Expression for log of normal density
We consider the log of the normal density
\begin{align}
\log p(y|\mu,\Sigma)=-\frac{D}{2}\log{|2\pi|}-\frac{1}{2}\log{|\Sigma|}-\frac{1}{2}(y-\mu)^\top\Sigma^{-1}(y-\mu)\quad\quad(1)
\end{align}
where $D$ denotes the dimension of $y$ and $\mu$.
Derivative w.r.t. mean
We have
\begin{align}
\frac{\partial\log p(y|\mu,\Sigma)}{\mu}=\Sigma^{-1}(y-\mu)
\end{align}
from (96, 97) the Matrix Cookbook and noting the first two terms on the r.h.s. of (1) differentiate to 0.
Derivative w.r.t. covariance
This requires careful consideration of the fact that $\Sigma$ is symmetric - see example at the bottom for the importance of taking this into account!
We have by (141) the Matrix Cookbook that for a symmetric $\Sigma$ the following derivatives
\begin{align}
\frac{\partial \log|\Sigma|}{\partial \Sigma}&=2\Sigma^{-1}-(\Sigma^{-1}\circ I)
\end{align}
and (139) the Matrix Cookbook gives
\begin{align}
\frac{\partial \textrm{trace}(\Sigma^{-1}xx^\top)}{\partial \Sigma}&=-2\Sigma^{-1}xx^\top\Sigma^{-1}+(\Sigma^{-1}xx^\top\Sigma^{-1}\circ I)
\end{align}
where $\circ$ denotes the Hadmard product and for convenience we have defined $x:=y-\mu$. Note that both expressions would be different is $\Sigma$ was not required to be symmetric. Putting these together we have
\begin{align}
\frac{\partial\log p(y|\mu,\Sigma)}{\Sigma}&=-\frac{\partial }{\partial \Sigma}\frac{1}{2}\left(D\log|2\pi|+ \log|\Sigma| + x^{\top}\Sigma^{-1}x)\right)\\
&=-\frac{\partial }{\partial \Sigma}\frac{1}{2}\left( \log|\Sigma| + \textrm{trace}(\Sigma^{-1}xx^\top)\right)\\
&=-\frac{1}{2}\left( 2\Sigma^{-1}-(\Sigma^{-1}\circ I) -2\Sigma^{-1}xx^\top\Sigma^{-1}+(\Sigma^{-1}xx^\top\Sigma^{-1}\circ I)\right)
\end{align}
as the derivative of $\frac{D}{2}\log|2\pi|$ is 0.
Note that it is WRONG to ignore that $\Sigma$ is symmetric
Impact of $\Sigma$ being symmetric
This example shows why you can't just ignore the fact $\Sigma$ is symmetric when differentiating with respect to its elements. Consider the matrix function
\begin{align}
f(X)=\Sigma_{ij} X_{ij}
\end{align}
so just sums up all the elements of $X$, some arbitrary matrix. If we consider
\begin{align*}
\\
&1)\quad X =\left(\begin{array}{cc}
a & b\\
c & d
\end{array}\right) & \implies && \frac{df}{dX} & =\left(\begin{array}{cc}
1 & 1\\
1 & 1
\end{array}\right)\\
&2)\quad X^{*}=\left(\begin{array}{cc}
a & b\\
b & c
\end{array}\right) & \implies && \frac{df}{dX^{*}} & =\left(\begin{array}{cc}
1 & 2\\
2 & 1
\end{array}\right)
\end{align*}
Then we see obviously the derivatives of $f$ w.r.t. the elements of $X$ vary depending on whether $X$ is symmetric or not.