diff options
| author | Blaise Thompson <blaise@untzag.com> | 2018-04-16 13:32:20 -0500 |
|---|---|---|
| committer | Blaise Thompson <blaise@untzag.com> | 2018-04-16 13:32:20 -0500 |
| commit | 798bd484137439bf1d0752ddde82bf49da4af6b7 (patch) | |
| tree | 030e73d1844a3d98226da55170af15ade862b584 /quantitative_ta | |
| parent | 6579cbe6381ee4bb805a6d5b5cc5fbd249daa9f2 (diff) | |
2018-04-16 13:32
Diffstat (limited to 'quantitative_ta')
| -rw-r--r-- | quantitative_ta/chapter.tex | 6 |
1 files changed, 3 insertions, 3 deletions
diff --git a/quantitative_ta/chapter.tex b/quantitative_ta/chapter.tex index 099b606..cecf2b9 100644 --- a/quantitative_ta/chapter.tex +++ b/quantitative_ta/chapter.tex @@ -62,7 +62,7 @@ calibration sample. % Given the eight experimental measurables ($V_\mathrm{T}$, $V_\mathrm{R}$, $V_{\Delta\mathrm{T}}$, $V_{\Delta\mathrm{R}}$, $V_{\mathrm{T},\,\mathrm{ref}}$, $V_{\mathrm{R},\,\mathrm{ref}}$, $\mathcal{T}_\mathrm{ref}$, $\mathcal{R}_\mathrm{ref}$) I can express all of the intensities in -\autoref{eq:ta_complete} in terms of $I_0$. % +\autoref{qta:eqn:ta_complete} in terms of $I_0$. % \begin{eqnarray} C_\mathrm{T} &=& \frac{\mathcal{T}_\mathrm{ref}}{V_{\mathrm{T},\,\mathrm{ref}}} \\ @@ -73,8 +73,8 @@ I_{\Delta\mathrm{T}} &=& I_0 C_\mathrm{T} V_{\Delta\mathrm{T}} \\ I_{\Delta\mathrm{R}} &=& I_0 C_\mathrm{R} V_{\Delta\mathrm{R}} \end{eqnarray} -Wonderfully, the $I_0$ cancels when plugged back in to \autoref{eq:ta_complete}, leaving a final -expression for $\Delta A$ that only depends on my eight measurables. % +Wonderfully, the $I_0$ cancels when plugged back into \autoref{qta:eqn:ta_complete}, leaving a +final expression for $\Delta A$ that only depends on my eight measurables. % \begin{equation} \Delta A = - \log_{10} \left(\frac{C_\mathrm{T}(V_\mathrm{T} + V_{\Delta\mathrm{T}}) + C_\mathrm{R}(V_\mathrm{R} + V_{\Delta\mathrm{R}})}{C_\mathrm{T} V_\mathrm{T} + C_\mathrm{R} V_\mathrm{R}}\right) |