diff --git a/doc/source/models/index.rst b/doc/source/models/index.rst
index 957b29e4603d0067e7eb9f786603a27201f357c9..caf53f8c3ebc1b2c6077c808fc085bfc7728e3d1 100644
--- a/doc/source/models/index.rst
+++ b/doc/source/models/index.rst
@@ -7,6 +7,7 @@ Models
 
    make_model
    cubics
+   model_potentials
    CPA
    PCSAFT
    multifluid
diff --git a/doc/source/models/model_potentials.ipynb b/doc/source/models/model_potentials.ipynb
new file mode 100644
index 0000000000000000000000000000000000000000..c0c400f50ab721eb0e08bb15287d0e5c6645580a
--- /dev/null
+++ b/doc/source/models/model_potentials.ipynb
@@ -0,0 +1,152 @@
+{
+ "cells": [
+  {
+   "cell_type": "markdown",
+   "id": "940cc903",
+   "metadata": {},
+   "source": [
+    "# Model Potentials\n",
+    "\n",
+    "These EOS for model potentials are useful for understanding theory, and capture some (but perhaps not all) of the physics of \"real\" fluids."
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": null,
+   "id": "f5463428",
+   "metadata": {},
+   "outputs": [],
+   "source": [
+    "import teqp\n",
+    "teqp.__version__"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "id": "bf22ac3d",
+   "metadata": {},
+   "source": [
+    "# Square-well"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": null,
+   "id": "435a84a9",
+   "metadata": {},
+   "outputs": [],
+   "source": [
+    "m = {  \n",
+    "  \"kind\": \"SW_EspindolaHeredia2009\", \n",
+    "  \"model\": {\n",
+    "      \"lambda\": 1.3\n",
+    "  }\n",
+    "}\n",
+    "model = teqp.make_model(m)"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "id": "f0caf9ea",
+   "metadata": {},
+   "source": [
+    "# EXP-6"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": null,
+   "id": "dc38b705",
+   "metadata": {},
+   "outputs": [],
+   "source": [
+    "m = {  \n",
+    "  \"kind\": \"EXP6_Kataoka1992\", \n",
+    "  \"model\": {\n",
+    "      \"alpha\": 12\n",
+    "  }\n",
+    "}\n",
+    "model = teqp.make_model(m)"
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "id": "b87cbd05",
+   "metadata": {},
+   "source": [
+    "# Lennard-Jones Fluid"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": null,
+   "id": "739e3e2b",
+   "metadata": {},
+   "outputs": [],
+   "source": [
+    "m = {  \n",
+    "  \"kind\": \"LJ126_TholJPCRD2016\", \n",
+    "  \"model\": {}\n",
+    "}\n",
+    "model = teqp.make_model(m) "
+   ]
+  },
+  {
+   "cell_type": "markdown",
+   "id": "fad87158",
+   "metadata": {},
+   "source": [
+    "# Two-Center Lennard-Jones Fluid"
+   ]
+  },
+  {
+   "cell_type": "code",
+   "execution_count": null,
+   "id": "ae5646de",
+   "metadata": {},
+   "outputs": [],
+   "source": [
+    "m = {  \n",
+    "  'kind': '2CLJF-Dipole', \n",
+    "  'model': {\n",
+    "      \"author\": \"2CLJF_Lisal\",\n",
+    "      'L^*': 0.5,\n",
+    "      '(mu^*)^2': 0.1\n",
+    "  }\n",
+    "}\n",
+    "model = teqp.make_model(m)\n",
+    "\n",
+    "m = {  \n",
+    "  'kind': '2CLJF-Quadrupole', \n",
+    "  'model': {\n",
+    "      \"author\": \"2CLJF_Lisal\",\n",
+    "      'L^*': 0.5,\n",
+    "      '(mu^*)^2': 0.1\n",
+    "  }\n",
+    "}\n",
+    "model = teqp.make_model(m)"
+   ]
+  }
+ ],
+ "metadata": {
+  "kernelspec": {
+   "display_name": "Python 3 (ipykernel)",
+   "language": "python",
+   "name": "python3"
+  },
+  "language_info": {
+   "codemirror_mode": {
+    "name": "ipython",
+    "version": 3
+   },
+   "file_extension": ".py",
+   "mimetype": "text/x-python",
+   "name": "python",
+   "nbconvert_exporter": "python",
+   "pygments_lexer": "ipython3",
+   "version": "3.10.6"
+  }
+ },
+ "nbformat": 4,
+ "nbformat_minor": 5
+}