In the proof below, we use the standard basis $e_{ij}$ ($i\neq j$), $h_{1}=e_{11}-e_{22}$, $h_{2}=e_{22}-e_{33}$ of $\mathfrak{sl}(3,\text{F})$.
Suppose $I\neq0$ is an ideal of $\mathfrak{sl}(3,\text{F})$. Suppose $x=\sum_{i,j}a_{ij}e_{ij}+b_{1}h_{1}+b_{2}h_{2}\in I$.
Firstly, we compute that
\begin{align}
[h_{1},e_{12}] &=2e_{12} \\
[h_{1},e_{21}] &=-2e_{21} \\
[h_{1},e_{23}] &=-e_{23} \\
[h_{1},e_{32}] &=e_{32} \\
[h_{1},e_{13}] &=e_{13} \\
[h_{1},e_{31}] &=-e_{31} \\
[h_{1},h_{2}] &=0.
\end{align}
Therefore, $\text{ad}_{h_{1}}$ is diagonalizable and $e_{ij}$, $h_{1}$, $h_{2}$ consist of a diagonal basis. So there is an eigenspace decomposition of $\mathfrak{sl}(3,\text{F})$ into
$$
\mathfrak{sl}(3,\text{F})=<e_{21}>\oplus<e_{23},e_{31}>\oplus<h_{1},h_{2}>\oplus<e_{13},e_{32}>\oplus<e_{12}>,
$$
where $<>$ denotes the vector space spanned by the vectors in the bracket. We re-express $x=\sum_{i,j}a_{ij}e_{ij}+b_{1}h_{1}+b_{2}h_{2}\in I$ as $x=x_{-2}+x_{-1}+x_{0}+x_{1}+x_{2}\in I$, where $x_{\lambda}$ denotes the component whose eigenvalue is $\lambda$.
Since $I$ is an ideal, $I$ is an invariant subspace of $\mathfrak{sl}(3,\text{F})$ under the action of $\text{ad}_{h_{1}}$. By a lemma in linear algebra, for each of the $x_{\lambda}\neq0$, $x_{\lambda}\in I$. More specifically, we can deduce $x_{-2}\in I$ and $x_{2}\in I$ directly for the specific $x$ in this exercise: since
$$
\begin{aligned}
\text{ad}_{h_{1}}(x) &=-2x_{-2}-x_{-1}+x_{1}+2x_{2}\in I \\
\text{ad}_{h_{1}}^{2}(x) &=4x_{-2}+x_{-1}+x_{1}+4x_{2}\in I \\
\text{ad}_{h_{1}}(x)+\text{ad}_{h_{1}}^{2}(x) &=2x_{-2}+2x_{1}+6x_{2}\in I \\
\text{ad}_{h_{1}}[\text{ad}_{h_{1}}(x)+\text{ad}_{h_{1}}^{2}(x)]=\text{ad}_{h_{1}}^{2}(x)+\text{ad}_{h_{1}}^{3}(x) &=-4x_{-2}+2x_{1}+12x_{2}\in I \\
\text{ad}_{h_{1}}(x)+\text{ad}_{h_{1}}^{2}(x)-[\text{ad}_{h_{1}}^{2}(x)+\text{ad}_{h_{1}}^{3}(x)]=\text{ad}_{h_{1}}(x)-\text{ad}_{h_{1}}^{3}(x) &=6x_{-2}-6x_{2}\in I \\
\text{ad}_{h_{1}}[\text{ad}_{h_{1}}(x)-\text{ad}_{h_{1}}^{3}(x)]=\text{ad}_{h_{1}}^{2}(x)-\text{ad}_{h_{1}}^{4}(x) &=-12x_{-2}-12x_{2}\in I,
\end{aligned}
$$
we deduce that $x_{-2}\in I$ and $x_{2}\in I$, that is, $e_{21}\in I$ and $e_{12}\in I$.
Since
\begin{align}
[e_{12},e_{21}] &=h_{1} \\
[e_{12},e_{23}] &=e_{13} \\
[e_{21},e_{13}] &=e_{23} \\
[e_{21},e_{32}] &=-e_{31} \\
[e_{31},e_{12}] &=e_{32},
\end{align}
we deduce that $e_{13},e_{31},e_{23},e_{32},h_{1}\in I$.
Since $$[e_{23},e_{32}]=h_{2},$$ we deduce that $h_{2}\in I$. Hence $I=\mathfrak{sl}(3,\text{F})$, and $\mathfrak{sl}(3,\text{F})$ is simple.