diff --git a/chapters/02_methods.ist b/chapters/02_methods.ist index de8466c..84cefc8 100644 --- a/chapters/02_methods.ist +++ b/chapters/02_methods.ist @@ -1,5 +1,5 @@ % makeindex style file created by the glossaries package -% for document '02_methods' on 2026-9-29 +% for document '02_methods' on 2026-9-30 actual '?' encap '|' level '!' diff --git a/chapters/02_methods.pdf b/chapters/02_methods.pdf index efe87f8..3789986 100644 Binary files a/chapters/02_methods.pdf and b/chapters/02_methods.pdf differ diff --git a/chapters/02_methods.tex b/chapters/02_methods.tex index 6051bfa..4dab1af 100644 --- a/chapters/02_methods.tex +++ b/chapters/02_methods.tex @@ -82,7 +82,7 @@ \subsection{Scanning Mobility Particle Sizer} \label{methods: subsec: SMPS} - The aerosol concentration is measured using a \gls{SMPSa}, which in turn consists of a \gls{DMAa} and a \gls{CPCa}, arranged in series. + The aerosol concentration is measured using a \gls{SMPSa}, which in turn consists of a neutraliser, a \gls{DMAa} and a \gls{CPCa}, arranged in series. The \gls{DMAa} is ramping a time-dependent voltage profile $U(t)$ between its two electrodes. This creates a time-varying electric field of the strength $E\approx U/(d_{o}-d_{i})$ which in turn causes particles within the \gls{DMAa} to experience a drift in this field of velocity $v=Z_{p}E$, where $Z_{p}$ denotes the electrical mobility. \begin{equation} m_{\textnormal{F}}=\int_{t_{\textnormal{in}}}^{t_{\textnormal{out}}}\gls{MFLOWs}\,\der{t}\approx\sum_{\textnormal{Samples}}\gls{MFLOWs}_{i}\Delta t_{i}