Hi Ed, others. I do not dispute that in a real world piano there is coupling. Obviously both the front and back terminations are not infinitely stiff in real life. I am trying to get at whether there is a connection between the degree of bridge stiffness and the degree of coupling. And whether this connection manifests itself in any way in the amount or degree of pitch drop that results from oscillating strings sharing a common support. This has several implications actually. One is that since coupling actually DOES occur in real life pianos, the bridge itself by definition becomes an integral part of the strings termination at the bridge and refutes the postulate that it is the bridge pin and the bridge pin alone that terminates the string at the bridge. One way or the other.... if there is interaction between the strings, then there must be a common support/termination for the interaction to take place. Another implication is that it may be possible to diagnose stiffness conditions by the degree of coupling observed. If this is true, then it no doubt would be a handy tool to have at hand. Given what we already know about termination stiffness and sustain characteristics, I would not be surprised about the Sauter you mention. Cheers RicB If you can hear the string, it's fair to assume the soundboard is moving at frequencies similar to some of those in the string, therefore it's reasonable to assume that the bridge is also moving. Thus it is also likely that when frequencies are very close, coupling will occur. The amplitude of the wave in the string will play a role as well. Perhaps when it becomes too small to move the bridge, the strings de-couple, at least at that particular partial. This may not involve all the partials of the unison at all times. For example, in the higher octaves the first partial may become inaudible almost immediately. The Sauter concert grand with titanium armor in the top octaves is remarkable for the clarity and sustain of the first partials in octaves 6 and 7. Ed S.
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