Commit 0249119d by Dmitry Yu. Naumov

### [web] Remove empty lines in latex scope.

This results in wrong rendering otherwise.
parent 05e5cc3b
 ... ... @@ -101,7 +101,6 @@ Newton-Raphson is applied to . Let $$\begin{gathered} \mathbf{r}= { \mathbf \sigma}^{n+1} - { \mathbf \sigma}^{n} - \mathbf{C} (\Delta { \mathbf \epsilon} - \alpha_T \Delta T \mathbf I) + 2bG \Delta t {\left\Vert{\mathbf s}^{n+1}\right\Vert}^{m-1} {\mathbf s}^{n+1} \end{gathered}$$ ... ...
 ... ... @@ -18,7 +18,6 @@ weight = 102 We start with Poisson equation: $$- k\; \Delta p = Q \quad \text{in }\Omega$$ w.r.t boundary conditions ... ...
 ... ... @@ -18,7 +18,6 @@ weight = 102 The Poisson equation is: $$- k\; \Delta p = Q \quad \text{in }\Omega$$ w.r.t boundary conditions ... ...
 ... ... @@ -20,7 +20,6 @@ $$\left( c \rho_R + \phi \frac{\partial \rho_R}{\partial p}\right) \frac{\partial p}{\partial t} - \nabla \cdot \left[ \rho_R \frac{\kappa}{\mu} \left( \nabla p + \rho_R g \right) \right] - Q_p = 0.$$ where ... ...
 ... ... @@ -33,7 +33,6 @@ We solve Laplace's Equation in 2D on a $1 \times 1$ square domain. Laplace's equation is $$- \mathop{\mathrm{div}} (a \mathop{\mathrm{grad}} u) = 0$$ ... ...
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