updated some links

Author: sveinlin

doc/.src/chapters/advec/advec.do.txt

@@ -265,7 +265,7 @@ which results in the updating formula
 !et
 A special scheme is needed to compute $u^1$, but we leave that problem for
 now. Anyway, this special scheme can be found in 
-"`advec1D.py`": "$https://github.com/hplgit/fdm-book/blob/master/src/advec/advec1D.py".
+"`advec1D.py`": "${src_advec}/advec1D.py".
 
 === Implementation ===
 
@@ -724,7 +724,7 @@ def run(scheme='UP', case='gaussian', C=1, dt=0.01):
     print 'Integral of u:', integral.max(), integral.min()
 !ec
 The complete code is found in the file
-"`advec1D.py`": "$https://github.com/hplgit/fdm-book/blob/master/src/advec/advec1D.py".
+"`advec1D.py`": "${src_advec}/advec1D.py".
 
 ===== A Crank-Nicolson discretization in time and centered differences in space =====
 label{advec:1D:CN}

doc/.src/chapters/softeng2/softeng2.do.txt

@@ -86,7 +86,7 @@ The general initial-boundary value problem
 (ref{wave:pde2:software:ueq2})-(ref{wave:pde2:software:bcL2})
 solved by finite difference methods can be implemented as shown in
 the following `solver` function (taken from the
-file "`wave1D_dn_vc.py`": "${src_wave}/wave1D/wave_dn_vc.py").
+file "`wave1D_dn_vc.py`": "${src_wave}/wave1D/wave1D_dn_vc.py").
 This function builds on
 simpler versions described in
 ref[Sections ref{wave:pde1:impl}, ref{wave:pde1:impl:vec}
@@ -269,7 +269,7 @@ Such actions must be
 taken care of outside the `solver` function, more precisely in the
 `user_action` function that is called at every time level.
 
-We have, in the "`wave1D_dn_vc.py`": "${src_wave}/wave1D/wave_dn_vc.py"
+We have, in the "`wave1D_dn_vc.py`": "${src_wave}/wave1D/wave1D_dn_vc.py"
 code, implemented the `user_action`
 callback function as a class `PlotAndStoreSolution` with a
 `__call__(self, x, t, t, n)` method for the `user_action` function.
@@ -343,7 +343,7 @@ resulting archive file with all solutions, is supposed to be a
 hash reflecting all import parameters in the problem such that this
 simulation has a unique name.
 The `hashed_input` string is made in the "`solver`":
-"${src_wave}/wave1D/wave_dn_vc.py" function, using the `hashlib`
+"${src_wave}/wave1D/wave1D_dn_vc.py" function, using the `hashlib`
 and `inspect` modules, based on the arguments to `solver`:
 
 !bc pycod
@@ -448,7 +448,7 @@ $u(x,t) = \cos(\frac{2\pi}{L}t)\sin(\frac{2\pi}{L}x)$. The call will
 be very similar to the one provided in the `test_convrate_sincos` function
 in ref[Section ref{wave:pde1:impl:verify:rate}][ in cite{Langtangen_deqbook_wave}][the section "Verification: convergence rates": "" in
 cite{Langtangen_deqbook_wave}], see the file "`wave1D_dn_vc.py`":
-"${src_wave}/wave1D/wave_dn_vc.py" for details.
+"${src_wave}/wave1D/wave1D_dn_vc.py" for details.
 
 
 ======= Programming the solver with classes =======
@@ -821,7 +821,7 @@ idx{Fortran subroutine}
 idx{`wave2D_u0_loop_f77.f`}
 
 We write a Fortran subroutine `advance` in a file
-"`wave2D_u0_loop_f77.f`": "${src_wave}/wave2D_u0/wave2D_u0_loop_f77.f"
+"`wave2D_u0_loop_f77.f`": "${src_softeng2}/wave2D_u0_loop_f77.f"
 for implementing the updating formula
 (ref{wave:2D3D:impl1:2Du0:ueq:discrete}) and setting the solution to zero
 at the boundaries:

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

@@ -255,7 +255,7 @@
 <center>[3] <b>Department of Process, Energy and Environmental Technology, University College of Southeast Norway</b></center>
 <br>
 <p>
-<center><h4>Dec 23, 2016</h4></center> <!-- date -->
+<center><h4>Aug 15, 2017</h4></center> <!-- date -->
 <br>
 <p>
 <!-- Externaldocuments: ../wave/main_wave -->
@@ -340,7 +340,7 @@ <h2>Table of contents</h2>
 
 
 <center style="font-size:80%">
-<!-- copyright --> &copy; 2016, Hans Petter Langtangen, Svein Linge. Released under CC Attribution 4.0 license
+<!-- copyright --> &copy; 2017, Hans Petter Langtangen, Svein Linge. Released under CC Attribution 4.0 license
 </center>
 
 

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

@@ -215,7 +215,7 @@
 <center>[3] <b>Department of Process, Energy and Environmental Technology, University College of Southeast Norway</b></center>
 <br>
 <p>
-<center><h4>Dec 23, 2016</h4></center> <!-- date -->
+<center><h4>Aug 15, 2017</h4></center> <!-- date -->
 <br>
 <p>
 <!-- Externaldocuments: ../wave/main_wave -->
@@ -286,7 +286,7 @@ <h2>Table of contents</h2>
 
 
 <center style="font-size:80%">
-<!-- copyright --> &copy; 2016, Hans Petter Langtangen, Svein Linge. Released under CC Attribution 4.0 license
+<!-- copyright --> &copy; 2017, Hans Petter Langtangen, Svein Linge. Released under CC Attribution 4.0 license
 </center>
 
 

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

@@ -255,7 +255,7 @@
 <center>[3] <b>Department of Process, Energy and Environmental Technology, University College of Southeast Norway</b></center>
 <br>
 <p>
-<center><h4>Dec 23, 2016</h4></center> <!-- date -->
+<center><h4>Aug 15, 2017</h4></center> <!-- date -->
 <br>
 <p>
 <!-- Externaldocuments: ../wave/main_wave -->
@@ -340,7 +340,7 @@ <h2>Table of contents</h2>
 
 
 <center style="font-size:80%">
-<!-- copyright --> &copy; 2016, Hans Petter Langtangen, Svein Linge. Released under CC Attribution 4.0 license
+<!-- copyright --> &copy; 2017, Hans Petter Langtangen, Svein Linge. Released under CC Attribution 4.0 license
 </center>