In this work, we study the set X ̇(φ,f) of points such that the Birkhoff averages do not exist. Following Thompson, our main result here is to show that the topological pressure of X ̇(φ,f) is total. As corollary, we get the some result for the Oseledets Irregular set for Lyapunov exponent in one dimension. For higher dimensions, this question is still open. / Conselho Nacional de Desenvolvimento Científico e Tecnológico / Neste trabalho, estudamos o conjunto X ̇(φ,f) de pontos tal que as médias de Birkhoff não existe. Seguindo Thompson, nosso resultado principal aqui é mostrar que a pressão topológica de X ̇(φ,f) é total. Como corolário, damos o mesmo resultado para o conjunto Irregular de Oseledets para os expoentes de Lyapunov em dimensão um. Para dimensões maiores, esta questão está em aberto.

We study two topics on surface diffeomorphisms, their mapping classes and dynamics. For the mapping classes of a punctured disc, we study the $\ZxZ$ subgroups of the fundamental groups of the corresponding mapping tori. An application is the proof of the fact that a satellite knot with braid pattern is prime. For the mapping classes of the disc minus a Cantor set, we study a special type of reducible mapping class. This has direct application on the embeddings of solenoids in $\mathbb{S}^3$. We also give some examples of other types of mapping classes of the disc minus a Cantor set. For the dynamics of surface diffeomorphisms, we prove three formulas for computing the topological pressure of a $C^1$-generic conservative diffeomorphism with no dominated splitting and show the continuity of topological pressure with respect to these diffeomorphisms. We prove for these generic diffeomorphisms that there is no equilibrium states with positive measure theoretic entropy. In particular, for hyperbolic potentials, there are no equilibrium states. For $C^1$ generic conservative diffeomorphisms on compact surfaces with no dominated splitting and $\phi_m(x):=-\frac{1}{m}\log \Vert D_x f^m\Vert, m \in \mathbb{N}$, we show that there exist equilibrium states with zero entropy and there exists a transition point $t_0$ for the one parameter family $\lbrace t \phi_m\rbrace_{t\geq 0}$, such that there is no equilibrium states for $ t \in [0, t_0)$ and there is an equilibrium state for $t \in [t_0,+\infty)$.