I have carefully read Mr. Hartman's articles regarding the effects of Downbearing. The first installment was well put together and it is the kind of think we need to see more of. Mr. Hartman explained the principles involved in a clear and inventive way. He has taken care to use terms and concepts that are well defined and understood by a broad scientific community. Since these concepts are well known and can be referred to in countless in texts there is no need to reference anything. Speaking for myself, I fell confident that I can check any of his arguments by looking it up quite easily without any quoted reference on his part. However, at the end of the first installment he illustrates the typical modes of soundboard and the spectrum of a soundboard driven at two frequencies; these are not referenced. I am left to wonder; where did he get this information? It is complicated further by his second installment. He speaks of energy being shifted to lower modes by the stiffness provided by downbearing. This is contrary to everything I have ever understood about the subject. Does he have sources or is it pure speculation on his part. Has he performed some type of reproducible experiment that shows this. My own reasoning leads me to <believe> that a stiff bridge divides the board's modes up into smaller areas by acting as a surface node. It would be much like striking a string with your finger lightly touching a cross section of the string. This would restrict the string from vibrating for any wavelength that was both greater and not an integral length of the distance between a termination and the finger. My own understanding leads me to appreciate just how great is the Baldwin acujust hitch pin that allows one to to have uniform downbearing angles and limit it to a reasonable small angle. The next greatest thing one can do is design a string scale that has uniform tension. Uniform tension translates to uniform downbearing force from note to note if the down bearing angles are all the same. Finally, the idea that greater downbearing means more sustain is something that I have not been able to verify. I have a monochord with a twenty inch speaking length (C#3 at 160 lbs tension, I believe). This string is excited by a grand action model. A fixed weight is set on the key to provide a fixed velocity for the hammer to excite the string. One end of the monochord has an acujust hitch pin so that I can control the downbearing on the wooden bridge. The other termination of the string is a mounted agraffe. A transducer is attached that consists of a six inch copper strip. It measures the change in the electric field as caused by the moving of the string which is acts like the other side of a capacitor. This signal is captured by an Analog to Digital board in my computer and the software graphs the changing voltage over time. I took six samples each at a different downbearing angle. I could find no correlation between downbearing angle and the sustain, as you call it. Now to be rigorous it would be best to take maybe thirty scans of each downbearing angle and then average them and check for a correlation again. Perhaps I might try this in the future. Also, my monochord is mounted on an aluminum I beam not a piano soundboard. But, with this model I really am checking the sustain or the dampening of the string independent of the sound that is produced. In other words it is measuring the movement of the string and not the sound that is produced. If Mr. Hartman has references I would like to know them.
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