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Stephen edited section_Methods_In_the_past__.tex
over 8 years ago
Commit id: e98ae9d156184b3c4efd2c61031603c24ab00376
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\[\delta - \delta_0\ = (\alpha-1)ln\bigg[\frac{q}{q_0}\bigg]\]
or
\[\R = R_0.f^{(\alpha_e-1)}\]
\textbf{Super Rayleigh???}
The idea of super rayleigh produces isotopic ratios that fall below open rayleigh models in $\delta$.H_2O space. \citet{Noone_2012} and \citet{Worden_2007} argued that this is caused by mixing between vapour evaporated from falling rain drops and ambient vapour. \citet{Noone_2012} showed that an increase in $\alpha$ as the rain re-evaporates would lead to this super rayleigh curve -> the slope of $\delta$.H_2O space is steeper than an open rayleigh system where $\alpha$ is smaller. Simply they suggested:
\[\alpha = (1+\phi)\alpha_e\]