Meaning and application of the connection coefficients (Christoffel symbols) I know that in polar coordinates, it is
$\frac{\partial \,{{\mathbf{e}}_{r}}}{\partial \theta }={{\mathbf{e}}_{\theta }}$ and $\frac{\partial \,{{\mathbf{e}}_{\theta }}}{\partial \theta }=-{{\mathbf{e}}_{r}}$
where ${{\mathbf{e}}_{r}}$ and ${{\mathbf{e}}_{\theta }}$ are the basis unit vectors.
Anyway, using the definition of the connection coefficients (Christoffel symbols) it should also be
$\frac{\partial \,{{\mathbf{e}}_{r}}}{\partial \theta }={{\Gamma }^{r}}_{r\theta }\,{{\mathbf{e}}_{r}}+{{\Gamma }^{\theta }}_{r\,\theta }\,{{\mathbf{e}}_{\theta }}$ and
$\frac{\partial \,{{\mathbf{e}}_{\theta }}}{\partial \theta }={{\Gamma }^{r}}_{\theta \,\theta }\,{{\mathbf{e}}_{r}}+{{\Gamma }^{\theta }}_{\theta \,\theta }\,{{\mathbf{e}}_{\theta }}$
And since it is ${{\Gamma }^{r}}_{\theta \,\theta }=-r$ , ${{\Gamma }^{\theta }}_{r\,\theta }=\frac{1}{r}$ , ${{\Gamma }^{r}}_{r\,\theta }=0$, ${{\Gamma }^{\theta }}_{\theta \,\theta }=0$    (calculated with the metric)
it should be
$\frac{\partial \,{{\mathbf{e}}_{r}}}{\partial \theta }=\frac{1}{r}{{\mathbf{e}}_{\theta }}$ and $\frac{\partial \,{{\mathbf{e}}_{\theta }}}{\partial \theta }=-r\,{{\mathbf{e}}_{r}}$
Where am I wrong?
 A: You are using two different sets of basis vectors.  $\frac{\partial\mathbf e_r}{\partial \theta} = \mathbf e_\theta$ and $\frac{\partial \mathbf e_\theta}{\partial \theta} = -\mathbf e_r$ hold for the orthonormal polar basis, in which the metric takes the form
$$g_{ij} = \pmatrix{1 & 0 \\ 0 & 1}$$
The connection coefficients you quote arise from the polar coordinate basis $\left\{\frac{\partial}{\partial r},\frac{\partial}{\partial \theta}\right\}$ which is not orthonormal, and in which the metric takes the form
$$g_{ij} = \pmatrix{1 & 0 \\ 0 & r^2}$$
The two bases are related via $\mathbf e_r = \frac{\partial}{\partial r}$ and $\mathbf e_\theta = r\frac{\partial }{\partial \theta}$.

An important thing to recognize is that the basis $\left\{\frac{\partial}{\partial r},\frac{\partial}{\partial \theta}\right\}$ arises naturally as the basis induced by the polar coordinates $(r,\theta)$.  On the other hand, the orthonormal basis $\{e_r,e_\theta\}$ is not induced by a coordinate system; there is no set of coordinates $(u,v)$ such that $e_r = \frac{\partial}{\partial u}$ and $e_\theta =\frac{\partial}{\partial v}$.  This is an example of a non-holonomic basis.
The reason that this is important is that in your first pass through GR, you will likely start off by using holonomic bases exclusively.  Accidentally using a non-holonomic basis can lead to some apparent contradictions.
