diff --git a/Mathematics/5th/Introduction_to_evolution_PDEs/Introduction_to_evolution_PDEs.tex b/Mathematics/5th/Introduction_to_evolution_PDEs/Introduction_to_evolution_PDEs.tex deleted file mode 100644 index 724d078..0000000 --- a/Mathematics/5th/Introduction_to_evolution_PDEs/Introduction_to_evolution_PDEs.tex +++ /dev/null @@ -1,8 +0,0 @@ -\documentclass[../../../main_math.tex]{subfiles} - -\begin{document} -\changecolor{IEPDE} -\begin{multicols}{2}[\section{Introduction to evolution PDEs}] - -\end{multicols} -\end{document} \ No newline at end of file diff --git a/Mathematics/5th/Introduction_to_nonlinear_elliptic_PDEs/Introduction_to_nonlinear_elliptic_PDEs.tex b/Mathematics/5th/Introduction_to_nonlinear_elliptic_PDEs/Introduction_to_nonlinear_elliptic_PDEs.tex index 8f78029..d678b7e 100644 --- a/Mathematics/5th/Introduction_to_nonlinear_elliptic_PDEs/Introduction_to_nonlinear_elliptic_PDEs.tex +++ b/Mathematics/5th/Introduction_to_nonlinear_elliptic_PDEs/Introduction_to_nonlinear_elliptic_PDEs.tex @@ -223,5 +223,26 @@ \begin{definition} If the weak solution $u_f$ of the problem $\mathcal{D}_f$ is in $H^1_0(\Omega)\cap W^{2,p}(\Omega)$ for some $p\in [1,\infty)$, then we say that $u_f$ is called a \emph{strong solution} of $\mathcal{D}_f$. If $u_f\in \mathcal{C}^2(\Omega)\cap H^1_0(\Omega)$, then we say that $u_f$ is a \emph{classical solution} of $\mathcal{D}_f$. \end{definition} + \begin{theorem} + Let $1Mathematics
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  • diff --git a/main_math.tex b/main_math.tex index 90e8f13..c58d895 100644 --- a/main_math.tex +++ b/main_math.tex @@ -110,9 +110,6 @@ \chapter{Fifth year} \subfile{Mathematics/5th/Advanced_topics_in_functional_analysis_and_PDEs/Advanced_topics_in_functional_analysis_and_PDEs.tex} \cleardoublepage -% \subfile{Mathematics/5th/Introduction_to_evolution_PDEs/Introduction_to_evolution_PDEs.tex} -% \cleardoublepage - \subfile{Mathematics/5th/Introduction_to_nonlinear_elliptic_PDEs/Introduction_to_nonlinear_elliptic_PDEs.tex} \cleardoublepage