In decreasing order: $\rho_2$ then $\rho_1$, because no state is less entangled than a separable state like $\rho_1$. We know that $\rho_1$ is separable, because it is a convex combination of product states.
On the other hand, $\rho_2$ is entangled because its Schmidt rank is $2$. Moreover, its density matrix
$$
\rho_2 = \begin{pmatrix}
0.99 & & & 0.1\sqrt{0.99} \\
& & & \\
& & & \\
0.1\sqrt{0.99} & & & 0.01
\end{pmatrix}
$$
fails Peres-Horodecki criterion, because
$$
\begin{pmatrix}
0.99 & & & \\
& & 0.1\sqrt{0.99} & \\
& 0.1\sqrt{0.99}& & \\
& & & 0.01
\end{pmatrix} \begin{pmatrix}0 \\ 1 \\ -1 \\ 0 \end{pmatrix} =
-0.1\sqrt{0.99}\begin{pmatrix}0 \\ 1 \\ -1 \\ 0 \end{pmatrix}.
$$