fixed some movie links in wave chapter

Author: sveinlin

doc/.src/chapters/mako_code.txt

@@ -33,8 +33,12 @@ doc = 'http://htmlpreview.github.io/?https://github.com/slgit/fdm-book-mov/blob/
 doc = 'http://tinyurl.com/gmw2yrj'
 
 # For movies:
-docraw = 'https://raw.githubusercontent.com/hplgit/fdm-book/master/doc/.src/book/'
-docraw = 'http://tinyurl.com/hfdndao'
+# 24jan2017, HP original lines:
+# docraw = 'https://raw.githubusercontent.com/hplgit/fdm-book/master/doc/.src/book/'
+# docraw = 'http://tinyurl.com/hfdndao'
+docraw = 'https://raw.githubusercontent.com/slgit/fdm-book-mov/master/'
+docraw = 'http://tinyurl.com/zeyvdse'
+
 
 #writing_reports = 'http://hplgit.github.io/teamods/writing_reports'
 writing_reports = 'http://tinyurl.com/nc4upel'

doc/.src/chapters/wave/wave1D_fd1.do.txt

@@ -361,9 +361,9 @@ We can now summarize the computational algorithm:
 The algorithm essentially consists of moving a finite difference
 stencil through all the mesh points, which can be seen as an animation
 in a "web page":
-"${doc_notes}/pub/wave/html/mov-wave/D_stencil_gpl/index.html"
+"${doc_notes}/mov-wave/D_stencil_gpl/index.html"
 or a "movie file":
-"${doc_notes}/pub/wave/html/mov-wave/D_stencil_gpl/movie.ogg".
+"${docraw}/mov-wave/D_stencil_gpl/movie.ogg".
 
 
 ===== Sketch of an implementation =====

doc/pub/book/pdf/fdm-book-4print.pdf

@@ -724,7 +724,7 @@
 <center>[3] <b>Department of Process, Energy and Environmental Technology, University College of Southeast Norway</b></center>
 <br>
 <p>
-<center><h4>Jan 21, 2017</h4></center> <!-- date -->
+<center><h4>Jan 24, 2017</h4></center> <!-- date -->
 <br>
 <p>
 <!-- Externaldocuments: ../../../../../decay-book/doc/.src/book/book, ../vib/main_vib, ../../../../../scaling-book/doc/.src/book -->

doc/pub/book/pdf/fdm-book-4screen-sol.pdf

@@ -1059,8 +1059,8 @@ <h2 id="wave:string:alg">Formulating a recursive algorithm</h2>
 
 The algorithm essentially consists of moving a finite difference
 stencil through all the mesh points, which can be seen as an animation
-in a <a href="http://tinyurl.com/pu5uyfn/pub/pub/wave/html/mov-wave/D_stencil_gpl/index.html" target="_self">web page</a>
-or a <a href="http://tinyurl.com/pu5uyfn/pub/pub/wave/html/mov-wave/D_stencil_gpl/movie.ogg" target="_self">movie file</a>.
+in a <a href="http://tinyurl.com/gmw2yrj/mov-wave/D_stencil_gpl/index.html" target="_self">web page</a>
+or a <a href="http://tinyurl.com/gmw2yrj/mov-wave/D_stencil_gpl/movie.ogg" target="_self">movie file</a>.
 
 <h2 id="wave:string:impl">Sketch of an implementation</h2>
 

doc/pub/book/pdf/fdm-book-4screen.pdf

@@ -1329,7 +1329,7 @@ <h2 id="wave:pde1:guitar:data">Running a case</h2>
 </pre></div>
 <p>
 The associated program has the name <a href="http://tinyurl.com/nu656p2/wave/wave1D/wave1D_u0.py" target="_self"><tt>wave1D_u0.py</tt></a>. Run
-the program and watch the <a href="http://tinyurl.com/pu5uyfn/pub/pub/wave/html/mov-wave/guitar_C0.8/movie.html" target="_self">movie of the vibrating string</a>.
+the program and watch the <a href="http://tinyurl.com/gmw2yrj/pub/wave/html/mov-wave/guitar_C0.8/movie.html" target="_self">movie of the vibrating string</a>.
 The string should ideally consist of straight segments, but these are
 somewhat wavy due to numerical approximation. Run the case with the
 <code>wave1D_u0.py</code> code and \( C=1 \) to see the exact solution.

doc/pub/wave/html/._wave-sol000.html

@@ -705,8 +705,8 @@ <h1 id="wave:pde2:Neumann">Generalization: reflecting boundaries</h1>
 <p>
 The boundary condition \( u=0 \) in a wave equation reflects the wave, but
 \( u \) changes sign at the boundary, while the condition \( u_x=0 \) reflects
-the wave as a mirror and preserves the sign, see a <a href="http://tinyurl.com/pu5uyfn/pub/pub/wave/html/mov-wave/demo_BC_gaussian/index.html" target="_self">web page</a> or a
-<a href="http://tinyurl.com/pu5uyfn/pub/pub/wave/html/mov-wave/demo_BC_gaussian/movie.flv" target="_self">movie file</a> for
+the wave as a mirror and preserves the sign, see a <a href="http://tinyurl.com/gmw2yrj/pub/wave/html/mov-wave/demo_BC_gaussian/index.html" target="_self">web page</a> or a
+<a href="http://tinyurl.com/gmw2yrj/pub/wave/html/mov-wave/demo_BC_gaussian/movie.flv" target="_self">movie file</a> for
 demonstration.
 
 <p>
@@ -836,8 +836,8 @@ <h2 id="wave:pde2:Neumann:discr">Discretization of derivatives at the boundary</
 The modification of the scheme at the boundary is also required for
 the special formula for the first time step. How the stencil moves
 through the mesh and is modified at the boundary can be illustrated by
-an animation in a <a href="http://tinyurl.com/pu5uyfn/pub/pub/wave/html/mov-wave/N_stencil_gpl/index.html" target="_self">web page</a>
-or a <a href="http://tinyurl.com/pu5uyfn/pub/pub/wave/html/mov-wave/N_stencil_gpl/movie.ogg" target="_self">movie file</a>.
+an animation in a <a href="http://tinyurl.com/gmw2yrj/pub/wave/html/mov-wave/N_stencil_gpl/index.html" target="_self">web page</a>
+or a <a href="http://tinyurl.com/gmw2yrj/pub/wave/html/mov-wave/N_stencil_gpl/movie.ogg" target="_self">movie file</a>.
 
 <h2 id="wave:pde2:Neumann:impl">Implementation of Neumann conditions</h2>
 

doc/pub/wave/html/._wave-sol001.html

@@ -583,7 +583,7 @@
 <center>[3] <b>Department of Process, Energy and Environmental Technology, University College of Southeast Norway</b></center>
 <br>
 <p>
-<center><h4>Jan 21, 2017</h4></center> <!-- date -->
+<center><h4>Jan 24, 2017</h4></center> <!-- date -->
 <br>
 <p>
 <!-- Externaldocuments: ../../../../../decay-book/doc/.src/book/book, ../vib/main_vib, ../../../../../scaling-book/doc/.src/book -->