How to show pointwise/uniform converge for Fourier series in general I have asked this question before but I did not get any answers so I hope it is OK if I ask again. 
Consider the function $f: \mathbb{R} \rightarrow \mathbb{R}$ in $C_{\text{st}}$ which satisfies that
$$
f(x) = 6x+2
$$
when $-\pi < x < \pi$. Then I have to argue for or against if the Fourier series converges pointwise or uniformly on $\mathbb{R}$. I have asked this question before but as $C_{\text{st}}$ is not common notation I hope I can get some more answers when defining what it means.
I would very much like to know how to tackle these kinds of questions as they most definitely will be a part of my analysis exam in three weeks. 

Definition: Let $C_{\text{st}}$ be the set of the functions $f:
 \mathbb{R} \rightarrow \mathbb{C}$ which satisfies that
  
  
*
  
*$f$ is $2\pi$-periodic
  
*$f$ is piecewise continuous on the interval $[-\pi, \pi]$
  
*$f$ is normalized in its points of discontinunation meaning that $f(x) =\frac{f(x_{-})+f(x_{+})}{2}$

Futhermore we also need the following

Definition: Let $C^1_{\text{st}}$ be the set of the functions $f:
 \mathbb{R} \rightarrow \mathbb{C}$ which satisfies
  
  
*
  
*$f$ is $2\pi$-periodic
  
*$f$ is piecewise differentiable on the interval $[-\pi, \pi]$
  
*$f$ is normalized in its points of discontinunation
  

Then my book says that

Definition: The Fourier series for a function $f \in C^1_{\text{st}}$
  converges pointwise towards $f$ on $\mathbb{R}$

and

Definition: If $f \in C^1_{\text{st}}$ and continuous on $\mathbb{R}$ then the Fourier series for $f$ converges uniformly on $\mathbb{R}$

Then to prove pointwise convergence, are these definitions sufficient to show that $f$ is piecewise differentiable on $[-\pi,\pi]$ as $f \in C_{\text{st}}$?
Then to prove uniform convergence, are these definitions sufficient to show that $f$ is piecewise differentiable on $[-\pi,\pi]$ as $f \in C_{\text{st}}$ and that $f$ is continuous on $\mathbb{R}$? 
 A: There seems to be a number of questions here, likely covered in your book, but it could be helpful to list non-exhaustively some of the main results regarding the convergence of Fourier series.  Apologies if long, but I hope it will be a helpful checklist for you.
We shall assume $ f : \mathbb R \to \mathbb C $ is $2\pi$-periodic.  We consider the normed Lebesgue integrable spaces, $L^1(-\pi,\pi)$ and $L^2(-\pi,\pi)$, recalling that on a bounded interval $L^2 \subset L^1$.  We can associate any $f$ in either $L^2(-\pi,\pi)$ or $L^1(-\pi,\pi)$ with its Fourier series, writing
$$f \sim \sum_{k=-\infty}^{+\infty} a_k e^{ikx}  \quad\text{and}\quad
S_n(f,x) = \sum_{k=-n}^{n}a_ke^{ikx} $$
where each coefficient is given by $\displaystyle a_k =\frac{1}{2\pi} \int_{-\pi}^{\pi} f(x) e^{-ikx} ~dx $.  The integrals exists for $ f \in L^2 $ or $L^1$.
The most common covergence results are : 


*

*Convergence in $L^2$ norm.  For all $f \in L^2(-\pi,\pi)$
$$\left\lVert S_n - f \right\rVert_{L^2} \to 0 \text{ as } n \to \infty $$
where the norm for any $f$ is $ \displaystyle \lVert f \rVert_{L^2} = \int_{-\pi}^{\pi} \lvert f(x) \rvert^2 ~dx $.

*Parseval. For all $f \in L^2(-\pi,\pi)$, the sum $\displaystyle \sum_{k=-n}^{n} |a_k|^2 \to \lVert f \rVert^2$ as $n \to\infty$

*Pointwise convergence (Jordan). Let $x_0 \in \mathbb R$. If $f \in L^1(-\pi,\pi)$ has bounded variation on an interval $[x_0-r, x_0+r]$ for some $ r > 0$. Then the limits $$f(x_0+) = \lim_{h \searrow 0} f(x+h) \quad\text{and}\quad f(x_0-) = \lim_{h\searrow 0} f(x-h) $$
both exist and $S_n(f,x_0) \to \dfrac{1}{2} ( f(x_0+) + f(x_0-) ) $. 
This resulte embodies the localisation principle where the convergence of $f$ at $x_0$ depends only on its characteristics in an arbitrarily small interval around $x_0$.

*Uniform convergence.  If $f$ is $2\pi$-periodic, continuous on $\mathbb R$ (note that implies $f(\pi) = f(-\pi)$) and piecewise continuously differentiable (i.e. the interval $[-\pi,\pi]$ can be divided into a finite number of sub-inetrvals $I_j, j=1, \cdots, m$ and $f$ is continuously differentiable in each $I_j$, with one sided derivatives at the end points) then the Fourier series $S_n(f,x)$ converges absolutely and uniformly to $f(x)$ on $[-\pi,\pi]$.

*Gibbs phenomena.  For a function $f$ that is piecewise continuous, convergence at points of discontinuity is non-uniform.  In fact the the maximum error between $S_n(f,x)$ and $f(x)$ has positive limit.  
The function $f(x) = 6x+2$ meets the criteria for 1,2,3 but not 4 because there is no definition at $x = \pm \pi$ that would allow the function to be continuous there.  The Fourier series at $\pm \pi$ converges to the mid point $\frac{1}{2}(f(0+)+f(0-)) = 2$.
