Well, here is the very basic idea.
A positive going pulse, current increase along x axis, target reaches saturation. Current decays to zero, however target magnetization does not return to it's starting point( let's call it zero, neglecting the earth field) but to a point which we call retentivity.
On the negative cycle, the current increases, but in opposite direction, saturating the target, now in the opposite direction, however this point of maximum saturation (optimal magnetivity) is not the inverse of the positive going saturation point.
That's because the starting point of magnetization for the negative going cycle is the previous point of retentivity after the positive going current returns to zero.
My assertion is that because both saturation points are not symmetrical, different metals will have different degrees of asymmetrical saturation points distinctive enough to be measured by dsp.
A positive going pulse, current increase along x axis, target reaches saturation. Current decays to zero, however target magnetization does not return to it's starting point( let's call it zero, neglecting the earth field) but to a point which we call retentivity.
On the negative cycle, the current increases, but in opposite direction, saturating the target, now in the opposite direction, however this point of maximum saturation (optimal magnetivity) is not the inverse of the positive going saturation point.
That's because the starting point of magnetization for the negative going cycle is the previous point of retentivity after the positive going current returns to zero.
My assertion is that because both saturation points are not symmetrical, different metals will have different degrees of asymmetrical saturation points distinctive enough to be measured by dsp.
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