I'm submitting this idea for comments. Perhaps the most knowledgeable would care to point to any misconceptions.
System structure:
Free running LC oscillator -> Peak detector -> Amplifier -> Output A (amplitude signal)
. . . . . . . . . . . . . .-> Frequency to Voltage conversion (PLL) -> Output F (frequency signal)
Even without a target, a change in the frequency of the LC tank also translates into a change in the oscillator's amplitude. This is due to the oscillator's characteristics.
Therefore the amplitude signal is a combination of two factors:
1. The resistive component of the taget (R)
2. The frequency deviation caused by the target.
The system can be calibrated to eliminate the 2nd factor by using a purely magnetic target (a ferrite), this way the relationship frequency/amplitude can be established (brown line in the graph).
Similarly, a diamagnetic good conductor (pure Ag) is used to calibrate the other extreme of the frequency deviations (green line).
We now got two linearly independent vectors, though not orthogonal, and any target falls in between.
In order to separate the two components of the amplitude we need to convert the R and F signals to an orthogonal coordinate system where the x-axis is only affected by frequency and the y-axis is only affected by resistivity. This can readily be done using Algebra, in particular a change of basis, once the two vectors above are known. In the new basis the X and Y components would be equivalent to those produced by an IB system.
Any weak points in my reasoning?
System structure:
Free running LC oscillator -> Peak detector -> Amplifier -> Output A (amplitude signal)
. . . . . . . . . . . . . .-> Frequency to Voltage conversion (PLL) -> Output F (frequency signal)
Even without a target, a change in the frequency of the LC tank also translates into a change in the oscillator's amplitude. This is due to the oscillator's characteristics.
Therefore the amplitude signal is a combination of two factors:
1. The resistive component of the taget (R)
2. The frequency deviation caused by the target.
The system can be calibrated to eliminate the 2nd factor by using a purely magnetic target (a ferrite), this way the relationship frequency/amplitude can be established (brown line in the graph).
Similarly, a diamagnetic good conductor (pure Ag) is used to calibrate the other extreme of the frequency deviations (green line).
We now got two linearly independent vectors, though not orthogonal, and any target falls in between.
In order to separate the two components of the amplitude we need to convert the R and F signals to an orthogonal coordinate system where the x-axis is only affected by frequency and the y-axis is only affected by resistivity. This can readily be done using Algebra, in particular a change of basis, once the two vectors above are known. In the new basis the X and Y components would be equivalent to those produced by an IB system.
Any weak points in my reasoning?
Comment