From f6c762266440ef4a15cbca98d35a7e6a3d9f1c30 Mon Sep 17 00:00:00 2001
From: NT <nils.thuerey@tum.de>
Date: Fri, 20 Aug 2021 11:28:02 +0200
Subject: [PATCH] additional unicode tweaks

---
 diffphys-code-ns.ipynb | 12 ++++++------
 fixup-latex.py         |  7 +++++++
 2 files changed, 13 insertions(+), 6 deletions(-)

diff --git a/diffphys-code-ns.ipynb b/diffphys-code-ns.ipynb
index 83bcddf..f6b647f 100644
--- a/diffphys-code-ns.ipynb
+++ b/diffphys-code-ns.ipynb
@@ -127,7 +127,7 @@
     {
      "data": {
       "text/plain": [
-       "(inflow_loc\u1d47=4, x\u02e2=32, y\u02e2=40)"
+       "(inflow_locᵇ=4, xˢ=32, yˢ=40)"
       ]
      },
      "execution_count": 2,
@@ -267,7 +267,7 @@
      "name": "stdout",
      "output_type": "stream",
      "text": [
-      "Velocity dimensions: (inflow_loc\u1d47=4, x\u02e2=32, y\u02e2=40, vector\u1d5b=2)\n"
+      "Velocity dimensions: (inflow_locᵇ=4, xˢ=32, yˢ=40, vectorᵛ=2)\n"
      ]
     }
    ],
@@ -313,8 +313,8 @@
      "name": "stdout",
      "output_type": "stream",
      "text": [
-      "Some gradient info: StaggeredGrid[(inflow_loc\u1d47=4, x\u02e2=32, y\u02e2=40, vector\u1d5b=2), size=(32, 40), extrapolation=0]\n",
-      "(x\u02e2=31, y\u02e2=40) float32  -17.366662979125977 < ... < 14.014090538024902\n"
+      "Some gradient info: StaggeredGrid[(inflow_locᵇ=4, xˢ=32, yˢ=40, vectorᵛ=2), size=(32, 40), extrapolation=0]\n",
+      "(xˢ=31, yˢ=40) float32  -17.366662979125977 < ... < 14.014090538024902\n"
      ]
     }
    ],
@@ -334,7 +334,7 @@
    "source": [
     "The last two lines just print some information about the resulting gradient field. Naturally, it has the same shape as the velocity itself: it's a staggered grid with four inflow locations. The last line shows how to access the x-components of one of the gradients.\n",
     "\n",
-    "We could use this to take a look at the content of the computed gradient with regular plotting functions, e.g., by converting the x component of one of the simulations to a numpy array via `velocity_grad.values.inflow_loc[0].vector[0].numpy('y,x')`. However, below we'll use phiflow's `view()` function instead. It automatically analyzes the grid content and provides UI buttons to choose different viewing modes. You can use them to show arrows, single components of the 2-dimensional velocity vectors, or their magnitudes.\n"
+    "We could use this to take a look at the content of the computed gradient with regular plotting functions, e.g., by converting the x component of one of the simulations to a numpy array via `velocity_grad.values.inflow_loc[0].vector[0].numpy('y,x')`. However, below we'll use phiflow's `view()` function instead. It automatically analyzes the grid content and provides UI buttons to choose different viewing modes. You can use them to show arrows, single components of the 2-dimensional velocity vectors, or their magnitudes. (Because of its interactive nature, the corresponding image won't show up outside of Jupyter, though.)\n"
    ]
   },
   {
@@ -664,5 +664,5 @@
   }
  },
  "nbformat": 4,
- "nbformat_minor": 0
+ "nbformat_minor": 1
 }
diff --git a/fixup-latex.py b/fixup-latex.py
index fd5ddcd..e48df5c 100644
--- a/fixup-latex.py
+++ b/fixup-latex.py
@@ -49,6 +49,7 @@ recs.append( re.compile(r"approach using continuous convolutions {.}.hyperlink{c
 rect.append( "approach using continuous convolutions {[}\\\\protect\\\\hyperlink{cite.references:id14}{UPTK19}{]}" )
 
 # fixup unicode symbols 
+# compare book-in2.tex -> book.tex after iconv 
 
 recs.append( re.compile(r"’" ) ) # unicode ' 
 rect.append( "\'" )
@@ -77,6 +78,12 @@ rect.append( " " )
 # recs.append( re.compile(r"") )
 # rect.append( "" )
 
+# recs.append( re.compile(r"") )
+# rect.append( "" )
+
+# recs.append( re.compile(r"") )
+# rect.append( "" )
+
 
 # fixup title , cumbersome...