From 4187df3c96a3da6ed689f0a52d86c51d95f57ad5 Mon Sep 17 00:00:00 2001
From: Gaspard Jankowiak <gaspard@math.janko.fr>
Date: Mon, 31 Jan 2022 13:10:21 +0100
Subject: [PATCH] [numerics] improve dAJLR

---
 css/screen.scss          |  8 +++++++-
 numérique/dAJLR.markdown | 31 +++++++++++++++++++------------
 2 files changed, 26 insertions(+), 13 deletions(-)

diff --git a/css/screen.scss b/css/screen.scss
index 73abe6e..2d71c4c 100644
--- a/css/screen.scss
+++ b/css/screen.scss
@@ -86,10 +86,13 @@ footer { font-size: 75%; padding-bottom: 175px; }
 em { font-style: italic; }
 
 table { width: 100%; }
-thead { color: $dim; }
+/*thead { color: $dim; }*/
 th, td { padding: 0.3em; }
 tr { border-bottom: 1px dotted $tr-rule; }
 
+table.bordered { border-collapse: collapse; }
+table.bordered tr { border-top: 1px solid #bbb; border-bottom: 1px solid #bbb; }
+
 .publi_table td:nth-child(1) { width: 30%; }
 .publi_table td:nth-child(2) { width: 60%; }
 .publi_table td:nth-child(3) { width: 10%; }
@@ -137,6 +140,9 @@ ol li:hover { border-right: 3px solid $links; padding-right: 7px; }
 
 #http_code { text-align: center; font-size: 10em; line-height: 1em; }
 
+.footnotes { font-size: 0.8em; padding-left: 1em; margin-top: 2em;}
+.footnotes ol li { padding: 0; border: none; }
+
 @media (max-width: $small-width) {
     body { font-size: 80%; }
 }
diff --git a/numérique/dAJLR.markdown b/numérique/dAJLR.markdown
index 7fea99e..38b750d 100644
--- a/numérique/dAJLR.markdown
+++ b/numérique/dAJLR.markdown
@@ -2,23 +2,30 @@
 layout: default
 math: true
 lang: en
+subtitle: Curves with modulated stiffness
 ---
 
 ## Parameters:
 
-- $N = 180$
-- $L = 2π$
-- $M = 0$
-- $\mu = 10^{-2}$
+|$N$|$L$|$M$|$\mu$|
+|-|
+|$180$|$2\pi$|$0$|$10^{-2}$|
+|-|
+{:.bordered.center}
 
-## Results ($c_0 = 0$):
 
-- $\beta \equiv 1$: [movie](/s/numerics/dAJLR/beta=1.mp4)
-- symmetric double well ($\beta(x) = 1.01 + (x - 1)^2  (x + 1)^2$): [movie](/s/numerics/dAJLR/sym.mp4)
-- asymmetric double well ($\beta(x) = 1.2 + (x - 1)^2  (x + 1)^2 + x$): [movie](/s/numerics/dAJLR/asym.mp4)
+## Results:
 
-## Results $(c_0 > 0$):
+|$c_0$|$\beta$|$t_{max}$, iter$_{max}$|result|comment|
+|-|
+|$0$|const.||[movie](/s/numerics/dAJLR/beta=1.mp4)|
+|$10$|const.||[movie](/s/numerics/dAJLR/const_c0=10.mp4)
+|$0$|SDW[^1]||[movie](/s/numerics/dAJLR/sym.mp4)|
+|$0.1$|SDW||[movie](/s/numerics/dAJLR/sym-c0=0.1.mp4)
+|$1$|SDW||[movie](/s/numerics/dAJLR/sym-c0=1.mp4)
+|$0$|ADW[^2]||[movie](/s/numerics/dAJLR/asym.mp4)|
+|-|
+{:.bordered.center}
 
-- symmetric, $c_0 = 0.1$: [movie](/s/numerics/dAJLR/sym-c0=0.1.mp4)
-- symmetric, $c_0 = 1$: [movie](/s/numerics/dAJLR/sym-c0=1.mp4)
-- constant, $c_0 = 10$: [movie](/s/numerics/dAJLR/const_c0=10.mp4)
+[^1]: ($\beta(x) = 1.01 + (x - 1)^2  (x + 1)^2$))
+[^2]: ($\beta(x) = 1.2 + (x - 1)^2  (x + 1)^2 + x$))