Page MenuHomeFreeBSD

D61427.1794682299.diff
No OneTemporary

Authored By
Unknown
Size
4 KB
Referenced Files
None
Subscribers
None

D61427.1794682299.diff

diff --git a/science/code_saturne/files/patch-docs_theory_cfbase.tex b/science/code_saturne/files/patch-docs_theory_cfbase.tex
new file mode 100644
--- /dev/null
+++ b/science/code_saturne/files/patch-docs_theory_cfbase.tex
@@ -0,0 +1,18 @@
+--- docs/theory/cfbase.tex.orig 2023-12-10 13:11:41 UTC
++++ docs/theory/cfbase.tex
+@@ -196,7 +196,6 @@ pour des \'ecoulements compressibles.
+
+ \begin{equation}\label{Cfbl_Cfbase_eq_ref_laminaire_cfbase}
+ \left\{\begin{array}{l}
+-
+ \displaystyle\frac{\partial\rho}{\partial t} + \divs(\vect{Q}) = 0 \\
+ \\
+ \displaystyle\frac{\partial\vect{Q}}{\partial t}
+@@ -206,7 +205,6 @@ - \divs{\,\vect{\Phi}_s} + \rho\Phi_v
+ \displaystyle\frac{\partial E}{\partial t} + \divs( \vect{u} (E+P) )
+ = \rho\vect{f}_v\cdot\vect{u} + \divs(\tens{\Sigma}^v \vect{u})
+ - \divs{\,\vect{\Phi}_s} + \rho\Phi_v
+-
+ \end{array}\right.
+ \end{equation}
+
diff --git a/science/code_saturne/files/patch-docs_theory_cfmsvl.tex b/science/code_saturne/files/patch-docs_theory_cfmsvl.tex
new file mode 100644
--- /dev/null
+++ b/science/code_saturne/files/patch-docs_theory_cfmsvl.tex
@@ -0,0 +1,34 @@
+--- docs/theory/cfmsvl.tex.orig 2023-12-10 13:11:41 UTC
++++ docs/theory/cfmsvl.tex
+@@ -39,7 +39,6 @@ On a donc le syst\`eme suivant, entre $t^n$ et $t^*$~:
+ On a donc le syst\`eme suivant, entre $t^n$ et $t^*$~:
+ \begin{equation}\label{Cfbl_Cfmsvl_eq_acoustique_cfmsvl}
+ \left\{\begin{array}{l}
+-
+ \displaystyle\frac{\partial\rho}{\partial t}+\divs{\vect{Q}_{ac}} = 0 \\
+ \\
+ \displaystyle\frac{\partial\vect{Q}_{ac}}{\partial t}+\gradv{P} =
+@@ -48,7 +47,6 @@ e^*=e^n\\
+ \vect{Q}^*=\vect{Q}^n\\
+ \\
+ e^*=e^n\\
+-
+ \end{array}\right.
+ \end{equation}
+
+@@ -83,7 +81,6 @@ Le syst\`eme (\ref{Cfbl_Cfmsvl_eq_acoustique_cfmsvl})
+ Le syst\`eme (\ref{Cfbl_Cfmsvl_eq_acoustique_cfmsvl}) discr\'etis\'e en temps donne :
+ \begin{equation}\label{Cfbl_Cfmsvl_eq_acoustique_discrete_cfmsvl}
+ \left\{\begin{array}{l}
+-
+ \displaystyle\frac{\rho^{n+1}-\rho^n}{\Delta t^n}
+ + \divs{\vect{Q}_{ac}^{n+1}} = 0 \\
+ \\
+@@ -93,7 +90,6 @@ e^*=e^n\\
+ Q^*=Q^n\\
+ \\
+ e^*=e^n\\
+-
+ \end{array}\right.
+ \end{equation}
+
diff --git a/science/code_saturne/files/patch-docs_theory_cfqdmv.tex b/science/code_saturne/files/patch-docs_theory_cfqdmv.tex
new file mode 100644
--- /dev/null
+++ b/science/code_saturne/files/patch-docs_theory_cfqdmv.tex
@@ -0,0 +1,18 @@
+--- docs/theory/cfqdmv.tex.orig 2023-12-10 13:11:41 UTC
++++ docs/theory/cfqdmv.tex
+@@ -50,7 +50,6 @@ module compressible)~:
+
+ \begin{equation}\label{Cfbl_Cfqdmv_eq_qdm_cfqdmv}
+ \left\{\begin{array}{l}
+-
+ \rho^{**}=\rho^{*}=\rho^{n+1}\\
+ \\
+ \displaystyle\frac{\partial \rho\vect{u}}{\partial t}+
+@@ -58,7 +57,6 @@ e^{**}=e^{*}=e^n\\
+ = \rho \vect{f}_v + \divv(\tens{\Sigma}^v)\\
+ \\
+ e^{**}=e^{*}=e^n\\
+-
+ \end{array}\right.
+ \end{equation}
+
diff --git a/science/code_saturne/files/patch-docs_theory_cfxtcl.tex b/science/code_saturne/files/patch-docs_theory_cfxtcl.tex
new file mode 100644
--- /dev/null
+++ b/science/code_saturne/files/patch-docs_theory_cfxtcl.tex
@@ -0,0 +1,26 @@
+--- docs/theory/cfxtcl.tex.orig 2023-12-10 13:11:41 UTC
++++ docs/theory/cfxtcl.tex
+@@ -36,7 +36,6 @@ le syst\`eme (\ref{Cfbl_Cfxtcl_eq_ref_laminaire_cfxtcl
+
+ \begin{equation}\label{Cfbl_Cfxtcl_eq_ref_laminaire_cfxtcl}
+ \left\{\begin{array}{l}
+-
+ \displaystyle\frac{\partial\rho}{\partial t} + \divs(\vect{Q}) = 0 \\
+ \\
+ \displaystyle\frac{\partial\vect{Q}}{\partial t}
+@@ -46,7 +45,6 @@ - \divs{\,\vect{\Phi}_s} + \rho\Phi_v
+ \displaystyle\frac{\partial E}{\partial t} + \divs( \vect{u} (E+P) )
+ = \rho\vect{f}_v\cdot\vect{u} + \divs(\tens{\Sigma}^v \vect{u})
+ - \divs{\,\vect{\Phi}_s} + \rho\Phi_v
+-
+ \end{array}\right.
+ \end{equation}
+
+@@ -1296,7 +1294,6 @@ -\dive{\left(\frac{K}{C_v}\,\grad{(\frac{1}{2}\,u^2+\v
+ si \ \ } C_v \text{\ est constant}\\
+ &=& \displaystyle\dive{\left(\frac{K}{C_v}\,\grad\,e\right)}
+ -\dive{\left(\frac{K}{C_v}\,\grad{(\frac{1}{2}\,u^2+\varepsilon_{sup})}\right)} \\
+-
+ \end{array}
+ \end{equation}
+
diff --git a/science/code_saturne/files/patch-docs_theory_cs__velocity__prediction.tex b/science/code_saturne/files/patch-docs_theory_cs__velocity__prediction.tex
new file mode 100644
--- /dev/null
+++ b/science/code_saturne/files/patch-docs_theory_cs__velocity__prediction.tex
@@ -0,0 +1,10 @@
+--- docs/theory/cs_velocity_prediction.tex.orig 2023-12-10 13:11:41 UTC
++++ docs/theory/cs_velocity_prediction.tex
+@@ -96,7 +96,6 @@ T_{s}^{\,imp}\ \vect{u}}_{\text{other source terms}}
+ \underbrace { \vect{T}_{\,s}^{\,exp}+
+ T_{s}^{\,imp}\ \vect{u}}_{\text{other source terms}}
+ \label{Base_Predvv_eqqdm}
+-
+ \end{array}
+ \end{equation}
+ with $p$ denoting the difference in pressure relative to the reference hydrostatic

File Metadata

Mime Type
text/plain
Expires
Sat, Nov 14, 6:51 PM (6 h, 24 s)
Storage Engine
blob
Storage Format
Raw Data
Storage Handle
41720017
Default Alt Text
D61427.1794682299.diff (4 KB)

Event Timeline