Covariant derivative of determinant of the metric tensor Let $(M,g)$ be a Riemannian manifold and $g$ the Riemannian metric in coordinates $g=g_{\alpha \beta}dx^{\alpha} \otimes dx^{\beta}$, where $x^{i}$ are local coordinates on $M$. Denote by $g^{\alpha \beta}$ the inverse components of the inverse metric $g^{-1}$. Let $\nabla$ be the Levi-Civita connection of the metric $g$. Consider, locally, the function $\det((g_{\alpha \beta})_{\alpha \beta})$. It is known that $\nabla \det((g_{\alpha \beta})_{\alpha \beta}) = 0$ by using normal coordinates etc...
I would like to show this fact without using normal coordinates. Just by computation. Here is what I have so far: 
$$\nabla \det((g_{\alpha \beta})_{\alpha \beta}) =  \left [ g^{\gamma \delta} \partial_{\delta} \det((g_{\alpha \beta})_{\alpha \beta}) \right ] \partial_{\gamma} = \left [ \det((g_{\alpha \beta})_{\alpha \beta}) g^{\gamma \delta} g^{\beta \alpha} \partial_{\delta} g_{\alpha \beta}\right ] \partial_{\gamma}.$$
Here: the first equality sign follows from the definition of the gradient of a function and the second equality sign is the derivative of the determinant.
Question: How do I continue from here without using normal coordinates? Or are there any mistakes? If yes, where and which?
 A: Calculate $\Gamma^\nu_{\mu\nu}=\frac{1}{2}g^{\nu\kappa}(\partial_\mu g_{\nu\kappa}+\partial_\nu g_{\mu\kappa}-\partial_\kappa g_{\mu\nu})=\frac{1}{2}g^{\nu\kappa}\partial_\mu g_{\nu\kappa}$. Using the well known formula $$ \det A^{-1}\frac{d}{dt}\det A=\text{Tr}\left(A^{-1}\frac{d A}{dt}\right), $$ we obtain $$ \Gamma_\mu\equiv\Gamma^\nu_{\mu\nu}=\frac{1}{2}\frac{1}{g}\partial_\mu g=\frac{1}{2}\partial_\mu\ln|g|=\partial_\mu\ln \sqrt{|g|}, $$ where $g$ denotes the determinant of the matrix with elements $g_{\mu\nu}$.
The expression $\rho=\sqrt{|g|}$ transforms under a change of chart as follows: We have $g_{\mu^\prime \nu^\prime}=\partial_{\mu^\prime}x^\mu\partial_{\nu^\prime}x^\nu g_{\mu\nu}=J^\mu_{\mu^\prime}J^\nu_{\nu^\prime}g_{\mu\nu}$, taking determinants gives $$ g^\prime=\det J^2g \\ \sqrt{|g^\prime|}=|\det J|\sqrt{|g|}. $$ This object is called a "scalar density of weight 1". It makes sense in a coordinate-free manner too as a section of the density bundle, but whatever. One can show that the components of the covariant derivative of such an object is $$\nabla_\mu\rho=\partial_\mu\rho-\Gamma_\mu\rho=\partial_\mu\rho-\partial_\mu\ln\sqrt{|g|}\rho.$$ Inserting $\rho=\sqrt{|g|}$ gives $$ \nabla_\mu\sqrt{|g|}=\partial_\mu\sqrt{|g|}-\frac{1}{\sqrt{|g|}}\partial_\mu\sqrt{|g|}\sqrt{|g|}=\partial_\mu\sqrt{|g|}-\partial_\mu\sqrt{|g|}=0. $$
A: One can give a short proof by considering the reciprocal basis $\partial^k=g^{k\sigma}\partial_{\sigma}$ and its derivative $\nabla_{\partial_k}\partial^j=-\Gamma^{j}{}_{ks}\partial^s$, because if we represent the metric tensor as 
$$g=g^{st}\partial_s\otimes\partial_t$$
then 
\begin{eqnarray*}
g&=&g^{st}\partial_s\otimes\partial_t\\
&=&\partial_s\otimes g^{st}\partial_t\\
&=&\partial_s\otimes\partial^s.
\end{eqnarray*}
So
\begin{eqnarray*}
\nabla_{\partial_k}g&=&\nabla_{\partial_k}(\partial_s\otimes\partial^s)\\
&=&(\nabla_{\partial_k}\partial_s)\otimes\partial^s+\partial_s\otimes\nabla_{\partial_k}\partial^s\\
&=&\Gamma^r{}_{ks}\partial_r\otimes\partial^s-\partial_s\otimes
\Gamma^s{}_{kr}\partial^r\\
&=&\Gamma^r{}_{ks}\partial_r\otimes\partial^s-\Gamma^s{}_{kr}\partial_s\otimes
\partial^r\\
&=&\Gamma^r{}_{ks}\partial_r\otimes\partial^s-\Gamma^r{}_{ks}\partial_r\otimes
\partial^s\\
&=&0.
\end{eqnarray*}
