From 9589967c406bc2c6f6681ab36ee733eee9bb7bfe Mon Sep 17 00:00:00 2001 From: David Wells Date: Fri, 25 Mar 2022 10:57:27 -0400 Subject: [PATCH] Fix some typos in the source file. --- examples/step-81/step-81.cc | 14 +++++++------- 1 file changed, 7 insertions(+), 7 deletions(-) diff --git a/examples/step-81/step-81.cc b/examples/step-81/step-81.cc index 0fbf4fd6d9..5d4c4932f1 100644 --- a/examples/step-81/step-81.cc +++ b/examples/step-81/step-81.cc @@ -19,8 +19,8 @@ // @sect3{Include files} -// The set of include files is quite standard. The most notable incluse is -// the fe/fe_nedelec_sz.h file that allows us to use the FE_NedelecSZ elements. +// The set of include files is quite standard. The most notable include is +// the fe/fe_nedelec_sz.h file which allows us to use the FE_NedelecSZ elements. // This is an implementation of the $H^{curl}$ conforming Nédélec Elements // that resolves the sign conflict issues that arise from parametrization. @@ -84,12 +84,12 @@ namespace Step81 // More explanation on the use and inheritance from the ParameterAcceptor // can be found in step-60. - // epsilon is the Electric Permitivitty coefficient and it is a rank 2 tensor. + // epsilon is the Electric Permittivity coefficient and it is a rank 2 tensor. // Depending on the material, we assign the i^th diagonal element of the // tensor to the material epsilon value (one of the private epsilon_1_ or // epsilon_2_ variables). // - // mu_inv is the inverese of the Magnetic Permiabillity coefficient and it is + // mu_inv is the inverse of the Magnetic Permiability coefficient and it is // a complex number. // sigma is the Surface Conductivity coefficient between material left and @@ -375,7 +375,7 @@ namespace Step81 // At this point we are ready to instantiate all the major functions of // the finite element program and also a list of variables. Most of these // an exact copy of the functions in the tutorial programs. In addition, - // we instatiate the parameters and the perfectly matched layer. The + // we instantiate the parameters and the perfectly matched layer. The // default values of these parameters are set to show us a standing wave // with absorbing boundary conditions and a PML. @@ -419,7 +419,7 @@ namespace Step81 // @sect4{The Constructor} // The Constructor simply consists specifications for the mesh - // and the order of the fnite elements. These are editable through + // and the order of the finite elements. These are editable through // the .prm file. The absorbing_boundary boolean can be modified to // remove the absorbing boundary conditions (in which case our boundary // would be perfectly conducting). @@ -601,7 +601,7 @@ namespace Step81 // \f} // In doing so, we need test functions $\phi_i$ and $\phi_j$, and the curl // of these test variables. We must be careful with the signs of the - // imaginary parts of these comples test variables. Moreover, we have a + // imaginary parts of these complex test variables. Moreover, we have a // conditional that changes the parameters if the cell is in the PML region. for (const auto &cell : dof_handler.active_cell_iterators()) { -- 2.39.5