doc typos

jdevemy · Jul 26, 2015 · 027fc8b · 027fc8b
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diff --git a/doc/Section_howto.html b/doc/Section_howto.html
@@ -2430,7 +2430,7 @@ <H5>Example calculations with chunks
 <A HREF = "#howto_26">CORESHELL</A> package, 
 
 <LI>the thermalized Drude dipole method, implemented in the
-<A HREF = "#howto_26">USER-DRUDE</A> package. 
+<A HREF = "#howto_27">USER-DRUDE</A> package. 
 </UL>
 <P>The fluctuating charge method calculates instantateous charges on
 interacting atoms based on the electronegativity equalization
@@ -2466,7 +2466,7 @@ <H5>Example calculations with chunks
 timestep. In the fluctuating charge scheme this is done by the matrix
 inversion method in <A HREF = "fix_qeq.html">fix qeq/point</A>, but for core-shell
 or Drude-dipoles the relaxed-dipoles technique would require an slow
-iterative procedure. These self-consistent solutions yield accurae
+iterative procedure. These self-consistent solutions yield accurate
 trajectories since the additional degrees of freedom representing
 polarization are massless.  An alternative is to attribute a mass to
 the additional degrees of freedom and perform time integration using

diff --git a/doc/Section_howto.txt b/doc/Section_howto.txt
@@ -2413,7 +2413,7 @@ package, :ulb,l
 the adiabatic core-shell method, implemented in the
 "CORESHELL"_#howto_26 package, :l
 the thermalized Drude dipole method, implemented in the
-"USER-DRUDE"_#howto_26 package. :l,ule
+"USER-DRUDE"_#howto_27 package. :l,ule
 
 The fluctuating charge method calculates instantateous charges on
 interacting atoms based on the electronegativity equalization
@@ -2449,7 +2449,7 @@ self-consistent calculation of charges or induced dipoles at each
 timestep. In the fluctuating charge scheme this is done by the matrix
 inversion method in "fix qeq/point"_fix_qeq.html, but for core-shell
 or Drude-dipoles the relaxed-dipoles technique would require an slow
-iterative procedure. These self-consistent solutions yield accurae
+iterative procedure. These self-consistent solutions yield accurate
 trajectories since the additional degrees of freedom representing
 polarization are massless.  An alternative is to attribute a mass to
 the additional degrees of freedom and perform time integration using