Originally posted by Mike Sulzer
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I believe we are talking about three things here.
1. The human ear is very sensitive to the initial transient of the string response as it gets translated by the (2) pickup and then the (3) amplifier/speaker.
2. The pickup must translate the initial string transient where the motion is the greatest and the full range of the string mechanical motion is captured and not attenuated by either the magnetic field limiting the most extreme string movement or pickup-related seen capacitance that reduces the slew rate. Slew rate - Wikipedia, the free encyclopedia
3. The amplifier and speaker must be able to fully capture the full range of the initial string transient and it's harmonics and reproduce it through the speaker.
See an excellent explaination by Ken Gilbert. slew rate explained | ken-gilbert.com See his explaination of capacitance on how it limits slew rate in general.
Here are some points to ponder. If one were to model a perfect string transient, what initial voltage would that peak string motion represent to capture the full movement of the initial attack? How do different pickup designs (magnetic field, inductance, capacitance) affect the transduction of the mechanical motion of the string? How much amplifier headroom is needed to fully capture the initial transient and not affect the subtle audible aspects of the initial transient. The answers to these questions will begin to answer the relationship of these variables to what we hear.
Joseph Rogowski
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