From 0268072ba91bf80ffd3164ea9a325502d5fe6f8c Mon Sep 17 00:00:00 2001 From: Malcolm Ramsay Date: Wed, 26 Feb 2020 18:09:47 +1100 Subject: [PATCH] chore: Move placeholder figure to methods There are still a couple of figures in the methods chapter. This breaks it's use elsewhere. ref #83 --- 00_Introduction/introduction.md | 4 +++- 01_Methods/Simulation_Conditions.md | 8 ++++---- .../figures/placeholder_figure.png | Bin 3 files changed, 7 insertions(+), 5 deletions(-) rename placeholder_figure.png => 01_Methods/figures/placeholder_figure.png (100%) diff --git a/00_Introduction/introduction.md b/00_Introduction/introduction.md index d290650..378fe2e 100644 --- a/00_Introduction/introduction.md +++ b/00_Introduction/introduction.md @@ -137,7 +137,9 @@ replicating experimental results. The Lewis--Wahnström model displays the same two-step relaxation process [@Wahnstrom1993,@Wahnstrom1997,@Lombardo2006] that is characteristic of fragile liquids in experiments. -![The geometry of the Lewis--Wahnström model](../placeholder_figure.png){width=80% #fig:lewis_wahnstrom_mol} +![The geometry of the Lewis--Wahnström model. +There is an angle of \SI{75}{\degree} subtending the centers of the thee particles. +](../00_Introduction/figures/lewis_wahnstrom.svg){width=80% #fig:lewis_wahnstrom_mol} The Lewis--Wahnström model of ortho-terphenyl is the most widely studied computational model of ortho-terphenyl, diff --git a/01_Methods/Simulation_Conditions.md b/01_Methods/Simulation_Conditions.md index 4a29f32..c764ca0 100644 --- a/01_Methods/Simulation_Conditions.md +++ b/01_Methods/Simulation_Conditions.md @@ -244,9 +244,9 @@ were packed together :::{class=subfigures id=fig:crystal_unit_cell} -![p2](../placeholder_figure.png){width=33% #fig:crystal_unit_cell_p2} -![pg](../placeholder_figure.png){width=33% #fig:crystal_unit_cell_pg} -![p2gg](../placeholder_figure.png){width=33% #fig:crystal_unit_cell_p2gg} +![p2](../01_Methods/figures/placeholder_figure.png){width=33% #fig:crystal_unit_cell_p2} +![pg](../01_Methods/figures/placeholder_figure.png){width=33% #fig:crystal_unit_cell_pg} +![p2gg](../01_Methods/figures/placeholder_figure.png){width=33% #fig:crystal_unit_cell_p2gg} The unit cells of the p2 (a) the pg (b) and the p2gg (c) crystals documenting the unit cell parameters @@ -308,7 +308,7 @@ of the number of overall layers so the orthorhombic configuration is favourable. ![Depicting conversion of tilted cell to orthorhombic -](../placeholder_figure.png){width=80% #fig:orthorhombisation} +](../01_Methods/figures/placeholder_figure.png){width=80% #fig:orthorhombisation} The outer 1/3 of the orthorhombic configuration is then melted at 2.2 times the melting point, diff --git a/placeholder_figure.png b/01_Methods/figures/placeholder_figure.png similarity index 100% rename from placeholder_figure.png rename to 01_Methods/figures/placeholder_figure.png