Re-export everything

content/article/mcinroy99_dynam.md

@@ -53,7 +53,7 @@ In order to provide low frequency passive vibration isolation, the hard actuator
 <a id="table--tab:mcinroy99-strut-model"></a>
 <div class="table-caption">
   <span class="table-number"><a href="#table--tab:mcinroy99-strut-model">Table 1</a>:</span>
-  Definition of quantities on <a href="#orgfe6d4ea">2</a>
+  Definition of quantities on <a href="#orgf3f08ed">2</a>
 </div>
 
 | **Symbol**                   | **Meaning**                                |
@@ -142,7 +142,7 @@ where:
 -   \\(\mathcal{F}\_e\\) represents a vector of exogenous generalized forces applied at the center of mass
 -   \\(g\\) is the gravity vector
 
-By combining \ref{eq:strut\_dynamics\_vec}, \ref{eq:payload\_dynamics} and \ref{eq:generalized\_force}, a single equation describing the dynamics of a flexure jointed hexapod can be found:
+By combining \eqref{eq:strut\_dynamics\_vec}, \eqref{eq:payload\_dynamics} and \eqref{eq:generalized\_force}, a single equation describing the dynamics of a flexure jointed hexapod can be found:
 
 \begin{aligned}
   & {}^UJ^T [ f\_m - M\_s \ddot{l} - B \dot{l} - K(l - l\_r) - M\_s \ddot{q}\_u\\\\