From 5ad5b2ccd65a67329f716733d0af634da1a55f99 Mon Sep 17 00:00:00 2001 From: =?UTF-8?q?Marek=20Ne=C4=8Dada?= Date: Mon, 8 Jul 2019 17:54:36 +0300 Subject: [PATCH] More convention table entries Former-commit-id: b821b2664292d006056b8fc98167a89e820327b6 --- notes/conventions.md | 10 +++++++--- notes/mathjax_newcommands.js | 8 +++++++- 2 files changed, 14 insertions(+), 4 deletions(-) diff --git a/notes/conventions.md b/notes/conventions.md index bae6ac5..2e8956d 100644 --- a/notes/conventions.md +++ b/notes/conventions.md @@ -4,7 +4,7 @@ VSWF conventions | Source | VSWF definition | VSWF norm | CS Phase | Field expansion | Radiated power | Notes | |--- |--- |--- |--- |--- |--- |--- | -| Kristensson I \cite kristensson_spherical_2014 | \f[ \wfkcreg, \wfkcout= \dots \f] | | | \f[ +| Kristensson I \cite kristensson_spherical_2014 | \f[ \wfkcreg, \wfkcout= \dots \f] | | Yes, in the spherical harmonics definition, cf. sect. D.2. | \f[ \vect E = k \sqrt{\eta_0\eta} \sum_n \left( \wckcreg_n \wfkcreg_n + \wckcout_n \wfkcout_n \right), \\ \vect H = \frac{k \sqrt{\eta_0\eta}}{i\eta_0\eta} \sum_n \left( \wckcreg_n \wfkcreg_n + \wckcout_n \wfkcout_n \right), @@ -18,7 +18,11 @@ VSWF conventions \f] | \f[ P = \frac{1}{2k^2\eta_0\eta} \sum_n \left( \abs{\wckrout_n}^2 +\Re \left(\wckrout_n\wckrreg_n^{*}\right)\right) \f] | The \f$ \wckrreg, \wckrout \f$ coefficients have dimension \f$ \mathrm{V/m} \f$. | -| Reid \cite reid_electromagnetism_2016 | | | | | | | +| Reid \cite reid_electromagnetism_2016 | | | | \f[ + \vect E = \sum_\alpha \pr{ \wcrreg_\alpha \wfrreg_\alpha + \wcrout_\alpha wfrout_\alpha }, \\ + \vect H = \frac{1}{Z_0Z^r} \sum_\alpha \pr{ \wcrreg_\alpha \sigma_\alpha\wfrreg_\overline{\alpha} + + \wcrout_\alpha \sigma_\alpha\wfrout_\overline{\alpha}}, +\f] where \f$ \sigma_{lmM} = +1, \sigma_{lmN}=-1, \overline{lmM}=lmM, \overline{lmN}=lmM, \f$ cf. eq. (6). The notation is not extremely consistent throughout Reid's memo. | | | | Taylor \cite taylor_optical_2011 | \f[ \wfet_{mn}^{(j)} = \frac{n(n+1)}{kr}\sqrt{\frac{2n+1}{4\pi}\frac{\left(n-m\right)!}{\left(n+m\right)!}}P_{n}^{m}\left(\cos\theta\right)e^{im\phi}z_{n}^{j}\left(kr\right)\uvec{r} \\ +\left[\tilde{\tau}_{mn}\left(\cos\theta\right)\uvec{\theta}+i\tilde{\pi}_{mn}\left(\cos\theta\right)\uvec{\phi}\right]e^{im\phi}\frac{1}{kr}\frac{\ud\left(kr\,z_{n}^{j}\left(kr\right)\right)}{\ud(kr)}, \\ @@ -30,5 +34,5 @@ VSWF conventions \f] cf. \cite taylor_optical_2011, eqs. (2.40–41). I suspect that this is also wrong and \f$\delta_{m,m'}\f$ should be replaced with \f$\delta_{m,-m'}\f$. | | \f[ \vect E = \sum_{mn} \pr{-i \pr{\wcetreg_{mn}\wfetreg_{mn} + \wcmtreg_{mn}\wfmtreg{mn}} +i \pr{\wcetout_{mn}\wfetout_{mn} + \wcmtout_{mn}\wfmtout_{mn}}}, \\ \vect H = n_{ext}\sum_{mn} \pr{- \pr{\wcmtreg_{mn}\wfetreg_{mn} + \wcetreg_{mn}\wfmtreg{mn}} + \pr{\wcmtout_{mn}\wfetout_{mn} + \wcetout_{mn}\wfmtout_{mn}}}, -\f] | | Different sign for regular/scattered waves! Also WTF are the units of \f$ n_{ext} \f$? The whole definition seems rather inconsistent. | +\f] | | Different sign for regular/scattered waves! Also WTF are the units of \f$ n_{ext} \f$? The whole definition seems rather inconsistent. | diff --git a/notes/mathjax_newcommands.js b/notes/mathjax_newcommands.js index 3ce431b..7152545 100644 --- a/notes/mathjax_newcommands.js +++ b/notes/mathjax_newcommands.js @@ -28,7 +28,13 @@ MathJax.Hub.Config({ wcmtreg: "{q}", // regular magnetic wave coeff wcetreg: "{p}", // regular electric wave coeff wcmtout: "{b}", // outgoing magnetic wave coeff - wcetout: "{a}" // outgoing electric wave coeff + wcetout: "{a}", // outgoing electric wave coeff + + // Reid's VSWFs + wfrreg: "\\mathbf{\\mathcal{W}}^{\\mathrm{reg}}", // regular wave + wfrout: "\\mathbf{\\mathcal{W}}^{\\mathrm{out}}", // outgoing wave + wcrreg: "C^\\mathrm{inc}", // regular wave coeff + wcrout: "C^\\mathrm{scat}", // outgoing wave coeff } } });