diff --git a/notes/cylinder.png b/notes/cylinder.png new file mode 100644 index 0000000..6c5ec58 Binary files /dev/null and b/notes/cylinder.png differ diff --git a/notes/cylinderT.lyx b/notes/cylinderT.lyx new file mode 100644 index 0000000..0378527 --- /dev/null +++ b/notes/cylinderT.lyx @@ -0,0 +1,323 @@ +#LyX 2.4 created this file. For more info see https://www.lyx.org/ +\lyxformat 584 +\begin_document +\begin_header +\save_transient_properties true +\origin unavailable +\textclass article +\use_default_options true +\maintain_unincluded_children false +\language english +\language_package default +\inputencoding utf8 +\fontencoding auto +\font_roman "default" "default" +\font_sans "default" "default" +\font_typewriter "default" "default" +\font_math "auto" "auto" +\font_default_family default +\use_non_tex_fonts false +\font_sc false +\font_roman_osf false +\font_sans_osf false +\font_typewriter_osf false +\font_sf_scale 100 100 +\font_tt_scale 100 100 +\use_microtype false +\use_dash_ligatures true +\graphics default +\default_output_format default +\output_sync 0 +\bibtex_command default +\index_command default +\float_placement class +\float_alignment class +\paperfontsize default +\spacing single +\use_hyperref false +\papersize default +\use_geometry false +\use_package amsmath 1 +\use_package amssymb 1 +\use_package cancel 1 +\use_package esint 1 +\use_package mathdots 1 +\use_package mathtools 1 +\use_package mhchem 1 +\use_package stackrel 1 +\use_package stmaryrd 1 +\use_package undertilde 1 +\cite_engine basic +\cite_engine_type default +\biblio_style plain +\use_bibtopic false +\use_indices false +\paperorientation portrait +\suppress_date false +\justification true +\use_refstyle 1 +\use_minted 0 +\use_lineno 0 +\index Index +\shortcut idx +\color #008000 +\end_index +\secnumdepth 3 +\tocdepth 3 +\paragraph_separation indent +\paragraph_indentation default +\is_math_indent 0 +\math_numbering_side default +\quotes_style english +\dynamic_quotes 0 +\papercolumns 1 +\papersides 1 +\paperpagestyle default +\tablestyle default +\tracking_changes false +\output_changes false +\html_math_output 0 +\html_css_as_file 0 +\html_be_strict false +\end_header + +\begin_body + +\begin_layout Standard +\begin_inset CommandInset include +LatexCommand input +filename "makrot.lyx" +literal "false" + +\end_inset + + +\end_layout + +\begin_layout Title +T-matrix of an axially symmetric particle +\end_layout + +\begin_layout Standard +So we have +\begin_inset CommandInset citation +LatexCommand cite +after "(9.12)" +key "kristensson_scattering_2016" +literal "false" + +\end_inset + +: +\begin_inset Formula +\begin{align*} +R_{nn'} & =ik^{2}\iint_{S_{s}}\left(\frac{\eta}{\eta_{1}}\wfkcreg_{n}\left(k\vect r\right)\times\wfkcreg_{\overline{n'}}\left(k\vect r\right)+\wfkcreg_{\overline{n'}}\left(k\vect r\right)\times\wfkcreg_{n}\left(k\vect r\right)\right)\cdot\uvec{\nu}\,\ud S,\\ +Q_{nn'} & =ik^{2}\iint_{S_{s}}\left(\frac{\eta}{\eta_{1}}\wfkcout_{n}\left(k\vect r\right)\times\wfkcreg_{\overline{n'}}\left(k\vect r\right)+\wfkcout_{\overline{n'}}\left(k\vect r\right)\times\wfkcreg_{n}\left(k\vect r\right)\right)\cdot\uvec{\nu}\,\ud S, +\end{align*} + +\end_inset + +where +\begin_inset Formula $S_{s}$ +\end_inset + + is the scatterer surface and +\begin_inset Formula $\uvec{\nu}$ +\end_inset + + is the outwards pointing unit normal to it; then +\begin_inset Formula +\[ +T_{nn'}=-\sum_{n''}R_{nn''}Q_{n''n}^{-1}. +\] + +\end_inset + + +\end_layout + +\begin_layout Standard +Let us consider the case with full rotational symmetry around the +\begin_inset Formula $z$ +\end_inset + + axis and parametrise the integral in terms of polar angle +\begin_inset Formula $\theta$ +\end_inset + +. + Let +\begin_inset Formula $\beta$ +\end_inset + + be the angle between the surface normal +\begin_inset Formula $\uvec{\nu}$ +\end_inset + + and the coordinate radial direction +\begin_inset Formula $\uvec r$ +\end_inset + +. + The infinitesimal surface area element is then +\begin_inset Formula +\[ +\ud S\left(\theta\right)=\frac{\left(r\left(\theta\right)\right)^{2}\sin\theta}{\cos\beta\left(\theta\right)}\ud\theta\,\ud\phi +\] + +\end_inset + +and the surface normal in local coordinates +\begin_inset Formula +\[ +\uvec{\nu}\left(\theta\right)=\uvec r\cos\beta\left(\theta\right)+\uvec{\theta}\sin\beta\left(\theta\right), +\] + +\end_inset + +which also sets a convention for the sign of +\begin_inset Formula $\beta$ +\end_inset + +. +\end_layout + +\begin_layout Standard +For fully axially symmetric particles the integrals vanish for +\begin_inset Formula $m\ne-m'$ +\end_inset + + due to the +\begin_inset Formula $e^{i\left(m+m'\right)}$ +\end_inset + + asimuthal factor in the integrand. +\end_layout + +\begin_layout Standard +\begin_inset Float figure +placement document +alignment document +wide false +sideways false +status open + +\begin_layout Plain Layout +\align center +\begin_inset Graphics + filename cylinder.png + lyxscale 30 + width 50text% + +\end_inset + + +\end_layout + +\begin_layout Plain Layout +\begin_inset Caption Standard + +\begin_layout Plain Layout +Parametrisation of cylindrical particle surface. +\end_layout + +\end_inset + + +\end_layout + +\begin_layout Plain Layout + +\end_layout + +\end_inset + + +\end_layout + +\begin_layout Standard +For cylindrical particle of radius +\begin_inset Formula $R$ +\end_inset + + and height +\begin_inset Formula $h$ +\end_inset + +, we can divide the parametrisation into three intervals +\begin_inset Formula $\left(0,\theta_{1}\right),\left(\theta_{1},\theta_{2}\right),\left(\theta_{2},\pi\right)$ +\end_inset + + where +\begin_inset Formula $\theta_{1}=\tan^{-1}\left(2R/h\right),\theta_{2}=\pi-\tan^{-1}\left(2R/h\right)$ +\end_inset + +: +\end_layout + +\begin_layout Enumerate +In the first section, +\begin_inset Formula $0<\theta<\theta_{1}$ +\end_inset + +, +\begin_inset Formula +\begin{align*} +r & =\frac{h}{2\cos\theta},\\ +\beta & =-\theta. +\end{align*} + +\end_inset + + +\end_layout + +\begin_layout Enumerate +In the second section, +\begin_inset Formula $\theta_{1}<\theta<\theta_{2}$ +\end_inset + +, +\begin_inset Formula +\begin{align*} +r & =\frac{R}{\cos\left(\theta-\pi/2\right)}=\frac{R}{\sin\theta},\\ +\beta & =-\theta+\pi/2. +\end{align*} + +\end_inset + + +\end_layout + +\begin_layout Enumerate +In the third section, +\begin_inset Formula $\theta_{2}<\theta<\pi$ +\end_inset + +, +\begin_inset Formula +\begin{align*} +r & =\frac{h}{2\cos\left(\theta-\pi\right)}=-\frac{h}{2\cos\theta},\\ +\beta & =-\theta+\pi. +\end{align*} + +\end_inset + + +\end_layout + +\begin_layout Standard +\begin_inset CommandInset bibtex +LatexCommand bibtex +btprint "btPrintCited" +bibfiles "Electrodynamics" +options "plain" +encoding "default" + +\end_inset + + +\end_layout + +\end_body +\end_document diff --git a/notes/makrot.lyx b/notes/makrot.lyx new file mode 100644 index 0000000..ab9c5ba --- /dev/null +++ b/notes/makrot.lyx @@ -0,0 +1,144 @@ +#LyX 2.4 created this file. For more info see https://www.lyx.org/ +\lyxformat 584 +\begin_document +\begin_header +\save_transient_properties true +\origin unavailable +\textclass article +\use_default_options true +\maintain_unincluded_children false +\language finnish +\language_package default +\inputencoding utf8 +\fontencoding auto +\font_roman "default" "default" +\font_sans "default" "default" +\font_typewriter "default" "default" +\font_math "auto" "auto" +\font_default_family default +\use_non_tex_fonts false +\font_sc false +\font_roman_osf false +\font_sans_osf false +\font_typewriter_osf false +\font_sf_scale 100 100 +\font_tt_scale 100 100 +\use_microtype false +\use_dash_ligatures true +\graphics default +\default_output_format default +\output_sync 0 +\bibtex_command default +\index_command default +\paperfontsize default +\use_hyperref false +\papersize default +\use_geometry false +\use_package amsmath 1 +\use_package amssymb 1 +\use_package cancel 1 +\use_package esint 1 +\use_package mathdots 1 +\use_package mathtools 1 +\use_package mhchem 1 +\use_package stackrel 1 +\use_package stmaryrd 1 +\use_package undertilde 1 +\cite_engine basic +\cite_engine_type default +\use_bibtopic false +\use_indices false +\paperorientation portrait +\suppress_date false +\justification true +\use_refstyle 1 +\use_minted 0 +\use_lineno 0 +\index Index +\shortcut idx +\color #008000 +\end_index +\secnumdepth 3 +\tocdepth 3 +\paragraph_separation indent +\paragraph_indentation default +\is_math_indent 0 +\math_numbering_side default +\quotes_style english +\dynamic_quotes 0 +\papercolumns 1 +\papersides 1 +\paperpagestyle default +\tablestyle default +\tracking_changes false +\output_changes false +\html_math_output 0 +\html_css_as_file 0 +\html_be_strict false +\end_header + +\begin_body + +\begin_layout Standard +\begin_inset FormulaMacro +\newcommand{\ud}{\mathrm{d}} +\end_inset + + +\begin_inset FormulaMacro +\newcommand{\abs}[1]{\left|#1\right|} +\end_inset + + +\begin_inset FormulaMacro +\newcommand{\vect}[1]{\mathbf{#1}} +\end_inset + + +\begin_inset FormulaMacro +\newcommand{\uvec}[1]{\hat{\mathbf{#1}}} +\end_inset + + +\end_layout + +\begin_layout Standard +\begin_inset FormulaMacro +\newcommand{\vsh}{\vect A} +\end_inset + + +\begin_inset FormulaMacro +\newcommand{\vshD}{\vect{A'}} +\end_inset + + +\begin_inset FormulaMacro +\newcommand{\wfkc}{\vect y} +\end_inset + + +\begin_inset FormulaMacro +\newcommand{\wfkcout}{\vect u} +\end_inset + + +\begin_inset FormulaMacro +\newcommand{\wfkcreg}{\vect v} +\end_inset + + +\begin_inset FormulaMacro +\newcommand{\wckcreg}{a} +\end_inset + + +\begin_inset FormulaMacro +\newcommand{\wckcout}{f} +\end_inset + + +\end_layout + +\end_body +\end_document