diff --git a/docs/source/methods/introduction.rst b/docs/source/methods/introduction.rst
index 0bd067470c..dab1c544ad 100644
--- a/docs/source/methods/introduction.rst
+++ b/docs/source/methods/introduction.rst
@@ -124,7 +124,7 @@ proceed. The life of a single particle will proceed as follows:
      continuous-energy simulation, reactions of type :math:`(n,xn)` are treated
      as scattering and any additional particles which may be created are added
      to a secondary particle bank to be tracked later. In a multi-group
-     simulation, this secondary bank is ont used but the particle weight is
+     simulation, this secondary bank is not used but the particle weight is
      increased accordingly.  The original particle then continues from step 3.
      If the reaction is absorption or fission, the particle dies and if
      necessary, fission sites are created and stored in the fission bank.
diff --git a/docs/source/methods/physics.rst b/docs/source/methods/physics.rst
index bb26ffec53..b246584c8b 100644
--- a/docs/source/methods/physics.rst
+++ b/docs/source/methods/physics.rst
@@ -8,7 +8,7 @@ There are limited differences between physics treatments used in the
 continuous-energy and multi-group modes.  If distinctions are necessary, each
 of the following sections will provide an explanation of the differences.
 Otherwise, replacing any references of the particle's energy (`E`) with
-references to the particle's energy group (`g) will suffice.
+references to the particle's energy group (`g`) will suffice.
 
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 Sampling Distance to Next Collision