From fd1f6ed2186f4e7d3da9d82f3e4617a13c52089b Mon Sep 17 00:00:00 2001 From: Philipp Edelmann Date: Wed, 19 Jun 2024 23:31:56 -0600 Subject: [PATCH] fix typos --- doc/source/User_Guide/model_setup.rst | 4 ++-- 1 file changed, 2 insertions(+), 2 deletions(-) diff --git a/doc/source/User_Guide/model_setup.rst b/doc/source/User_Guide/model_setup.rst index 2c855cb9..1f012f4d 100644 --- a/doc/source/User_Guide/model_setup.rst +++ b/doc/source/User_Guide/model_setup.rst @@ -404,7 +404,7 @@ to consider whether it makes sense to separately initialize the spherically-symmetric component of the thermal field with a profile that is in conductive balance. This is almost certainly the case when running with fixed temperature conditions. The logical namelist variable -``conductive_profile`` can be used for this purpose. It’s default value +``conductive_profile`` can be used for this purpose. Its default value is ``.false.`` (off), and its value is ignored completely when restarting from a checkpoint. To initialize a simulation with a random temperature field superimposed on a spherically-symmetric, conductive background @@ -453,7 +453,7 @@ vector-potential functions are given a random power distribution described by Equation eq_init_. Each mode’s random amplitude is then determined by namelist variable ``mag_amp``. This variable should be interpreted as an approximate magnetic field strength -(it’s value is rescaled appropriately for the poloidal and toroidal +(its value is rescaled appropriately for the poloidal and toroidal vector potentials, which are differentiated to yield the magnetic field).