diff --git a/doc/sphinx/apiFortran/timeAdvLinear.rst b/doc/sphinx/apiFortran/timeAdvLinear.rst
index 97458562..c94b3a4f 100644
--- a/doc/sphinx/apiFortran/timeAdvLinear.rst
+++ b/doc/sphinx/apiFortran/timeAdvLinear.rst
@@ -38,7 +38,6 @@ Linear calculation part of the time stepping (LMLoop)
 
 .. f:automodule:: updateb_mod
 
-
 ``updatePHI.f90``
 ------------------
 
diff --git a/doc/sphinx/apiPython/misc.rst b/doc/sphinx/apiPython/misc.rst
index a3e8e833..89f36161 100644
--- a/doc/sphinx/apiPython/misc.rst
+++ b/doc/sphinx/apiPython/misc.rst
@@ -23,3 +23,8 @@ Additional possible analyses
    :members:
    :private-members:
    :special-members:
+
+.. autoclass:: magic.libmelt
+   :members:
+   :private-members:
+   :special-members:
diff --git a/doc/sphinx/inputNamelists/controlNamelist.rst b/doc/sphinx/inputNamelists/controlNamelist.rst
index a0523cdb..940238ee 100644
--- a/doc/sphinx/inputNamelists/controlNamelist.rst
+++ b/doc/sphinx/inputNamelists/controlNamelist.rst
@@ -364,4 +364,4 @@ Miscellaneous
    | mpi_packing='single'   | Transpose each field individually                |
    +------------------------+--------------------------------------------------+
 
-* **l_adv_curl** (default :f:var:`l_adv_curl=.false. <l_adv_curl>`) is a logical. When set to True, the advection term is treated as :math:`\vec{u}\times\vec{\omega}` instead of :math:`\vec{u}\vec{\nabla}\vec{u}`. The practical consequence of that is to reduce the number of spectral/spatial Spherical Harmonic Transforms and hence to speed-up the code. Because of the treatment of the viscous heating term in the anelastic approximation, this is only an option when considering Boussinesq models.
+* **l_adv_curl** (default :f:var:`l_adv_curl=.true. <l_adv_curl>`) is a logical. When set to True, the advection term is treated as :math:`\vec{u}\times\vec{\omega}` instead of :math:`\vec{u}\vec{\nabla}\vec{u}`. The practical consequence of that is to reduce the number of spectral/spatial Spherical Harmonic Transforms and hence to speed-up the code. Because of the treatment of the viscous heating term in the anelastic approximation, this is only an option when considering Boussinesq models.