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Christer Watson edited Analysis.tex
over 9 years ago
Commit id: 130d364a89474acf69b3a66e56d5d0984d19e18a
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index bc4e84f..cc010d6 100644
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\begin{equation}
N = \frac{I}{B_\nu \mu_H m_H \kappa R_d}\\
B_\nu = \frac{2 h \nu^3}{c^2 (e^\frac{h \nu}{kT}-1)}\\
I = 1.085\times 10^{-18}
B_\nu(860 GHz)\left(\frac{18.6"}{\theta}\right)^2 B_{mod}(860 GHz)\left(\frac{18.6"}{\theta}\right)^2\\
\kappa = \kappa_{1mm} \left(\frac{\lambda}{1.3mm}\right)^{-\beta}\\
\end{equation}
where we have made the following assumptions: $\kappa_{1mm}$ = 0.11 $\frac{m^2}{kg}$, appropriate for ice-covered dust grains from OH94, $\theta$=15.0", the beamsize of the GBT at 49 GHz, and $\beta$ = 2.