claim 21

Apparatus for measuring a characteristic of a test material comprising means providing a periodic signal including means adapted to be positioned on one side of a test material to induce eddy currents in the material, sensing means adapted to be positioned on the same said side of the test material for developing a test signal in response to said eddy currents in the material, means responsive to said periodic signal to provide a reference signal, said periodic signal, said test signal and said reference signal all being at a test frequency selected such that eddy currents induced in the test material are substantially unrelated to material thickness, means responsive to said reference signal and said test signal to provide an output according to the phase angle differential between said test signal and said reference signal, means for varying said test frequency until said test frequency is at a preselected value, and means for determining a value of said characteristic of said material as a function of said first value of said test frequency.

Claim 22

Apparatus for measuring a characteristic of a test material comprising means providing a periodic signal including means adapted to be positioned on one side of a test material to induce eddy currents in the material, sensing means adapted to be positioned on the same said side of the test material for developing a test signal in response to said eddy currents in the material, means responsive to said periodic signal to provide a reference signal, said periodic signal, said test signal and said reference signal all being at a test frequency selected such that eddy currents induced in the test material are substantially unrelated to material thickness, means responsive to said reference signal and said test signal to provide an output according to the phase angle differential between said test signal and said reference signal, means for varying said test frequency until said test frequency is at a preselected value, and means for determining a value of said characteristic of said material as a function of said first value of said test frequency.

Claim 23

The apparatus set forth in claim 17 wherein said frequency varying means comprises means for varying the frequency of said periodic signal.

Claim 24

The apparatus set forth in claim 18 wherein said determining means comprises means measuring the period of said test frequency and means displaying said measured period as a direct scaled parameter of said characteristic.

Claim 25

The apparatus set forth in claim 19 wherein said means providing said phase differential output comprises means for integrating said test signal and means for comparing said integrated test signal to said reference signal to develop said phase differential output.

Claim 26

The apparatus set forth in claim 20 wherein said phase differential output is a direct current test signal and wherein said apparatus further comprises means providing a direct current reference representing said predetermined value of said phase differential output and means comparing said direct current test signal to said direct current reference to determine said first value of said signal parameter.

Claim 27

The apparatus set forth in claim 20 wherein said material characteristic is conductivity of a nonferrous metal and wherein said display means is calibrated to display conductivity in percent IACS.

Claim 28

The apparatus set forth in claim 19 wherein said means for measuring the period of said test frequency comprises means for dividing said test frequency by twice a preselected scaling factor to provide a scaled output signal, means for providing a second periodic signal and means for counting periods of said second periodic signal during a half cycle of said scaled output signal, the count during said half cycle being equal to said scaling factor multiplied by the ratio of the frequency of said second periodic signal divided by said test frequency.

Claim 29

Apparatus for measuring conductivity of a test material comprising means providing a periodic signal, means responsive to said periodic test signal to electromagnetically induce eddy currents in said test material, sensing means responsive to said eddy currents to develop a test signal as a function of said eddy currents, means for measuring the phase relationship between said periodic signal and said test signal, means for varying the frequency of said periodic signal until said phase relationship reaches a preselected specific level, means responsive to the period of said periodic signal to determine conductivity of the material as a direct linear function of said period when said phase relationship reaches said preselected level.

Claim 30

Apparatus for measuring conductivity of a test material comprising means providing a periodic signal, means responsive to said periodic test signal to electromagnetically induce eddy currents in said test material, sensing means responsive to said eddy currents to develop a test signal as a function of said eddy currents, means for measuring the phase relationship between said periodic signal and said test signal, means for varying the frequency of said periodic signal until said phase relationship reaches a preselected specific level, means responsive to the period of said periodic signal to determine conductivity of the material as a direct linear function of said period when said phase relationship reaches said preselected level.

Claim 31

The apparatus set forth in claim 24 wherein said sensing means includes a plurality of coils so arranged and disposed with respect to said eddy current inducing means and said material to develop said test signal independently of effects thereon caused by said periodic signal directly.

Claim 32

The apparatus set forth in claim 24 wherein said phase relationship measuring means comprises means connected to said eddy current sensing means to electronically integrate said test signal and phase detector means for comparing said integrated test signal to said periodic signal to develop a phase differential signal proportional to the phase angle between said integrated test signal and said periodic signal.

Claim 33

The apparatus set forth in claim 26 wherein said frequency varying means comprises a voltage controlled oscillator providing said periodic signal at a frequency controlled by said differential signal.

Claim 34

The apparatus set forth in claim 24 wherein said period responsive means comprises a frequency divider for dividing the frequency of said periodic signal by twice a preselected scaling factor, a reference oscillator providing a second periodic signal at preselected frequency, a counter, and means gating said second periodic signal to said counter during a half cycle of said frequency-divided periodic signal, whereby said counter counts periods of said second periodic signal for the duration of said half cycle.

Claim 35

The apparatus set forth in claim 28 further comprising means displaying the count in said counter after each said half cycle of said frequency-divided periodic signal.

Claim 36

The apparatus set forth in claim 29 wherein said display means comprises a digital display.

Claim 37

The apparatus set forth in claim 29 wherein said display is calibrated in percentage of a predetermined standard conductivity.

Claim 38

The apparatus set forth in claim 31 wherein said percentage is proportional to said scaling factor multiplied by the ratio of said preselected reference oscillator frequency divided by said frequency of said periodic signal.