Issue 920 dimensional interp

examples/notebooks/Creating Models/1-an-ode-model.ipynb

@@ -253,6 +253,13 @@
    "source": [
     "In the [next notebook](./2-a-pde-model.ipynb) we show how to create, discretise and solve a PDE model in pybamm."
    ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": null,
+   "metadata": {},
+   "outputs": [],
+   "source": []
   }
  ],
  "metadata": {
@@ -271,7 +278,7 @@
    "name": "python",
    "nbconvert_exporter": "python",
    "pygments_lexer": "ipython3",
-   "version": "3.7.5"
+   "version": "3.6.9"
   }
  },
  "nbformat": 4,

examples/notebooks/Creating Models/2-a-pde-model.ipynb

@@ -280,6 +280,13 @@
    "source": [
     "In the [next notebook](./3-negative-particle-problem.ipynb) we build on the example here to to solve the problem of diffusion in the negative electrode particle within the single particle model. In doing so we will also cover how to include parameters in a model. "
    ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": null,
+   "metadata": {},
+   "outputs": [],
+   "source": []
   }
  ],
  "metadata": {

examples/notebooks/Creating Models/3-negative-particle-problem.ipynb

@@ -298,6 +298,13 @@
    "source": [
     "In the [next notebook](./4-comparing-full-and-reduced-order-models.ipynb) we consider the limit of fast diffusion in the particle. This leads to a reduced-order model for the particle behaviour, which we compare with the full (Fickian diffusion) model. "
    ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": null,
+   "metadata": {},
+   "outputs": [],
+   "source": []
   }
  ],
  "metadata": {
@@ -316,7 +323,7 @@
    "name": "python",
    "nbconvert_exporter": "python",
    "pygments_lexer": "ipython3",
-   "version": "3.7.5"
+   "version": "3.6.9"
   }
  },
  "nbformat": 4,

examples/notebooks/Creating Models/4-comparing-full-and-reduced-order-models.ipynb

@@ -282,7 +282,7 @@
     {
      "data": {
       "application/vnd.jupyter.widget-view+json": {
-       "model_id": "dbcd70fa09c6404dab80036156401985",
+       "model_id": "a020dc7cd8574e698ef0e06d4392e689",
        "version_major": 2,
        "version_minor": 0
       },
@@ -357,6 +357,13 @@
    "source": [
     "In the [next notebook](./5-a-simple-SEI-model.ipynb) we consider a simple model for SEI growth, and show how to correctly pose the model in non-dimensional form and then create and solve it using pybamm."
    ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": null,
+   "metadata": {},
+   "outputs": [],
+   "source": []
   }
  ],
  "metadata": {
@@ -375,7 +382,7 @@
    "name": "python",
    "nbconvert_exporter": "python",
    "pygments_lexer": "ipython3",
-   "version": "3.7.5"
+   "version": "3.6.9"
   }
  },
  "nbformat": 4,

examples/notebooks/Creating Models/5-a-simple-SEI-model.ipynb

@@ -591,7 +591,7 @@
     {
      "data": {
       "application/vnd.jupyter.widget-view+json": {
-       "model_id": "efe1fe18458a42d88056baf689f6da80",
+       "model_id": "8d9c98b030934135908c6ddd5c92699b",
        "version_major": 2,
        "version_minor": 0
       },
@@ -635,6 +635,13 @@
    "source": [
     "The purpose of this notebook has been to go through the steps involved in getting a simple model working within PyBaMM. However, if you plan on reusing your model and want greater flexibility then we recommend that you create a new class for your model. We have set out instructions on how to do this in the \"Adding a Model\" tutorial in the documentation. "
    ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": null,
+   "metadata": {},
+   "outputs": [],
+   "source": []
   }
  ],
  "metadata": {

examples/notebooks/Getting Started/Tutorial 4 - Model Options.ipynb

@@ -54,7 +54,7 @@
     {
      "data": {
       "text/plain": [
-       "<pybamm.solvers.solution.Solution at 0x7fabe3f3e6a0>"
+       "<pybamm.solvers.solution.Solution at 0x7f648b879828>"
       ]
      },
      "execution_count": 3,
@@ -89,7 +89,7 @@
     {
      "data": {
       "application/vnd.jupyter.widget-view+json": {
-       "model_id": "6424823b40b548c8ad170e2e6797b5cb",
+       "model_id": "a551cd74c2c94180870a552c07bd0715",
        "version_major": 2,
        "version_minor": 0
       },

examples/notebooks/expression_tree/expression-tree.ipynb

@@ -202,13 +202,6 @@
     "\n",
     "After the third stage, our expression tree is now able to be evaluated by one of the solver classes. Note that we have used a single equation above to illustrate the different types of expression trees in PyBaMM, but any given models will consist of many RHS or algebraic equations, along with boundary conditions. See [here](https://github.com/pybamm-team/PyBaMM/blob/master/examples/notebooks/add-model.ipynb) for more details of PyBaMM models."
    ]
-  },
-  {
-   "cell_type": "code",
-   "execution_count": null,
-   "metadata": {},
-   "outputs": [],
-   "source": []
   }
  ],
  "metadata": {
@@ -227,7 +220,7 @@
    "name": "python",
    "nbconvert_exporter": "python",
    "pygments_lexer": "ipython3",
-   "version": "3.6.7"
+   "version": "3.6.9"
   }
  },
  "nbformat": 4,

examples/notebooks/models/DFN.ipynb

@@ -195,7 +195,7 @@
     {
      "data": {
       "application/vnd.jupyter.widget-view+json": {
-       "model_id": "29f22a3ab3bd4ce8825acdd6fb655f36",
+       "model_id": "c0cb0a7f6d134873aeff4ef5b3a4730a",
        "version_major": 2,
        "version_minor": 0
       },
@@ -247,6 +247,13 @@
     "[1] M. Doyle,  T.F. Fuller,  and J. Newman.  Modeling of galvanostatic charge and discharge of thelithium/polymer/insertion cell.Journal of the Electrochemical society, 140(6):1526–1533, 1993"
    ]
   },
+  {
+   "cell_type": "code",
+   "execution_count": null,
+   "metadata": {},
+   "outputs": [],
+   "source": []
+  },
   {
    "cell_type": "code",
    "execution_count": null,