finish first cut for CCA talk

Author: zingale

presentations/custom.css

@@ -4,6 +4,11 @@ font-size: 80%;
 }
 
 
+em {
+color: blue;
+}
+
+
 .reveal p {
 margin-bottom: 0.25em;
 margin-top: 0.5em;
@@ -20,5 +25,5 @@ font-family: carlito;
 }
 
 div.output pre {
-    font-size: 60%;
+    font-size: 65%;
 }

presentations/docs.png

@@ -69,17 +69,17 @@
    "source": [
     "## History:\n",
     "\n",
-    "  * First version in 2003: python + Numeric + C extensions\n",
+    "  - _First version in 2003_: python + Numeric + C extensions\n",
     "  \n",
-    "  * May 2004: switch to python + numarray + C extensions\n",
+    "  - _May 2004_: switch to python + numarray + C extensions\n",
     "  \n",
-    "    cvs commit:\n",
+    "    - cvs commit:\n",
     "  \n",
-    "    > convert from Numeric to numarray, since numarray seems to be the future.\n",
+    "      > convert from Numeric to numarray, since numarray seems to be the future.\n",
     "        \n",
-    "  * May 2012: revived, rewritten in python + NumPy + f2py\n",
+    "  - _May 2012_: revived, rewritten in python + NumPy + f2py\n",
     "  \n",
-    "  * Nov 2018: python + NumPy + Numba"
+    "  - _Nov 2018_: python + NumPy + Numba"
    ]
   },
   {
@@ -92,21 +92,21 @@
    "source": [
     "## Current Solvers\n",
     "\n",
-    "  * linear advection (2nd and 4th order FV, WENO; CTU, RK, and SDC time integration)\n",
+    "  * *linear advection*: 2nd and 4th order FV, WENO; CTU, RK, and SDC time integration\n",
     "  \n",
-    "  * compressible hydrodynamics (2nd order CTU PLM, 2nd order MOL RK, 4th order FV solver with RK or SDC integration)\n",
+    "  * *compressible hydrodynamics*: 2nd order CTU PLM, 2nd order MOL RK, 4th order FV solver with RK or SDC integration\n",
     "  \n",
-    "  * shallow water hydrodynamics\n",
+    "  * *shallow water hydrodynamics*\n",
     "  \n",
-    "  * multigrid\n",
+    "  * *multigrid*: force non-constant coefficient general elliptic equations\n",
     "  \n",
-    "  * implicit thermal diffusion (using multigrid)\n",
+    "  * *implicit thermal diffusion*: using multigrid\n",
     "  \n",
-    "  * incompressible hydrodynamics (approximate projection method)\n",
+    "  * *incompressible hydrodynamics*: 2nd order accurate approximate projection method\n",
     "  \n",
-    "  * low Mach number atmospheric hydrodynamics (pseudo-imcompressible method)\n",
+    "  * *low Mach number atmospheric hydrodynamics*: pseudo-imcompressible method\n",
     "  \n",
-    "  * special relativistic compressible hydrodynamics"
+    "  * *special relativistic compressible hydrodynamics*"
    ]
   },
   {
@@ -213,13 +213,13 @@
       "\u001b[33mparameter vis.store_images never used\u001b[0m\n",
       "\u001b[33mparameter particles.n_particles never used\u001b[0m\n",
       "\u001b[33mparameter particles.particle_generator never used\u001b[0m\n",
-      "main:  0.08763742446899414\n"
+      "main:  0.08537530899047852\n"
      ]
     },
     {
      "data": {
       "text/plain": [
-       "<advection.simulation.Simulation at 0x7f75b1772a90>"
+       "<advection.simulation.Simulation at 0x7f9c1829df10>"
       ]
      },
      "execution_count": 1,
@@ -482,11 +482,15 @@
    ]
   },
   {
-   "cell_type": "code",
-   "execution_count": null,
-   "metadata": {},
-   "outputs": [],
-   "source": []
+   "cell_type": "markdown",
+   "metadata": {
+    "slideshow": {
+     "slide_type": "slide"
+    }
+   },
+   "source": [
+    "![docs](docs.png)"
+   ]
   }
  ],
  "metadata": {