Originally posted by Qiaozhi
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ok, so the GEB signal, no matter if target is ferrous or not-ferrous, will slide to left when nearing target to coil.
On the other side... when a ferrous item is neared the amplitude of DISC signal fall; when non-ferrous instead it will rise.
So you say, like in Gifford's patent I think, that you'll scale disc channel level in a way it will compensate the geb channel level increase by same but reversed in sign (decrease) action due to ferrous target, thus resulting in an opposition or subtraction when ferrous stuff, and instead sum when there's a non-ferrous target.
When non-ferrous the geb channel out increase will actually sum with the disc channel output increase to give a "boost" on actual detection behaviour, so this will increase also SNR in some way cause will be superimposition of two effects, geb increase and disc increase.
Am I right on this ?
So the principle is... I will disc sliding the disc sample in a way I will consider in-phase components give me maximum amplitude, so other angles that will make the maximum of wave slide left or right of the sample interval will give actually a discrimination like could happen with foil when you set disc in a way the shift due to foil will be not enough to center maximum peak of wave exactly in the middle of sample interval.
But that doesn't actually mean there's also a phase shift due to target ?
Another thing:
I mean... I always thought at quadrature demodulator like something truly acting 90° apart about pulses sequence but seems here you set geb with one control and disc with another... thus giving not exactly 90° shift from one another in the general case but just "about" 90°, sometimes e.g. 85° , sometimes maybe 95° or 100°.
So in TGS, formerly speaking there isn't any quadrature demodulator, apart the case when you fix samples exactly at 90° shift using geb and disc knobs: the only case where signals are really in "quadrature" to exactly 90°.
If all this is right why the hell we still call it quadrature-demodulator ???

Now another question: suppose you can measure absolute phase of RX signal at output of rx amplifier respect to tx signal (reference) with very hi accurancy.
Now suppose you will do that on air: you will read rx-tx phase shift due to coil only when in air and no target near.
Then suppose you lower the coil on soil and then measure again the phase shift: you'll sure will read a different value than before, due to ground effect.
Suppose then you will consider that ground reading your zero phase, like moving the needle of an old IB/VLF to the central zero: will you read any target signal phase variation as positive or negative then to the zero point ?
What I'm asking here... is... Is right if I assume 2 phase components effects from a target buried in soil (one due to soil only, and the other due to target only) that actually give you the composite effect on RX signal ?
I think it's so... and when we do GEB tuning on soil... we actually rotate the coordinate system to make the component due to soil only give no effects on the disc channel signal , cause its projection on it is zero, since the 2 channels have input at a real quadrature demodulator to are 90° truly shifted.
If so, zzy is right and we lose some GEB nulling when in TGS cause it has not always a quadrature-demodulator action.
Sorry for the long post... but I have this dubt also before... but don't wanna make people spend much time on details of TGS design or mistakes before they show up like in this case.
Kind regards,
Max
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