Continuing with the analysis from before the interruption
To get back to analyzing what happens when two pickups are combined passively in parallel, and then buffered, as opposed to individual buffering followed by addition, this is from my earlier post (slightly edited).
The result is that the voltage of each pickup, used alone, is attenuated by a factor of two at the point where they are paralleled, independent of frequency.
Now we want to see what happens when both pickups are on at once. For this we need the superposition theorem: The response to several independent sources is the sum of the responses to each independent source with the remaining independent sources dead. (Close, The Analysis of Linear Circuits) A dead voltage source is one which has been replaced by a short circuit. Note that this theorem is first derived for dc, but then later extended to ac. We apply it for a sine wave of each frequency, making sure to account of the phases of the signals.
The text in the quote above shows that the responses to be added are just that of the pickups themselves divided by two, independent of frequency. So that is what we get when we buffer after putting the pickups in parallel.
If we buffer each pickup first, and then add with a pair of resistors, we get the same thing. So the frequency response is the same whether we buffer before or after combining. In neither case is the frequency response of the pickups altered.
If you combine pickups without buffering and connect to a cable, there is a change in the frequency response as described earlier.
To get back to analyzing what happens when two pickups are combined passively in parallel, and then buffered, as opposed to individual buffering followed by addition, this is from my earlier post (slightly edited).
So consider a pickup model composed of a voltage source in series with an inductor (which can have a resistor in series if we like) and a capacitor in parallel with the series combination. We put two of these in parallel. For simplicity, detach the capacitors; we will put them back in later after combining the inductors.
Consider one pickup at a time. This means that we short out the voltage source of the inactive one. Now we have a voltage divider consisting of two identical inductors (maybe with resistors in series, but still both are the same). This means that the voltage at the output is half that of the voltage source. This holds true at all frequencies; so if the source varies as a function of frequency, this variation is preserved. If we short out both sources and look back into the network, we have two inductors in parallel which is equivalent to a single inductor of half the value. So the Thevenin equivalent is a voltage source of half the original source and an inductor of half the value of the original. Now we can put the capacitors back in. Note that two capacitors in parallel have half the impedance of a single one, and so the frequency response is preserved. That is, the product of L and C stays the same because the L is halved, and the C is doubled.
Consider one pickup at a time. This means that we short out the voltage source of the inactive one. Now we have a voltage divider consisting of two identical inductors (maybe with resistors in series, but still both are the same). This means that the voltage at the output is half that of the voltage source. This holds true at all frequencies; so if the source varies as a function of frequency, this variation is preserved. If we short out both sources and look back into the network, we have two inductors in parallel which is equivalent to a single inductor of half the value. So the Thevenin equivalent is a voltage source of half the original source and an inductor of half the value of the original. Now we can put the capacitors back in. Note that two capacitors in parallel have half the impedance of a single one, and so the frequency response is preserved. That is, the product of L and C stays the same because the L is halved, and the C is doubled.
Now we want to see what happens when both pickups are on at once. For this we need the superposition theorem: The response to several independent sources is the sum of the responses to each independent source with the remaining independent sources dead. (Close, The Analysis of Linear Circuits) A dead voltage source is one which has been replaced by a short circuit. Note that this theorem is first derived for dc, but then later extended to ac. We apply it for a sine wave of each frequency, making sure to account of the phases of the signals.
The text in the quote above shows that the responses to be added are just that of the pickups themselves divided by two, independent of frequency. So that is what we get when we buffer after putting the pickups in parallel.
If we buffer each pickup first, and then add with a pair of resistors, we get the same thing. So the frequency response is the same whether we buffer before or after combining. In neither case is the frequency response of the pickups altered.
If you combine pickups without buffering and connect to a cable, there is a change in the frequency response as described earlier.
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