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materialsvirtuallab · Jul 13, 2024 · 1e0a723 · 1e0a723
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diff --git a/notebooks/2013-01-01-Calculating Reaction Energies with the Materials API.ipynb b/notebooks/2013-01-01-Calculating Reaction Energies with the Materials API.ipynb
@@ -9,7 +9,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 1,
+   "execution_count": null,
    "metadata": {},
    "outputs": [],
    "source": [
@@ -19,7 +19,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 2,
+   "execution_count": null,
    "metadata": {},
    "outputs": [
     {

diff --git a/notebooks/2013-01-01-Calculating XRD patterns.ipynb b/notebooks/2013-01-01-Calculating XRD patterns.ipynb
@@ -11,7 +11,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 1,
+   "execution_count": null,
    "metadata": {},
    "outputs": [],
    "source": [
@@ -21,7 +21,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 2,
+   "execution_count": null,
    "metadata": {},
    "outputs": [],
    "source": [
@@ -46,7 +46,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 3,
+   "execution_count": null,
    "metadata": {},
    "outputs": [
     {
@@ -79,7 +79,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 4,
+   "execution_count": null,
    "metadata": {},
    "outputs": [
     {
@@ -108,7 +108,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 5,
+   "execution_count": null,
    "metadata": {},
    "outputs": [
     {
@@ -153,7 +153,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 6,
+   "execution_count": null,
    "metadata": {},
    "outputs": [
     {

diff --git a/notebooks/2013-01-01-Molecule.ipynb b/notebooks/2013-01-01-Molecule.ipynb
@@ -215,7 +215,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 1,
+   "execution_count": null,
    "metadata": {},
    "outputs": [
     {

diff --git a/notebooks/2013-01-01-Ordering Disordered Structures.ipynb b/notebooks/2013-01-01-Ordering Disordered Structures.ipynb
@@ -93,7 +93,9 @@
     }
    ],
    "source": [
-    "from pymatgen.transformations.standard_transformations import OrderDisorderedStructureTransformation\n",
+    "from pymatgen.transformations.standard_transformations import (\n",
+    "    OrderDisorderedStructureTransformation,\n",
+    ")\n",
     "\n",
     "trans = OrderDisorderedStructureTransformation()\n",
     "\n",
@@ -159,7 +161,9 @@
    "metadata": {},
    "outputs": [],
    "source": [
-    "from pymatgen.transformations.advanced_transformations import EnumerateStructureTransformation\n",
+    "from pymatgen.transformations.advanced_transformations import (\n",
+    "    EnumerateStructureTransformation,\n",
+    ")\n",
     "\n",
     "specie = {\"Cu\": 0.5, \"Au\": 0.5}\n",
     "cuau = Structure.from_spacegroup(\"Fm-3m\", Lattice.cubic(3.677), [specie], [[0, 0, 0]])\n",

diff --git a/notebooks/2013-01-01-Plotting the electronic structure of Fe.ipynb b/notebooks/2013-01-01-Plotting the electronic structure of Fe.ipynb
@@ -9,7 +9,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 1,
+   "execution_count": null,
    "metadata": {},
    "outputs": [],
    "source": [
@@ -20,7 +20,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 2,
+   "execution_count": null,
    "metadata": {},
    "outputs": [],
    "source": [
@@ -40,7 +40,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 6,
+   "execution_count": null,
    "metadata": {},
    "outputs": [
     {
@@ -91,13 +91,6 @@
     "grid(True)\n",
     "show()"
    ]
-  },
-  {
-   "cell_type": "code",
-   "execution_count": null,
-   "metadata": {},
-   "outputs": [],
-   "source": []
   }
  ],
  "metadata": {

diff --git a/... the Study and Design of Alkali Superionic Conductors Part 1 - Structure Generation.ipynb b/... the Study and Design of Alkali Superionic Conductors Part 1 - Structure Generation.ipynb
@@ -36,7 +36,9 @@
     "from pymatgen.core import Structure\n",
     "from pymatgen.io.vasp.sets import MPRelaxSet, batch_write_input\n",
     "from pymatgen.symmetry.analyzer import SpacegroupAnalyzer\n",
-    "from pymatgen.transformations.advanced_transformations import EnumerateStructureTransformation"
+    "from pymatgen.transformations.advanced_transformations import (\n",
+    "    EnumerateStructureTransformation,\n",
+    ")"
    ]
   },
   {

diff --git a/...Design of Alkali Superionic Conductors Part 2 - Phase and Electrochemical Stability.ipynb b/...Design of Alkali Superionic Conductors Part 2 - Phase and Electrochemical Stability.ipynb
@@ -18,7 +18,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 1,
+   "execution_count": null,
    "metadata": {},
    "outputs": [],
    "source": [
@@ -29,7 +29,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 2,
+   "execution_count": null,
    "metadata": {},
    "outputs": [],
    "source": [
@@ -40,7 +40,11 @@
     "\n",
     "import matplotlib as mpl\n",
     "import palettable\n",
-    "from pymatgen.analysis.phase_diagram import CompoundPhaseDiagram, PDPlotter, PhaseDiagram\n",
+    "from pymatgen.analysis.phase_diagram import (\n",
+    "    CompoundPhaseDiagram,\n",
+    "    PDPlotter,\n",
+    "    PhaseDiagram,\n",
+    ")\n",
     "from pymatgen.core import Composition, Element\n",
     "from pymatgen.entries.compatibility import MaterialsProjectCompatibility\n",
     "from pymatgen.entries.computed_entries import ComputedEntry\n",
@@ -60,7 +64,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 3,
+   "execution_count": null,
    "metadata": {},
    "outputs": [],
    "source": [
@@ -78,7 +82,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 4,
+   "execution_count": null,
    "metadata": {},
    "outputs": [
     {
@@ -110,7 +114,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 5,
+   "execution_count": null,
    "metadata": {},
    "outputs": [],
    "source": [
@@ -128,7 +132,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 6,
+   "execution_count": null,
    "metadata": {},
    "outputs": [
     {
@@ -157,7 +161,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 7,
+   "execution_count": null,
    "metadata": {},
    "outputs": [
     {
@@ -3026,7 +3030,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 8,
+   "execution_count": null,
    "metadata": {},
    "outputs": [
     {
@@ -4286,7 +4290,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 9,
+   "execution_count": null,
    "metadata": {},
    "outputs": [
     {
@@ -4315,7 +4319,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 10,
+   "execution_count": null,
    "metadata": {},
    "outputs": [],
    "source": [
@@ -4332,7 +4336,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 11,
+   "execution_count": null,
    "metadata": {},
    "outputs": [
     {
@@ -4390,7 +4394,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 12,
+   "execution_count": null,
    "metadata": {},
    "outputs": [
     {
@@ -4399,7 +4403,7 @@
        "Text(0, 0.5, 'Li uptake per f.u.')"
       ]
      },
-     "execution_count": 12,
+     "execution_count": null,
      "metadata": {},
      "output_type": "execute_result"
     },