Ray optics is a good approximation when:
\[ z = \frac{a^2}{\lambda} \]
where $a = 3 \text{ mm} = 3 \times 10^{-3} \text{ m}$ and $\lambda = 500 \text{ nm} = 500 \times 10^{-9} \text{ m}$:
\[ z = \frac{(3 \times 10^{-3})^2}{500 \times 10^{-9}} \approx 18 \text{ m} \]