Free-free bar: Difference between revisions

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Created page with "A '''free-free bar''' is an idealized bar that is completely free to vibrate at both ends without external constraints.<ref>http://www.hopestreetmarimba.com/a-driftwood-marimba-on-the-beach-of-improbability/</ref> A marimba or xylophone bar can be modeled by this. Free-free bars are highly inharmonic, and their vibration is governed by a complex differential equation which can be solved to determine the spectrum of a free bar <ref>https://web.archive..."
 
Correct math; improve reference display
 
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A '''free-free bar''' is an idealized bar that is completely free to vibrate at both ends without external constraints.<ref>http://www.hopestreetmarimba.com/a-driftwood-marimba-on-the-beach-of-improbability/</ref> A marimba or xylophone bar can be modeled by this. Free-free bars are highly [[harmonic timbre|inharmonic]], and their vibration is governed by a complex differential equation which can be solved to determine the spectrum of a free bar <ref>https://web.archive.org/web/20260816073448/http://www.varg.unsw.edu.au/Assets/link%20pdfs/Beam_vibration.pdf</ref>. The nth [[overtone]] of a free bar can be approximately represented by the formula below <ref>https://web.archive.org/web/20260212000442/http://hyperphysics.phy-astr.gsu.edu/hbase/Music/barres.html</ref>
A '''free-free bar''' is an idealized bar that is completely free to vibrate at both ends without external constraints.<ref>[http://www.hopestreetmarimba.com/a-driftwood-marimba-on-the-beach-of-improbability/ Hope Street Marimba | ''A driftwood marimba on the Beach of Improbability'']</ref> A [[marimba]] or [[xylophone]] bar can be modeled by this. Free-free bars are highly [[harmonic timbre|inharmonic]], and their vibration is governed by a complex differential equation which can be solved to determine the spectrum of a free bar.<ref>[https://web.archive.org/web/20260816073448/http://www.varg.unsw.edu.au/Assets/link%20pdfs/Beam_vibration.pdf Mauro Caresta. ''Vibrations of a Free-Free Beam''. ]</ref> The ''n''-th [[overtone]] of a free bar can be approximately represented by the formula below.<ref>[https://web.archive.org/web/20260212000442/http://hyperphysics.phy-astr.gsu.edu/hbase/Music/barres.html HyperPhysics | ''Bar Resonances'']</ref>
<math>f_n=0.441[n+1\frac{1}{2}]^2f_1</math>
 
where <math>f_1</math> is the fundamental frequency.
<math display="block">f_n = 0.441 \left( n + \frac{1}{2} \right) ^2 f_1</math>
 
where ''f''<sub>1</sub> is the fundamental frequency.


== See also ==
== See also ==
* [[Freave]]  
* [[Freave]]  
== References ==
== References ==
<references />
<references />
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[[Category:Instruments]]
[[Category:Instruments]]
[[Category:Math]]
[[Category:Math]]
[[Category:Xenharmonic series]]
[[Category:Xenharmonic series]]
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Latest revision as of 11:57, 23 October 2026

A free-free bar is an idealized bar that is completely free to vibrate at both ends without external constraints.[1] A marimba or xylophone bar can be modeled by this. Free-free bars are highly inharmonic, and their vibration is governed by a complex differential equation which can be solved to determine the spectrum of a free bar.[2] The n-th overtone of a free bar can be approximately represented by the formula below.[3]

\begin{displaymjx}f_n = 0.441 \left( n + \frac{1}{2} \right) ^2 f_1\end{displaymjx}

where f1 is the fundamental frequency.

See also

References


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