3-NIRVANA-user-guide/3.2-User-interfaces.md

@@ -983,11 +983,10 @@ and *Δ*<sub>iz</sub> are given by
 and (*Â*<sub>*x*</sub>, *Â*<sub>*y*</sub>, *Â*<sub>*z*</sub>) 
 are the cell-edge integrals
 
-![ic_A](uploads/d7670a3203d0f3a1e2a9a759e69e2e77/ic_A.png)  
+![ic_A](uploads/d7670a3203d0f3a1e2a9a759e69e2e77/ic_A.png){width=300px}  
 
-The  *Â*'s
-The $\hat{A}$'s are usually easier to compute than the face-averaged
-magnetic field components directly. Even if the $\hat{A}$'s are
+The  *Â*'s are usually easier to compute than the face-averaged
+magnetic field components directly. Even if the  *Â*'s are
 approximated but otherwise set *unambiguously* on cell edges in the grid
 hierarchy, the magnetic field derived from the above discrete curl of
 vector potential has a divergence-free mesh representation.