If the rabbits-foxes system is written for brevity as $\dot{r}=R(r, f)$ and $\dot{f}=F(r, f)$, the modified Euler algorithm for solving the equations is
$$
r_{n+1}=r_n+\frac{h}{2}\left(R_1[n]+R_2[n]\right), \quad f_{n+1}=f_n+\frac{h}{2}\left(F_1[n]+F_2[n]\right),
$$
where
$$
\begin{aligned}
& t_{n+1}=t_n+h, \quad R_1[n] \equiv R\left(r_n, f_n\right), \quad F_1[n] \equiv F\left(r_n, f_n\right), \\
& R_2[n] \equiv R\left(r_n+h R_1[n], f_n+h F_1[n]\right), \quad F_2[n] \equiv F\left(r_n+h R_1[n], f_n+h F_1[n]\right) . \\
&
\end{aligned}
$$
Taking the same parameter values as in the text recipe, but $N$ twice as large, solve the rabbits-foxes equations using the modified Euler algorithm given above. Rotate your plot to show the $r-f$ phase plane and compare the result with that for the Euler method.