From 2c28c25d952dd1bd790c645e92ca6a1900243780 Mon Sep 17 00:00:00 2001 From: "W. Trevor King" Date: Sun, 5 May 2013 14:36:33 -0400 Subject: [PATCH] calibcant/discussion.tex: Cleanup peak-frequency discussion Add $f_\text{max}$ for clarity, and link to this equation from the vibration figure. --- src/calibcant/discussion.tex | 20 ++++++++++++-------- src/calibcant/procedure.tex | 10 ++++++---- 2 files changed, 18 insertions(+), 12 deletions(-) diff --git a/src/calibcant/discussion.tex b/src/calibcant/discussion.tex index 9173778..62d60b3 100644 --- a/src/calibcant/discussion.tex +++ b/src/calibcant/discussion.tex @@ -49,17 +49,21 @@ $\PSD_f$ in \cref{eq:model-psd-df}, it's useful to also calculate the frequency of the resonant peak. \begin{align} 0 &= \deriv{f}{\PSD_f} - = \frac{2G_{1f}f}{\p({(f_0^2-f^2)^2 + \beta_f^2 f^2})^2} - \p({2(f_0^2-f^2) - \beta_f^2}) - = 2(f_0^2-f^2) - \beta_f^2 \\ - f^2 &= f_0^2 - \frac{\beta_f^2}{2} \\ - f &= \sqrt{f_0^2 - \frac{\beta_f^2}{2}} \;, + = \frac{2G_{1f}f_\text{max}} + {\p({(f_0^2-f_\text{max}^2)^2 + \beta_f^2 f_\text{max}^2})^2} + \p({2(f_0^2-f_\text{max}^2) - \beta_f^2}) + = 2(f_0^2-f_\text{max}^2) - \beta_f^2 \\ + f_\text{max}^2 &= f_0^2 - \frac{\beta_f^2}{2} \\ + f_\text{max} &= \sqrt{f_0^2 - \frac{\beta_f^2}{2}} \;, \label{eq:peak-frequency} \end{align} where we used $f\ne0$ during the large simplifying multiplication. We -see that the peak frequency is actually shifed from $f_0$ depending on -the damping term $\beta_f$. For overdamped cantilevers with large -values of $\beta$, the peak frequency will not have a real solution. +see that the peak frequency is shifted from $f_0$ depending on the +damping term $\beta_f$. For overdamped cantilevers with large values +of $\beta$, the peak frequency will not have a real solution.% +% +\nomenclature{$f_\text{max}$}{The frequency of the peak power in + $\PSD_f$ (\cref{eq:eq:peak-frequency}).} \subsection{Propogation of errors} \label{sec:calibcant:discussion:errors} diff --git a/src/calibcant/procedure.tex b/src/calibcant/procedure.tex index cd012ec..e09a7fe 100644 --- a/src/calibcant/procedure.tex +++ b/src/calibcant/procedure.tex @@ -133,10 +133,12 @@ vibrations are configurable (with \hFconfig, panel shows the $\PSD_f(V_p,f)$ with a fit following \cref{eq:psd-Vp-offset}. The constant offset $P_{0f}$, drawn as the horizontal line in the third panel, accounts for white noise - in the measurement circuit. Only data in the blue region was - used when computing the best fit. This is the first vibration - from the 2013-02-07T08-20-46 calibration, yielding a fitted - variance $\avg{V_p(t)^2}=96.90\pm0.99\U{mV$^2$}$. + in the measurement circuit. The vertical line marks the peak + frequency $f_\text{max}$ (\cref{eq:peak-frequency}). Only data + in the blue region was used when computing the best fit. This + is the first vibration from the 2013-02-07T08-20-46 calibration, + yielding a fitted variance + $\avg{V_p(t)^2}=96.90\pm0.99\U{mV$^2$}$. \label{fig:calibcant:vibration}} \end{center} \end{figure} -- 2.26.2