From 8ffb5df7b094ccbc46f5c5fab070e973ca6d696a Mon Sep 17 00:00:00 2001
From: Andreas Lauser <and@poware.org>
Date: Fri, 20 Jan 2012 16:36:40 +0000
Subject: [PATCH] fix LaTeX errors in formulas
that was a lot of fun!
git-svn-id: svn://svn.iws.uni-stuttgart.de/DUMUX/dumux/trunk@7478 2fb0f335-1f38-0410-981e-8018bf24f1b0
---
doc/doxygen/html/dummy.gif | 0
dumux/boxmodels/MpNc/MpNcmodel.hh | 19 ++++++++++---------
dumux/decoupled/2p2c/fvpressure2p2c.hh | 10 +++++-----
dumux/material/fluidsystems/1pfluidsystem.hh | 4 ++--
.../fluidsystems/2pimmisciblefluidsystem.hh | 4 ++--
.../material/fluidsystems/basefluidsystem.hh | 4 ++--
.../material/fluidsystems/h2on2fluidsystem.hh | 4 ++--
.../1p2c/interstitialfluidtrailfluidsystem.hh | 4 ++--
8 files changed, 25 insertions(+), 24 deletions(-)
delete mode 100644 doc/doxygen/html/dummy.gif
diff --git a/doc/doxygen/html/dummy.gif b/doc/doxygen/html/dummy.gif
deleted file mode 100644
index e69de29bb2..0000000000
diff --git a/dumux/boxmodels/MpNc/MpNcmodel.hh b/dumux/boxmodels/MpNc/MpNcmodel.hh
index dfcd924489..718b67ba4d 100644
--- a/dumux/boxmodels/MpNc/MpNcmodel.hh
+++ b/dumux/boxmodels/MpNc/MpNcmodel.hh
@@ -44,14 +44,15 @@ namespace Dumux
* the conservation of momentum:
* \f[
v_\alpha = - \frac{k_{r\alpha}}{\mu_\alpha} \boldsymbol{K}
- \left(\text{grad} p_\alpha - \varrho_{\alpha} \boldsymbol{g} \right)
- * \f]
+ \left(
+ \text{grad} p_\alpha - \varrho_{\alpha} \boldsymbol{g}
+ \right)
+ \f]
*
* By inserting this into the equations for the conservation of the
* components, one gets one transport equation for each component \f$\kappa\f$
- * \f{equation*}
+ * \f[
\sum_{\kappa} \left(
- %
\phi \frac{\partial \varrho_\alpha x_\alpha^\kappa S_\alpha}{\partial t}
-
\nabla \cdot
@@ -60,16 +61,16 @@ namespace Dumux
\frac{k_{r\alpha}}{\mu_\alpha} \boldsymbol{K}
(\nabla p_\alpha - \varrho_{\alpha} \boldsymbol{g})
\right\}
- \left)
+ \right)
= q^\kappa
- \f{equation*}
+ \f]
* with \f$\overline M_\alpha\f$ being the average molar mass of the phase \f$\alpha\f$:
* \f[ \overline M_\alpha = \sum_\kappa M^\kappa \; x_\alpha^\kappa \f]
*
* For the missing \f$M\f$ model assumptions, the model assumes that
* if a fluid phase is not present, the sum of the mole fractions of
* this fluid phase is smaller than \f$1\f$, i.e.
- * \f[ \forall \alpha: S_\alpha = 0 \implies \sum_\kappa x_\alpha^\kappa \leq 1 \]
+ * \f[ \forall \alpha: S_\alpha = 0 \implies \sum_\kappa x_\alpha^\kappa \leq 1 \f]
*
* Also, if a fluid phase may be present at a given spatial location
* its saturation must be positive:
@@ -91,7 +92,7 @@ namespace Dumux
* \f[ \Phi(a,b) = a + b - \sqrt{a^2 + b^2} \;. \f]
*
* Though this model uses
- * \f[ \Phi(a,b) = \min \{a, b}}\;, \f]
+ * \f[ \Phi(a,b) = \min \{a, b \}\;, \f]
* because of its piecewise linearity.
*
* These equations are then discretized using a fully-implicit vertex
@@ -102,7 +103,7 @@ namespace Dumux
* The model assumes thermodynamic equilibrium and uses the following
* primary variables:
*
- * - The componentfugacities \f$f^1, \dots, f^{N}
+ * - The componentfugacities \f$f^1, \dots, f^{N}\f$
* - The pressure of the first phase \f$p_1\f$
* - The saturations of the first \f$M-1\f$ phases \f$S_1, \dots, S_{M-1}\f$
* - Temperature \f$T\f$ if the energy equation is enabled
diff --git a/dumux/decoupled/2p2c/fvpressure2p2c.hh b/dumux/decoupled/2p2c/fvpressure2p2c.hh
index bc63604b79..1ef948f11b 100644
--- a/dumux/decoupled/2p2c/fvpressure2p2c.hh
+++ b/dumux/decoupled/2p2c/fvpressure2p2c.hh
@@ -225,7 +225,7 @@ void FVPressure2P2C<TypeTag>::getSource(Dune::FieldVector<Scalar, 2>& sourceEntr
/** for first == true, there is no storage contribution.
* for first == false, the storage term comprises the compressibility (due to a change in
* pressure from last timestep):
- * \f[ V_i c_{t,i}& \frac{p^t_i - p^{t-\Delta t}_i}{\Delta t} \f]
+ * \f[ V_i c_{t,i} \frac{p^t_i - p^{t-\Delta t}_i}{\Delta t} \f]
* and the damped error introduced by the incorrect transport of the last timestep:
* \f[ V_i \alpha_r \frac{v_{t} - \phi}{\Delta t} \f].
* The latter is damped according to Fritz 2011.
@@ -304,8 +304,8 @@ void FVPressure2P2C<TypeTag>::getStorage(Dune::FieldVector<Scalar, 2>& storageEn
\frac{\frac{\partial v_{t,j}}{\partial C^{\kappa}_j}-\frac{\partial v_{t,i}}{\partial C^{\kappa}_i}}{\Delta x} X^{\kappa}_{\alpha}
\left( \frac{p_{\alpha,j}^t - p^{t}_{\alpha,i}}{\Delta x} + \varrho_{\alpha} \mathbf{g}\right) \f]
* This includes a boundary integral and a volume integral, because
- * \f$ \frac{\partial v_{t,i}}{\partial C^{\kappa}_i}} \f$ is not constant.
- * Here, \f$ \mathbf{u} \f$ is the normalized vector connecting the cell centers, and \f$ \mathbf{n}_{\gamma_{ij} \f$
+ * \f$ \frac{\partial v_{t,i}}{\partial C^{\kappa}_i} \f$ is not constant.
+ * Here, \f$ \mathbf{u} \f$ is the normalized vector connecting the cell centers, and \f$ \mathbf{n}_{\gamma_{ij}} \f$
* represents the normal of the face \f$ \gamma{ij} \f$.
* \param entries The Matrix and RHS entries
* \param intersection Intersection between cell I and J
@@ -526,9 +526,9 @@ void FVPressure2P2C<TypeTag>::getFlux(Dune::FieldVector<Scalar, 2>& entries,
* \f[ - A_{\gamma_{ij}} \cdot \mathbf{K} \cdot \mathbf{u} \cdot (\mathbf{n}_{\gamma_{ij}} \cdot \mathbf{u})
\sum_{\alpha} \varrho_{\alpha} \lambda_{\alpha} \sum_{\kappa} \frac{\partial v_{t}}{\partial C^{\kappa}} X^{\kappa}_{\alpha}
\left( \frac{p_{\alpha,j}^t - p^{t}_{\alpha,i}}{\Delta x} + \varrho_{\alpha} \mathbf{g}\right) \;, \f]
- * where we skip the volume integral assuming \f$ \frac{\partial v_{t,i}}{\partial C^{\kappa}_i}} \f$
+ * where we skip the volume integral assuming \f$ \frac{\partial v_{t,i}}{\partial C^{\kappa}_i} \f$
* to be constant at the boundary.
- * Here, \f$ \mathbf{u} \f$ is the normalized vector connecting the cell centers, and \f$ \mathbf{n}_{\gamma_{ij} \f$
+ * Here, \f$ \mathbf{u} \f$ is the normalized vector connecting the cell centers, and \f$ \mathbf{n}_{\gamma_{ij}} \f$
* represents the normal of the face \f$ \gamma{ij} \f$.
* \param entries The Matrix and RHS entries
* \param intersection Intersection between cell I and J
diff --git a/dumux/material/fluidsystems/1pfluidsystem.hh b/dumux/material/fluidsystems/1pfluidsystem.hh
index ecdf9ef31d..0fd1909083 100644
--- a/dumux/material/fluidsystems/1pfluidsystem.hh
+++ b/dumux/material/fluidsystems/1pfluidsystem.hh
@@ -282,9 +282,9 @@ public:
* component in a fluid phase [mol^2 * s / (kg*m^3)]
*
* Molecular diffusion of a compoent \f$\kappa\f$ is caused by a
- * gradient of the chemical potential and follows the law
+ * mathbf{grad}ient of the chemical potential and follows the law
*
- * \f[ J = - D \grad mu_\kappa \f]
+ * \f[ J = - D \mathbf{grad} mu_\kappa \f]
*
* where \f$\mu_\kappa\f$ is the component's chemical potential,
* \f$D\f$ is the diffusion coefficient and \f$J\f$ is the
diff --git a/dumux/material/fluidsystems/2pimmisciblefluidsystem.hh b/dumux/material/fluidsystems/2pimmisciblefluidsystem.hh
index ec0f80b09d..bb63ed14b9 100644
--- a/dumux/material/fluidsystems/2pimmisciblefluidsystem.hh
+++ b/dumux/material/fluidsystems/2pimmisciblefluidsystem.hh
@@ -313,9 +313,9 @@ public:
* a component in a fluid phase [mol^2 * s / (kg*m^3)]
*
* Molecular diffusion of a compoent \f$\kappa\f$ is caused by a
- * gradient of the chemical potential and follows the law
+ * mathbf{grad}ient of the chemical potential and follows the law
*
- * \f[ J = - D \grad mu_\kappa \f]
+ * \f[ J = - D \mathbf{grad} mu_\kappa \f]
*
* where \f$\mu_\kappa\f$ is the component's chemical potential,
* \f$D\f$ is the diffusion coefficient and \f$J\f$ is the
diff --git a/dumux/material/fluidsystems/basefluidsystem.hh b/dumux/material/fluidsystems/basefluidsystem.hh
index a61a2d2273..4a28085e92 100644
--- a/dumux/material/fluidsystems/basefluidsystem.hh
+++ b/dumux/material/fluidsystems/basefluidsystem.hh
@@ -87,9 +87,9 @@ public:
* a component in a fluid phase [mol^2 * s / (kg*m^3)]
*
* Molecular diffusion of a compoent \f$\kappa\f$ is caused by a
- * gradient of the chemical potential and follows the law
+ * mathbf{grad}ient of the chemical potential and follows the law
*
- * \f[ J = - D \grad mu_\kappa \f]
+ * \f[ J = - D \mathbf{grad} mu_\kappa \f]
*
* where \f$\mu_\kappa\f$ is the component's chemical potential,
* \f$D\f$ is the diffusion coefficient and \f$J\f$ is the
diff --git a/dumux/material/fluidsystems/h2on2fluidsystem.hh b/dumux/material/fluidsystems/h2on2fluidsystem.hh
index de5e897bdf..5e8f420a60 100644
--- a/dumux/material/fluidsystems/h2on2fluidsystem.hh
+++ b/dumux/material/fluidsystems/h2on2fluidsystem.hh
@@ -501,9 +501,9 @@ public:
* component in a fluid phase [mol^2 * s / (kg*m^3)]
*
* Molecular diffusion of a compoent \f$\kappa\f$ is caused by a
- * gradient of the chemical potential and follows the law
+ * mathbf{grad}ient of the chemical potential and follows the law
*
- * \f[ J = - D \grad mu_\kappa \f]
+ * \f[ J = - D \mathbf{grad} mu_\kappa \f]
*
* where \f$\mu_\kappa\f$ is the component's chemical potential,
* \f$D\f$ is the diffusion coefficient and \f$J\f$ is the
diff --git a/test/boxmodels/1p2c/interstitialfluidtrailfluidsystem.hh b/test/boxmodels/1p2c/interstitialfluidtrailfluidsystem.hh
index 11afa681cb..489a84f9af 100644
--- a/test/boxmodels/1p2c/interstitialfluidtrailfluidsystem.hh
+++ b/test/boxmodels/1p2c/interstitialfluidtrailfluidsystem.hh
@@ -257,9 +257,9 @@ public:
* component in a fluid phase [mol^2 * s / (kg*m^3)]
*
* Molecular diffusion of a compoent \f$\kappa\f$ is caused by a
- * gradient of the chemical potential and follows the law
+ * mathbf{grad}ient of the chemical potential and follows the law
*
- * \f[ J = - D \grad mu_\kappa \f]
+ * \f[ J = - D \mathbf{grad} mu_\kappa \f]
*
* where \f$\mu_\kappa\f$ is the component's chemical potential,
* \f$D\f$ is the diffusion coefficient and \f$J\f$ is the
--
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