---------------------- multipart/alternative attachment Sarah, Now, thar ya' be goin' agin with all that there thinkin' and observin' and such....doncha know that's where all the trouble starts? Horace At 10:30 PM 8/21/2004, you wrote: >Hi all, > >Thanks for the advice about techniques to even out the SW curve! That >should give me a variety of techniques to use/combine in order to even out >the jags. > >But the question is one of what my target curve should *really* >be. Hmmmm.... My thoughts: > >The unmodified SW curve is obviously very linear. (Yes, I know what >linear means. I "minored" in mathematics, sort of -- except that my U. >didn't officially recognize minors). Stanwood's curves, OTOH, are all >concave downwards. > >I was advised off list that I shouldn't force the hammers to artificially >conform to a standardized Stanwood curve but to simply even out the jags >to make the action smooth from bottom to top. There's something to be >said for this idea. > >But as I got to thinking about the SW curves, I was wondering, where do >they REALLY come from? That is, where does the shape come from? I >suspect the hammer manufacturing people might be able to enlighten me as >to this. (Ray???) I'm *guessing* that the felt is denser than the >molding, and when the hammer becomes skinnier, it loses more felt than >molding, resulting in a more precipitous dropoff in weight at the higher >end. This would occur with a constant hammer length and a linear >variation in hammer and molding (and felt) width. Am I anywhere close on >this idea??? > >Contrast this function with other functions that might actually relate to >optimal hammer mass: String length and mass both decrease with the note >number, with a function that is concave upwards. Note frequency increases >with a function that is concave upwards. Note period (inverse of >frequency) increases with a function that is concave upwards. The >Stanwood curve seems rather meaningless with regard to any of these >functions. For instance, it might be good to match hammer mass to string >mass by some proportion. Right? As the scale goes up, string length and >mass approach an asymptote of zero. Therefore, shouldn't hammer mass >approach an asymptote of zero? Instead, the curve starts taking a dive in >the treble. If the scale went up well past 88, hammer mass would >eventually crash to zero. Because these curves do not have the same form, >the relationship between hammer and string mass is anything but >constant. That doesn't make sense. > >So is this something that is the way it is just because of tradition -- >because the cauls are built that way, and that's what ya' get? > >Now that I look at my linear SW curve (with jags), I'm wondering if this >isn't REALLY a closer match to something meaningful (like string mass) >than the idealized Stanwood curves. Any thoughts, y'all? > >Peace, >Sarah > > > ---------------------- multipart/alternative attachment An HTML attachment was scrubbed... URL: https://www.moypiano.com/ptg/pianotech.php/attachments/e7/7c/2d/e7/attachment.htm ---------------------- multipart/alternative attachment--
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