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+{
+    "title": "Pixels and Their Neighbors",
+    "subtitle": "A Finite Volume Tutorial",
+    "contributors": {
+        "authors": [
+            "@bricks:person:rowan",
+            "@bricks:person:lindsey",
+            {
+                "name": "Douglas W. Oldenburg",
+                "affiliation": "@bricks:org:ubcgif"
+            }
+        ],
+        "reviewers": [
+            "@bricks:person:sgkang"
+        ],
+        "funders": [
+            "@bricks:org:ubc",
+            "@bricks:org:ubcgif",
+            "@bricks:org:nserc/vanier2016_12345"
+        ]
+    },
+    "date": "11/06/2016",
+    "modules": {
+        "../include/equations/dc-resistivity.imd": {
+            "name":"dc-res",
+            "init": {
+                "electrode_1.x": 5
+            }
+        }
+    },
+    "properties": {
+        "include": {
+            "@bricks:mason/icare": "*",
+            "@bricks:mason/youtube": "*",
+            "@bricks:hjkewr234": {
+                "import":["sigma", {"x":"lindsey_x"}],
+            }
+        },
+        "icare": {
+            "type": "int",
+            "default": 3,
+            "range": [1, 5]
+        },
+        "icare_5": {
+            "type": "event.trigger",
+            "alt": "Show All",
+            "trigger": "icare = 5"
+        },
+        "x": {
+            "type": "float",
+            "default": 0.0,
+            "range": [0.0, 25.0, 2.5]
+        },
+        "y": {
+            "type": "function",
+            "args": ["x"],
+            "function": "0.2 * x + 5"
+        },
+        "sigma": {
+            "type": "float",
+            "doc": "electrical conductivity",
+            "ref": "@bricks:hjkewr234",
+            "default": 0.0,
+            "units": "S/m",
+            "format": ".2e"
+            "log_range": [-3, 3, 0.5]
+        },
+        "background": {
+            "type": "float",
+            "doc": "electrical conductivity of the background",
+            "default": 0.0,
+            "units": "S/m",
+            "log_range": [-3, 3, 0.5]
+        },
+        "dcimage":{
+            "type": "service",
+            "url": "https://simpeg.xyz/services/v1/dc/block"
+            "ref": [
+                "@sgkang",
+                "@simpeg2015",
+                {
+                    "type": "influence",
+                    "reason": "color choices",
+                    "pointer": "@bricks:org:seaborn#color_pallet5"
+                }
+            ],
+            "parameters": {
+                "hx": [[1,100]],
+                "hy": [[1,100]],
+                "x0": "CC",
+                "block_location": [["{{ x }}",-25],[25,25]],
+                "block_sigma": "{{ sigma }}",
+                "background_sigma": "{{ background }}",
+                "return": "phi",
+                "size": [200,200],
+                "labels": true
+            }
+            "return": "image"
+        }
+    },
+    "issues":["@bricks:issues:gjashdf7890"],
+    "parent":["@bricks:fgh5678mnbv"]
+}
+
+This is an interactive document, the variables can be edited in the top right settings menu, or you can define them inline.
+For example, try dragging this slider all the way to the right: {{ icare.view.slider }}. I have hooked this up to change the
+amount of text that is shown to explain things! if you are a programmer look at the code {{ programmer.view.toggle }}.
+
+[ icare > 3 ]{
+    [>anchor("dc")]{
+        ### Direct Current Resistivity
+
+        Direct current (DC) resistivity surveys are used to obtain information about subsurface electrical
+        conductivity, which can be a diagnostic physical property in, for example, mineral exploration or
+        hydrogeologic problems, where the target of interest has a significant electrical conductivity
+        contrast from the background. In a DC resistivity survey, steady state currents are set up in the
+        subsurface by injecting current through a positive electrode (located at $r_{s^+}$) and completing
+        the circuit with a return electrode at ($r_{s^-}$).
+        [>]{This is an extra sentence that is just a side note.}
+
+        [ programmer ]{
+
+
+            [>tabs(language)]{
+
+                [ language == "python" ]{
+
+                    ```python
+                    from SimPEG import *
+                    ```
+
+                }
+
+                [ language == "javascript" ]{
+
+                    ```javascript
+
+
+                    ```
+
+                }
+
+            }
+
+            [>warn]{
+                This is a warning.
+            }
+
+            [>outline]{
+                * One
+                * two
+                    * {{ dc.view.title }}
+            }
+
+            [>purpose]{
+                I am trying to give a bit of an overview of DC resistivity.
+            }
+
+        }
+        Conservation of charge (which can be derived by
+        taking the divergence of Ampere’s law at steady state) connects the divergence of the current density
+        everywhere in space to the source term, consisting of two point sources, essentially charges, one
+        positive and one negative.
+        [+]{
+            Sometimes you want to write more inline.
+
+        }
+        The flow of current sets up electric fields according to [Ohm’s law](@bricks:geosci/em#ohms_law), which
+        relates current density to electric fields through the subsurface electrical conductivity {{ @cockett2015; @heagySEG }}. From
+        static Faraday’s law, we can describe the [electric field](@wikipedia) in terms of a scalar potential, $\phi$,
+        which we sample at potential electrodes to obtain data (potential differences).
+    }
+}
+
+You can see in section {{ dc.view.number }} the explanation!
+Please note that you may need to click this button to see all of the text {{ icare_5.view.button }}.
+
+In the figure below we can see that the block is [ sigma <= 1e0 ]{ resistive } [ sigma > 1e0 ]{ conductive } because
+$ \sigma = {{ sigma.format }} $. Remember this is an interactive document, so you can set $\sigma$ directly and the image below
+will update:
+
+ * Block Conductivity ({{ sigma.units }}): {{ sigma.view.slider }}
+ * Background Conductivity ({{ background.units }}): {{ background.view.slider }}
+
+![The potential, $\phi$, of a block in a half space.]({{ dcimage }})
+
+{{ = log(sigma) }}
+{{ = mesh.nC + 1 }}
+
+{{ dc-res.electrode_1.x.view.slider }}
+
+<#app>{{ dc-res }}
+
+{{ dc-res#maxwell_time }}
+
+{{ @bricks:gjqsdckj123kl }}
+
+
+{{ @bricks:gjhasdf234 }}
+
+
+
+{{ vid1 }}
+[= 25 < vid1.progress < 35 ]{
+
+    The world needs to see EM
+
+}
+
+
+[+]{
+
+    By functions we mean anything that we can represent on the mesh:
+
+    For example:
+
+        *
+}
+
+
+Define a comment symbol.
+
+
+Inline references with a reason.
+
+
+## `[arg]{ content }`
+
+[+]{ more detail }                                      Gives more detail about a certain topic
+[>sidenote]{ content }                                  Puts a side-note in the margin
+[>comment]{ @bricks:comment:io123b2jnv9 }               Reference to a comment stream
+[>command]{ content }                                   Simple command around content
+[>command(arg1, arg2, ... )]{ content }                 Argumentative command around content
+[= prop > 2 ]{ content }                                Evaluative command to boolean which shows the content
+
+
+## `{{ insert }}`
+
+{{ property }}                                          Inject the property value
+{{ property.attribute }}                                Inject the attribute of the property
+{{ @citeKey1, @bricks:cite:789123 }}                    Inject a reference
+
+## Extended markdown
+content $ma^{th}$ content                               In-line math
+
+
+## Examples:
+
+### `>command`:
+[>math(name="myeq")]{ma^{th}}                           Equation block
+[>image(url="myeq")]{ma^{th}}                           Equation block
+[>anchor("my-tag")]{ content }                          Anchors a block of content
+[>ref("cockett2015", reason="", name="")]{ content }    This should create a citation annotation
+H[>sub]{2}O                                             Subscript
+[>sub]{2}                                               Superscript
+
+
+#### These are pluggable:
+[>@bricks:rfm/bio-tagger("uid")]{ Mouse }               For example, creating a biological tag to another service.
+
+