Fixing docs for PDF build (#1574)

doc/developer/guide.rst

@@ -33,7 +33,7 @@ of this hierarchy using the :py:mod:`armi.reactor.parameters` system to contain
 .. figure:: /.static/armi_reactor_objects.png
     :align: center
 
-    **Figure 1.** The primary data containers in ARMI
+    The primary data containers in ARMI
 
 Each level of the composite pattern hierarchy contains most of its state data in a
 collection of parameters detailing considerations of how the reactor has progressed
@@ -206,7 +206,7 @@ interface stack is traversed in order.
 .. figure:: /.static/armi_general_flowchart.png
     :align: center
 
-    **Figure 1.** The computational flow of the interface hooks
+    The computational flow of the interface hooks
 
 For example, input checking routines would run at beginning-of-life (BOL), calculation
 modules might run at every time node, etc. To accommodate these various needs, interface

doc/developer/profiling.rst

@@ -19,4 +19,4 @@ This produces images like this:
 .. figure:: /.static/buildMacros.png
     :align: center
 
-    **Figure 1.** An example of the profiler output rendered to a png.
+    An example of the profiler output rendered to a png.

doc/tutorials/walkthrough_lwr_inputs.rst

@@ -222,7 +222,7 @@ This should show a simple representation of the block.
 .. figure:: https://terrapower.github.io/armi/_static/c5g7-mox.png
    :figclass: align-center
 
-   **Figure 1.** A representation of a C5G7 fuel assembly. 
+   A representation of a C5G7 fuel assembly.
 
 
 Here are the full files used in this example:

doc/user/inputs.rst

@@ -456,7 +456,7 @@ The ARMI data model is represented schematically below, and the blueprints are d
 .. figure:: /.static/armi_reactor_objects.png
     :align: center
 
-    **Figure 1.** The primary data containers in ARMI
+    The primary data containers in ARMI
 
 :ref:`blocks <blocks-and-components>`:
     Defines :py:class:`~armi.reactor.components.component.Component` inputs for a

doc/user/physics_coupling.rst

@@ -75,4 +75,4 @@ These assembly-wise convergence parameters are then stored in an array of conver
 The total convergence of the power distribution is finally measured through the infinity norm (i.e, the max) of :math:`\xi`,
 
 .. math::
-    \epsilon = \| \xi \|_\inf = \max \xi.
+    \epsilon = \| \xi \|_{\inf} = \max \xi.

doc/user/radial_and_axial_expansion.rst

@@ -23,28 +23,28 @@ where, :math:`\Delta L` and :math:`\Delta T` are the change in length and temper
 Given Equation :eq:`linearExp`, we can create expressions for the change in length between our "hot" temperature (Equation :eq:`hotExp`)
 
 .. math::
-    \begin{align}
+    \begin{aligned}
         \frac{L_h - L_0}{L_0} &= \alpha(T_h)\left(T_h - T_0\right),\\
         \frac{L_h}{L_0} &= 1 + \alpha(T_h)\left(T_h - T_0\right).
-    \end{align}
+    \end{aligned}
     :label: hotExp
 
 and "non-reference" temperature, :math:`T_c` (Equation :eq:`nonRefExp`),
 
 .. math::
-    \begin{align}
+    \begin{aligned}
         \frac{L_c - L_0}{L_0} &= \alpha(T_c)\left(T_c - T_0\right),\\
         \frac{L_c}{L_0} &= 1 + \alpha(T_c)\left(T_c - T_0\right).
-    \end{align}
+    \end{aligned}
     :label: nonRefExp
 
 These are used within ARMI to enable thermal expansion and contraction with a temperature not equal to the reference temperature, :math:`T_0`. By taking the difference between Equation :eq:`hotExp` and :eq:`nonRefExp`, we can obtain an expression relating the change in length, :math:`L_h - L_c`, to the reference length, :math:`L_0`,
 
 .. math::
-    \begin{align}
+    \begin{aligned}
         \frac{L_h - L_0}{L_0} - \frac{L_c - L_0}{L_0} &= \frac{L_h}{L_0} - 1 - \frac{L_c}{L_0} + 1, \\
         &= \frac{L_h - L_c}{L_0}.
-    \end{align}
+    \end{aligned}
     :label: diffHotNonRef
 
 Using Equations :eq:`diffHotNonRef` and :eq:`nonRefExp`, we can obtain an expression for the change in length, :math:`L_h - L_c`, relative to the non-reference temperature,