l to L

Author: samjrholt

getting-started/unit-converter.ipynb

@@ -449,9 +449,9 @@
     "#### Micromagnetic\n",
     "The micromagnetic exchange correlation constant $A$ can be related to atomistic exchange using\n",
     "\\begin{equation}\n",
-    "A = \\frac{zJl^2}{12V},\n",
+    "A = \\frac{zJL^2}{12V},\n",
     "\\end{equation}\n",
-    "where $J$ is the Heisenberg exchange, $z$ is the number of nearest neighbour atoms, and $l$ is the distance between neighbouring atoms, and $V$ is the crystal volume per magnetic atom."
+    "where $J$ is the Heisenberg exchange, $z$ is the number of nearest neighbour atoms, and $L$ is the distance between neighbouring atoms, and $V$ is the crystal volume per magnetic atom."
    ]
   },
   {
@@ -496,7 +496,7 @@
    "source": [
     "The micromagnetic exchange correlation constant can be obtained directly from $T_c$ using \n",
     "\\begin{equation}\n",
-    "A = \\frac{k_\\text{B}T_\\text{C}l^2}{4\\epsilon V}.\n",
+    "A = \\frac{k_\\text{B}T_\\text{C}L^2}{4\\epsilon V}.\n",
     "\\end{equation}"
    ]
   },
@@ -556,9 +556,9 @@
     "#### Micromagentic\n",
     "The micromagnetic DMI constant $D$ can be related to atomistic DMI  using\n",
     "\\begin{equation}\n",
-    "D = \\frac{zdl}{12V},\n",
+    "D = \\frac{zdL}{12V},\n",
     "\\end{equation}\n",
-    "where $d$ is the atomistic DMI, $z$ is the number of nearest neighbour atoms, and $l$ is the distance between neighbouring atoms, and $V$ is the crystal volume per magnetic atom."
+    "where $d$ is the atomistic DMI, $z$ is the number of nearest neighbour atoms, and $L$ is the distance between neighbouring atoms, and $V$ is the crystal volume per magnetic atom."
    ]
   },
   {
@@ -627,7 +627,7 @@
    "id": "5709f726",
    "metadata": {},
    "source": [
-    "For a system with a micromagentic exchange of $6\\times 10^{-14}$ Jm$^{-1}$ and a helical period of 20 nm."
+    "For a system with a micromagentic exchange of $6\\times 10^{-14}$ Jm $^{-1}$ and a helical period of 20 nm."
    ]
   },
   {
@@ -660,9 +660,9 @@
    "source": [
     "For atomistic simulations, this can be converted into\n",
     "\\begin{equation}\n",
-    "P = \\frac{4\\pi J l}{|d|},\n",
+    "P = \\frac{4\\pi J L}{|d|},\n",
     "\\end{equation}\n",
-    "where $J$ is the Heisenberg exchange, $d$ is the atomistic DMI, and $l$ is the distance between neighbouring atoms."
+    "where $J$ is the Heisenberg exchange, $d$ is the atomistic DMI, and $L$ is the distance between neighbouring atoms."
    ]
   },
   {
@@ -763,7 +763,7 @@
    "source": [
     "### Anisotropy\n",
     "#### Micromagnetic\n",
-    "Anisotropy can be measured experimentally in a variety of different ways. The results torque magnetometry, for example, can give correct value for the anisotropy in units of Jm$^{-3}$."
+    "Anisotropy can be measured experimentally in a variety of different ways. The results torque magnetometry, for example, can give correct value for the anisotropy in units of Jm $^{-3}$."
    ]
   },
   {