Beautiful! Thanks for posting these. Of particular importance is that you measured at the output of the speaker. Your plots demonstrate that the expected differences in the responses of the different transducers are are not washed out by any deficits in the transient responses of the stages in the signal chain. Rather, they are carried through to the speaker output.To illustrate drurb's points in message 29, shown below are wave forms of plucked open E and A double bass strings transduced by an Underwood piezo bridge pickup, an AT35 clip-on microphone pointing upward through the bridge legs, and a Radio Shack Clip-on microphone pointing into the G-side F-hole. I've added plucked E and A strings on a Fender P-Bass with a Quarter-Pounder magnetic pickup for further contrast. Each signal was amplified through a Walter Woods head connected to a 12-inch speaker cabinet and recorded via microphone placed in front the speaker.
Note the higher, sustained intensity in the latter halves of the pickup notes compared to the sharp decays from the microphones aimed at the table.
Underwood Piezo Pickup
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AT35 Clip-on Microphone
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Radio Shack Clip-On Microphone
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P-Bass Magnetic Pickup
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For anyone interested, I mentioned the temporal attack/decay profile in post #22 of this thread and referred to the Ehrlund thread where this discussion began over three years ago.
Thanks again for taking the time to make the recordings!