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The reason
for connecting the load resistor to the shallot of the reed instead of to
the pickup is as follows. Have you ever noticed how in your home stereo system,
for example, you have just two wires going to either speaker? And yet, in
spite of that, all of the extremely complex audio information of, for instance,
an entire symphony orchestra is all represented by a single AC audio waveform
that requires only two wires. Along the same principle, Wurlitzer found that
they could "common" or tie together, all of the reed shallots and
then just have one common load resistor and one blocking capacitor, and no
matter how many notes the musician might use at any instance, and no matter
whether he's using one, two, or all three pickups, the resulting multitude
of individual notes and tones can all be combined into one single AC audio
waveform that represents all of them. This of course makes the circuitry much
simpler than if they had to use individual load resistors and blocking capacitors
for every single pickup on each reed individually. |
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Left. The waveform from a pickup over the front of a reed shows some appreciable low-order harmonic development, the second har-monic being quite prominent and also the third. These harmonics are not exactly in phase. This shows that the motion of the front edge of the reed is not sinusoidal but undergoes changes in instantaneous velocity. |
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Right, the waveform from a pickup over the center of a reed shows a somewhat similar shape but with considerably less harmonic development. The waveform above and this one clearly demonstrate that the motion of the reed becomes considerably more non sinu-soidal as we get closer to the front end. |
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Left. This waveform, and the one directly below are from the front edge sheet metal pickups on two different reeds. Although the waveforms are similar, they are slightly different even though both show sharp spikes indi-cating the presence of lots of high harmonics. The reason for the difference is due to slight positional differences of the sheet metal pickups relative to the reeds and their arcs of vib-ration. Tolerances are so close here that it is impossible to get everything exactly the same. The two waveforms sound identical during normal playing, but careful listening will reveal slight differences. Interestingly, these differences vary from one ins-trument to another and serve as a kind of electronic fingerprint for every instrument of this type.
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