Tenney–Euclidean temperament measures: Difference between revisions

Mike Battaglia (talk | contribs)
Span -> interval span
TE error: spell out the tuning map in terms of V
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is an '''adjusted error''' which makes the error of a rank ''r'' temperament correspond to the errors of the edo vals which support it; so that requiring the edo val error to be less than (1 + ε)ψ for any positive ε results in an infinite set of vals supporting the temperament.  
is an '''adjusted error''' which makes the error of a rank ''r'' temperament correspond to the errors of the edo vals which support it; so that requiring the edo val error to be less than (1 + ε)ψ for any positive ε results in an infinite set of vals supporting the temperament.  


By Graham Breed's definition, TE error may be accessed directly via [[Tenney-Euclidean Tuning|TE tuning map]]. If T is the tuning map, then the TE error G can be found by
By Graham Breed's definition, TE error may be accessed via [[Tenney-Euclidean Tuning|TE tuning map]]. If T is the tuning map, then the TE error G can be found by


<math>\displaystyle
<math>\displaystyle
G = \lVert T - J \rVert_\text{RMS} = \sqrt{\frac{(T - J) \cdot (T - J)^\mathsf{T}}{n}}</math>
\begin{align}
G &= \lVert T - J \rVert_\text{RMS} \\
&= \lVert J(V^+V - I) \rVert_\text{RMS} \\
&= \sqrt{J(V^+V - I)(V^+V - I)^\mathsf{T}J^\mathsf{T}/n}
\end{align}
</math>


where the dot represents the ordinary dot product. If T is denominated in cents, then J should be also, so that J = {{val|1200 1200 … 1200}}. Here T - J is the list of weighted mistunings of each prime harmonics. Note: this is the definition used by the temperament finder.  
where the dot represents the ordinary dot product. If T is denominated in cents, then J should be also, so that J = {{val|1200 1200 … 1200}}. Here T - J is the list of weighted mistunings of each prime harmonics. Note: this is the definition used by the temperament finder.  
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<math>\displaystyle G = \sqrt{\frac{n-1}{2n}} \psi = \sqrt{\frac{n-r}{(r+1)n}} \Psi</math>
<math>\displaystyle G = \sqrt{\frac{n-1}{2n}} \psi = \sqrt{\frac{n-r}{(r+1)n}} \Psi</math>


G and ψ error both have the advantage that higher rank temperament error corresponds directly to rank one error, but the RMS normalization has the further advantage that in the rank one case,  G = sin θ, where θ is the angle between J and the val in question. Multiplying by 1200 to obtain a result in cents leads to 1200 sin θ, TE error as it appears on the temperament finder pages.  
G and ψ error both have the advantage that higher rank temperament error corresponds directly to rank one error, but the RMS normalization has the further advantage that in the rank one case,  G = sin θ, where θ is the angle between J and the val in question. Multiplying by 1200 to obtain a result in cents leads to 1200 sin θ, TE error as it appears on the temperament finder pages.


== Examples of each definition ==
== Examples of each definition ==