Here is a picture from a project I did a few years ago:
manybells.png
Might be from 2009 or 2010.
The measurements without "adams" in them were done by some very knowledgeable people for whom I have great respect. The measurements with "adams" were done using a reference grid and digital camera with a quite long optical zoom. I have a 9 page PDF describing the method, and PDF for printing off the grid. It involves using the GNU Image Manipulation Program (GIMP) to count pixels to get external bell measurements within a few thousandths of an inch, assuming very careful setup to avoid known sources of error.
It also involves characterizing the curve made by the bell flare. In "Fundamentals of Musical Acoustics" by A. H. Benade, section 20.5 covers "Musically Useful Shapes: The Flaring and Conical Families of Brasses." Within this section, Benade provide this equation:
D = B/(y+y0)m
which characterizes the diameter D of the bell flare at any distance y from the large end of the bell.
This equation is not easy to rearrange to solve for "m." Spreadsheets like LibreOffice Calc or programming languages make it possible to solve this by iteratively substituting different values for the other parameters until things match up. I have a worksheet for this. It is not fun to use. But given a relatively few points along a curve, it does a very nice job of providing a single, unique identifying parameter for the curve.
You will note I have not attached the either the PDFs or workbook to this post. I feel I have good reason for not doing so. If I read Benade correctly, these curves are very good at identifying the gross tonal differences between trumpets, horns, and trombones (for example.) They are not so good ON THEIR OWN for determining how a specific trombone will sound.
For example, the bright green trace for the Duo Gravis lies closer to the Stearn Fuchs than anything else. The Sandhagen 70h is MUCH further from the Stearn Fuchs. Yet I'm CERTAIN we could all hear clear differences between the Fuchs and the Duo Gravis. I'm willing to bet we would rank the Sandhagen 70h as being closer to the Fuchs than the Duo Gravis.
I pick this particular example because those two boundary shapes have tuning in the slide. This has a very significant impact on how far the taper of the bell reaches before any acoustic disturbances to the waveform. But this also introduces very significant sound modification in the mass and resonance of the main slide.
So my bottom line is this: it is easy to get all wrapped up in this one component of the system and still not get much closer to much of a sound characterization.
Most of the progress I've seen on this front is still pretty experimental. A member of "The Trombone Forum" did some remarkable work, touched on in this link:
https://www.science20.com/news_articles ... st_century
You can use Dr. Braden's name to find some other interesting work. You can alse search for this paper: "Acoustic pulse reflectometry for the measurement of musical wind instruments" by David Brian Sharp.
This paper might be closer to what you are interested in: "NON-LINEAR PROPAGATION CHARACTERISTICS IN THE EVOLUTION OF BRASS MUSICAL INSTRUMENT DESIGN" by Myers, Gilbert, Pyle, and Campbell.
For me the biggest selling point of the above two papers is that they deal with the entire instrument hardware system. These help explain why adding an in-line 2nd valve can make a horn sound and feel very different. Pulse reflectometry sounds exotic (at least to me.) But keep in mind that the same basic ideas are used to allow a cell phone to measure projectile velocities. If the demand arises it is only a matter of time before "good enough" consumer apps using low cost microphones and sound sources make it possible to do this at home.
BTW: on the bell measurement: the non-adams values were taken inside the bell. My measurements were taken outside, then adjusted for the average thickness of the bell. Of course, such adjustments are fraught with error sources. For one thing, there is not law of physics that says a piece of metal being spun on a mandrel will spin EXACTLY down onto the mandrel, or at the same thickness. For another, as the bell flares out, the added diameter of, say, .020" of metal runs into some interesting trigonometry and adds more and more than .020" to the outer diameter.
Good luck with your quest quantifying tonal characterization!
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