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Just signed up to see if I could obtain any guidance on this topic. I'll start with some background.
As a guitarist, I exist within a set group that, by and large, is in love with 1958 - the Gibson Les Paul, Fender Stratocaster, and some other influential late 50's and 60's instrument designs all but completely speak for the design of the modern instrument, despite massive backlash against this by makers such as auerswald, steinberger, rick toone, etc.
The argument on tone, sustain, playability, attack, decay, tuning stability, etc, covers a very complex set of variables, but I'm interested in one set of controversies in particular - what, if anything, increases the sustain (length of time of vibration) of a plucked string, in the absence of an outside source of energy to drive the string into further motion? Is the hypothetical perfect sustain as simple as "A string immovably fixed between two infinitely hard, infinitely strong, infinitely heavy objects, will sustain longest?", or are there other elements to consider?
My laymans understanding is this:
1 - Once a string is struck with the plectrum, it has a set amount of kinetic and potential energy from being deformed and being in motion. Short of striking it again, subjecting it to electromagnetism, or driving it with high volume feedback, this energy will slowly dissipate into the air and the surrounding structures of the instrument until it is completely gone and the string is silent.
2 - This being the case, the most effective way of increasing the natural sustain of an instrument would be to limit the ways in which the energy can be lost. This could be done by:
So taking my current understanding into account - What would be the ideal scenario here?
[1] https://altguitars.files.wordpress.com/2011/09/locking-nut.jpg
[2] http://www.stewmac.com/tradesecrets/newsletter/ts0061/ts0061e.jpg
[3] http://www.lutherie.net/fret.samples..jpg
[4] http://www.glguitars.com/features/images/saddle-lock-bridge-large.gif
[5] http://www.stewmac.com/product/imag...gsby_B70_Vibrato_Chrome_Polished_aluminum.jpg
[6] http://www.guitarplayersanonymous.org/images/customer-images//81EpiphoneSheratonAngle014.jpg
As a guitarist, I exist within a set group that, by and large, is in love with 1958 - the Gibson Les Paul, Fender Stratocaster, and some other influential late 50's and 60's instrument designs all but completely speak for the design of the modern instrument, despite massive backlash against this by makers such as auerswald, steinberger, rick toone, etc.
The argument on tone, sustain, playability, attack, decay, tuning stability, etc, covers a very complex set of variables, but I'm interested in one set of controversies in particular - what, if anything, increases the sustain (length of time of vibration) of a plucked string, in the absence of an outside source of energy to drive the string into further motion? Is the hypothetical perfect sustain as simple as "A string immovably fixed between two infinitely hard, infinitely strong, infinitely heavy objects, will sustain longest?", or are there other elements to consider?
My laymans understanding is this:
1 - Once a string is struck with the plectrum, it has a set amount of kinetic and potential energy from being deformed and being in motion. Short of striking it again, subjecting it to electromagnetism, or driving it with high volume feedback, this energy will slowly dissipate into the air and the surrounding structures of the instrument until it is completely gone and the string is silent.
2 - This being the case, the most effective way of increasing the natural sustain of an instrument would be to limit the ways in which the energy can be lost. This could be done by:
- Making the anchor points and contact points stronger, in conjunction with...
- Making the mass at the anchor points greater, so that the relatively small amount of energy in the string would be insufficient to start the greater mass into motion
- Using a more homogenous material such as steel or tungsten, providing both of the above and also removing points of weakness in the structure that could vibrate and lose energy in a material of variable density like wood.
- Making the contact areas of the string with the body smaller, such as using a locking nut[1] with screws instead of using many wraps of string around the tuners[2], using taller, thinner frets[3], and using a simple, strong, locking bridge/saddle[4] arrangement rather than something more involved such as a bigsby[5] or trapeze tailpiece[6]
- Minimizing the amount of string that exists outside of the vibrating length, so that there can be less sympathetic vibrations generated outside the useful area.
So taking my current understanding into account - What would be the ideal scenario here?
[1] https://altguitars.files.wordpress.com/2011/09/locking-nut.jpg
[2] http://www.stewmac.com/tradesecrets/newsletter/ts0061/ts0061e.jpg
[3] http://www.lutherie.net/fret.samples..jpg
[4] http://www.glguitars.com/features/images/saddle-lock-bridge-large.gif
[5] http://www.stewmac.com/product/imag...gsby_B70_Vibrato_Chrome_Polished_aluminum.jpg
[6] http://www.guitarplayersanonymous.org/images/customer-images//81EpiphoneSheratonAngle014.jpg