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📁 一个用来实现偏微分方程中网格的计算库
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</pre></div><div class = "comment">The element shape function gradients evaluated at the quadraturepoints.</div><div class ="fragment"><pre>          const std::vector&lt;std::vector&lt;RealGradient&gt; &gt;& dphi = fe-&gt;get_dphi();        </pre></div><div class = "comment">The XY locations of the quadrature points used for face integration</div><div class ="fragment"><pre>          const std::vector&lt;Point&gt;& qface_points = fe_face-&gt;get_xyz();            </pre></div><div class = "comment">A reference to the \p DofMap object for this system.  The \p DofMapobject handles the index translation from node and element numbersto degree of freedom numbers.  We will talk more about the \p DofMapin future examples.</div><div class ="fragment"><pre>          const DofMap& dof_map = system.get_dof_map();          </pre></div><div class = "comment">Define data structures to contain the element matrixand right-hand-side vector contribution.  Followingbasic finite element terminology we will denote these"Ke" and "Fe".</div><div class ="fragment"><pre>          DenseMatrix&lt;Number&gt; Ke;          DenseVector&lt;Number&gt; Fe;          </pre></div><div class = "comment">This vector will hold the degree of freedom indices forthe element.  These define where in the global systemthe element degrees of freedom get mapped.</div><div class ="fragment"><pre>          std::vector&lt;unsigned int&gt; dof_indices;        </pre></div><div class = "comment">Here we extract the velocity & parameters that we put in theEquationSystems object.</div><div class ="fragment"><pre>          const RealVectorValue velocity =            es.parameters.get&lt;RealVectorValue&gt; ("velocity");                  const Real dt = es.parameters.get&lt;Real&gt;   ("dt");          const Real time = es.parameters.get&lt;Real&gt; ("time");        </pre></div><div class = "comment">Now we will loop over all the elements in the mesh thatlive on the local processor. We will compute the elementmatrix and right-hand-side contribution.  Since the meshwill be refined we want to only consider the ACTIVE elements,hence we use a variant of the \p active_elem_iterator.</div><div class ="fragment"><pre>          MeshBase::const_element_iterator       el     = mesh.active_local_elements_begin();          const MeshBase::const_element_iterator end_el = mesh.active_local_elements_end();                     for ( ; el != end_el; ++el)            {    </pre></div><div class = "comment">Store a pointer to the element we are currentlyworking on.  This allows for nicer syntax later.</div><div class ="fragment"><pre>              const Elem* elem = *el;              </pre></div><div class = "comment">Get the degree of freedom indices for thecurrent element.  These define where in the globalmatrix and right-hand-side this element willcontribute to.</div><div class ="fragment"><pre>              dof_map.dof_indices (elem, dof_indices);        </pre></div><div class = "comment">Compute the element-specific data for the currentelement.  This involves computing the location of thequadrature points (q_point) and the shape functions(phi, dphi) for the current element.</div><div class ="fragment"><pre>              fe-&gt;reinit (elem);              </pre></div><div class = "comment">Zero the element matrix and right-hand side beforesumming them.  We use the resize member here becausethe number of degrees of freedom might have changed fromthe last element.  Note that this will be the case if theelement type is different (i.e. the last element was atriangle, now we are on a quadrilateral).</div><div class ="fragment"><pre>              Ke.resize (dof_indices.size(),        		 dof_indices.size());                      Fe.resize (dof_indices.size());              </pre></div><div class = "comment">Now we will build the element matrix and right-hand-side.Constructing the RHS requires the solution and itsgradient from the previous timestep.  This myst becalculated at each quadrature point by summing thesolution degree-of-freedom values by the appropriateweight functions.</div><div class ="fragment"><pre>              for (unsigned int qp=0; qp&lt;qrule.n_points(); qp++)        	{</pre></div><div class = "comment">Values to hold the old solution & its gradient.</div><div class ="fragment"><pre>                  Number   u_old = 0.;        	  Gradient grad_u_old;        	  </pre></div><div class = "comment">Compute the old solution & its gradient.</div><div class ="fragment"><pre>                  for (unsigned int l=0; l&lt;phi.size(); l++)        	    {        	      u_old      += phi[l][qp]*system.old_solution  (dof_indices[l]);        	      </pre></div><div class = "comment">This will work,grad_u_old += dphi[l][qp]*system.old_solution (dof_indices[l]);but we can do it without creating a temporary like this:</div><div class ="fragment"><pre>                      grad_u_old.add_scaled (dphi[l][qp],system.old_solution (dof_indices[l]));        	    }        	  </pre></div><div class = "comment">Now compute the element matrix and RHS contributions.</div><div class ="fragment"><pre>                  for (unsigned int i=0; i&lt;phi.size(); i++)        	    {</pre></div><div class = "comment">The RHS contribution</div><div class ="fragment"><pre>                      Fe(i) += JxW[qp]*(</pre></div><div class = "comment">Mass matrix term</div><div class ="fragment"><pre>                                        u_old*phi[i][qp] +         				-.5*dt*(</pre></div><div class = "comment">Convection term(grad_u_old may be complex, so theorder here is important!)</div><div class ="fragment"><pre>                                                (grad_u_old*velocity)*phi[i][qp] +        					</pre></div><div class = "comment">Diffusion term</div><div class ="fragment"><pre>                                                0.01*(grad_u_old*dphi[i][qp]))             				);        	              	      for (unsigned int j=0; j&lt;phi.size(); j++)        		{</pre></div><div class = "comment">The matrix contribution</div><div class ="fragment"><pre>                          Ke(i,j) += JxW[qp]*(</pre></div><div class = "comment">Mass-matrix</div><div class ="fragment"><pre>                                              phi[i][qp]*phi[j][qp] +         				      .5*dt*(</pre></div><div class = "comment">Convection term</div><div class ="fragment"><pre>                                                     (velocity*dphi[j][qp])*phi[i][qp] +</pre></div><div class = "comment">Diffusion term</div><div class ="fragment"><pre>                                                     0.01*(dphi[i][qp]*dphi[j][qp]))              				      );        		}        	    }         	}         </pre></div><div class = "comment">At this point the interior element integration hasbeen completed.  However, we have not yet addressedboundary conditions.  For this example we will onlyconsider simple Dirichlet boundary conditions imposedvia the penalty method. <br><br>The following loops over the sides of the element.If the element has no neighbor on a side then thatside MUST live on a boundary of the domain.</div><div class ="fragment"><pre>              {</pre></div><div class = "comment">The penalty value.  </div><div class ="fragment"><pre>                const Real penalty = 1.e10;        </pre></div><div class = "comment">The following loops over the sides of the element.If the element has no neighbor on a side then thatside MUST live on a boundary of the domain.</div><div class ="fragment"><pre>                for (unsigned int s=0; s&lt;elem-&gt;n_sides(); s++)        	  if (elem-&gt;neighbor(s) == NULL)        	    {        	      fe_face-&gt;reinit(elem,s);        	              	      for (unsigned int qp=0; qp&lt;qface.n_points(); qp++)        		{        		  const Number value = exact_solution (qface_points[qp](0),        						       qface_points[qp](1),        						       time);        						       </pre></div><div class = "comment">RHS contribution</div><div class ="fragment"><pre>                          for (unsigned int i=0; i&lt;psi.size(); i++)        		    Fe(i) += penalty*JxW_face[qp]*value*psi[i][qp];        </pre></div><div class = "comment">Matrix contribution</div><div class ="fragment"><pre>                          for (unsigned int i=0; i&lt;psi.size(); i++)        		    for (unsigned int j=0; j&lt;psi.size(); j++)        		      Ke(i,j) += penalty*JxW_face[qp]*psi[i][qp]*psi[j][qp];        		}        	    }               }                       </pre></div><div class = "comment">We have now built the element matrix and RHS vector in termsof the element degrees of freedom.  However, it is possiblethat some of the element DOFs are constrained to enforcesolution continuity, i.e. they are not really "free".  We needto constrain those DOFs in terms of non-constrained DOFs toensure a continuous solution.  The\p DofMap::constrain_element_matrix_and_vector() method doesjust that.</div><div class ="fragment"><pre>              dof_map.constrain_element_matrix_and_vector (Ke, Fe, dof_indices);              </pre></div><div class = "comment">The element matrix and right-hand-side are now builtfor this element.  Add them to the global matrix andright-hand-side vector.  The \p PetscMatrix::add_matrix()and \p PetscVector::add_vector() members do this for us.</div><div class ="fragment"><pre>              system.matrix-&gt;add_matrix (Ke, dof_indices);              system.rhs-&gt;add_vector    (Fe, dof_indices);                          }</pre></div><div class = "comment">Finished computing the sytem matrix and right-hand side.</div><div class ="fragment"><pre>        #endif // #ifdef ENABLE_AMR        }</pre></div><a name="nocomments"></a> <br><br><br> <h1> The program without comments: </h1> <pre>      #include &lt;iostream&gt;  #include &lt;algorithm&gt;  #include &lt;cmath&gt;    #include <B><FONT COLOR="#BC8F8F">&quot;libmesh.h&quot;</FONT></B>  #include <B><FONT COLOR="#BC8F8F">&quot;mesh.h&quot;</FONT></B>  #include <B><FONT COLOR="#BC8F8F">&quot;mesh_refinement.h&quot;</FONT></B>  #include <B><FONT COLOR="#BC8F8F">&quot;gmv_io.h&quot;</FONT></B>  #include <B><FONT COLOR="#BC8F8F">&quot;equation_systems.h&quot;</FONT></B>  #include <B><FONT COLOR="#BC8F8F">&quot;fe.h&quot;</FONT></B>  #include <B><FONT COLOR="#BC8F8F">&quot;quadrature_gauss.h&quot;</FONT></B>  #include <B><FONT COLOR="#BC8F8F">&quot;dof_map.h&quot;</FONT></B>  #include <B><FONT COLOR="#BC8F8F">&quot;sparse_matrix.h&quot;</FONT></B>  #include <B><FONT COLOR="#BC8F8F">&quot;numeric_vector.h&quot;</FONT></B>  #include <B><FONT COLOR="#BC8F8F">&quot;dense_matrix.h&quot;</FONT></B>  #include <B><FONT COLOR="#BC8F8F">&quot;dense_vector.h&quot;</FONT></B>    #include <B><FONT COLOR="#BC8F8F">&quot;getpot.h&quot;</FONT></B>    #include <B><FONT COLOR="#BC8F8F">&quot;o_string_stream.h&quot;</FONT></B>    #include <B><FONT COLOR="#BC8F8F">&quot;transient_system.h&quot;</FONT></B>  #include <B><FONT COLOR="#BC8F8F">&quot;linear_implicit_system.h&quot;</FONT></B>  #include <B><FONT COLOR="#BC8F8F">&quot;vector_value.h&quot;</FONT></B>    #include <B><FONT COLOR="#BC8F8F">&quot;error_vector.h&quot;</FONT></B>  #include <B><FONT COLOR="#BC8F8F">&quot;kelly_error_estimator.h&quot;</FONT></B>    #include <B><FONT COLOR="#BC8F8F">&quot;elem.h&quot;</FONT></B>    <B><FONT COLOR="#228B22">void</FONT></B> assemble_cd (EquationSystems&amp; es,  		  <B><FONT COLOR="#228B22">const</FONT></B> std::string&amp; system_name);    <B><FONT COLOR="#228B22">void</FONT></B> init_cd (EquationSystems&amp; es,  	      <B><FONT COLOR="#228B22">const</FONT></B> std::string&amp; system_name);    Real exact_solution (<B><FONT COLOR="#228B22">const</FONT></B> Real x,  		     <B><FONT COLOR="#228B22">const</FONT></B> Real y,  		     <B><FONT COLOR="#228B22">const</FONT></B> Real t);    Number exact_value (<B><FONT COLOR="#228B22">const</FONT></B> Point&amp; p,  		    <B><FONT COLOR="#228B22">const</FONT></B> Parameters&amp; parameters,  		    <B><FONT COLOR="#228B22">const</FONT></B> std::string&amp;,  		    <B><FONT COLOR="#228B22">const</FONT></B> std::string&amp;)  {    <B><FONT COLOR="#A020F0">return</FONT></B> exact_solution(p(0), p(1), parameters.get&lt;Real&gt; (<B><FONT COLOR="#BC8F8F">&quot;time&quot;</FONT></B>));  }        <B><FONT COLOR="#228B22">int</FONT></B> main (<B><FONT COLOR="#228B22">int</FONT></B> argc, <B><FONT COLOR="#228B22">char</FONT></B>** argv)  {    <B><FONT COLOR="#5F9EA0">libMesh</FONT></B>::init (argc, argv);    #ifndef ENABLE_AMR    <B><FONT COLOR="#5F9EA0">std</FONT></B>::cerr &lt;&lt; <B><FONT COLOR="#BC8F8F">&quot;ERROR: This example requires libMesh to be\n&quot;</FONT></B>              &lt;&lt; <B><FONT COLOR="#BC8F8F">&quot;compiled with AMR support!&quot;</FONT></B>              &lt;&lt; std::endl;    <B><FONT COLOR="#A020F0">return</FONT></B> 0;  #<B><FONT COLOR="#A020F0">else</FONT></B>      {              <B><FONT COLOR="#5F9EA0">std</FONT></B>::cout &lt;&lt; <B><FONT COLOR="#BC8F8F">&quot;Usage:\n&quot;</FONT></B>        &lt;&lt;<B><FONT COLOR="#BC8F8F">&quot;\t &quot;</FONT></B> &lt;&lt; argv[0] &lt;&lt; <B><FONT COLOR="#BC8F8F">&quot; -init_timestep 0\n&quot;</FONT></B>        &lt;&lt; <B><FONT COLOR="#BC8F8F">&quot;OR\n&quot;</FONT></B>        &lt;&lt;<B><FONT COLOR="#BC8F8F">&quot;\t &quot;</FONT></B> &lt;&lt; argv[0] &lt;&lt; <B><FONT COLOR="#BC8F8F">&quot; -read_solution -init_timestep 26\n&quot;</FONT></B>        &lt;&lt; std::endl;        <B><FONT COLOR="#5F9EA0">std</FONT></B>::cout &lt;&lt; <B><FONT COLOR="#BC8F8F">&quot;Running: &quot;</FONT></B> &lt;&lt; argv[0];        <B><FONT COLOR="#A020F0">for</FONT></B> (<B><FONT COLOR="#228B22">int</FONT></B> i=1; i&lt;argc; i++)        <B><FONT COLOR="#5F9EA0">std</FONT></B>::cout &lt;&lt; <B><FONT COLOR="#BC8F8F">&quot; &quot;</FONT></B> &lt;&lt; argv[i];        <B><FONT COLOR="#5F9EA0">std</FONT></B>::cout &lt;&lt; std::endl &lt;&lt; std::endl;        GetPot command_line (argc, argv);          <B><FONT COLOR="#228B22">const</FONT></B> <B><FONT COLOR="#228B22">bool</FONT></B> read_solution   = command_line.search(<B><FONT COLOR="#BC8F8F">&quot;-read_solution&quot;</FONT></B>);  

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