Iterative spectral integration algorithm: Difference between revisions
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Created page with "Spectral integration is an iterative procedure because the bandwidth required to estimate the variance of shear depends on the rate of dissipation, the level of electronic noi..." |
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\varepsilon = \frac{15}{2} \nu \int^{k_c}_{k_0} E^2(k) dk | \varepsilon = \frac{15}{2} \nu \int^{k_c}_{k_0} E^2(k) dk | ||
\end{equation} | \end{equation} | ||
</math> | </math> | ||
Revision as of 21:16, 20 August 2021
Spectral integration is an iterative procedure because the bandwidth required to estimate the variance of shear depends on the rate of dissipation, the level of electronic noise in the shear-probe signal, on the wavenumber of spurious signals that were not removed by the Goodman algorithm, and on the wavenumber resolution of the shear probe. The rate of dissipation is estimated using
[math]\displaystyle{ \begin{equation} \varepsilon = \frac{15}{2} \nu \int^{k_c}_{k_0} E^2(k) dk \end{equation} }[/math]
