Bob Jewett said:It is easy to get a gram or two of lead wire (or solder) and wrap it around the ferrule. No drilling required. It's a pretty interesting experiment. It is much less dramatic than the brass-filled shafts Jim Buss made to demo extreme squirt, though.
As for stiffness, and how it's involved, that's much harder to test. Theory says that if nothing else changed and the shaft were made stiffer, there would be more squirt because the stiffness is expected to increase the length of the shaft that participats in the sideways motion during contact. Unfortunately, I don't know of an easy way to change stiffness without changing anything else.
The current estimated length is about six inches which agrees generally with the speed of transverse waves (like a violin string) in the shaft and contact time, but I think we need a good mechanical engineer to fill in some of the details. I think the speed depends on the stiffness of the material, so if you had a stiffness knob to turn, a stiffer cue would give more squirt.
Hello Bob,
I think you were answering this post about the same time I was answering yours. I also think for clarity we should be talking about the same thing so I will henceforth speak in terms of the cueball instead of the cue (my natural point of interest) if I can accomplish it. I feel the cue ball is fixed and I cannot do much about it so i have considered the problem from the standpoint of cue.
I do find it interesting that you speak in terms of wavelength and pretty quickly thereafter in terms of stiffness increasing the length of the shaft that participates in the sideways motion. Aren't these terms for the same arguement...how much of the shaft is "in play"? Don't these terms somehow contradict? I'm assuming the same shaft with a different structure (that could be config of taper, size, bridge length or bridge type or in the extreme somethng as simple as firmness/location of grip...these would be easy ways to change stiffness). I don't think we are going to get anywhere if we don't think out of the box that has been created...that the cue is not part of a complex structure. I began this thread trying to break out of this constraint. Mr. sheldon's work is a solid beginning...let's expand the model to include a closer likeness to what's actually happening...so data from experimentation more closely approximates experience at the table. This is the crux of my question...I realise it may be somewhat more difficult to measure...but I think we can do it pretty quickly...and wouldn't there be a relevant range of stiffness as well? I actually believe that changing the structure of a shaft from a solid cylinder to a thin walled tube would likely increase the stiffness, as tubular structures are generally defined. I am assuming that the stiffness knob you speak of would work in reverse (as far as participating in sideways motion).
I have to go to work now and will return this afternoon to continue...thanks again.
Andy