A slit of width a diffracts a beam of light. Half angular width of central maximum is:
θ ≅ sin θ = \(\frac{\lambda}{a}\)
In travelling distance z, half angular width of beam would become \((\frac{z\lambda}{a})\)
This width will become more than width of slit, i.e. \(\frac{z\lambda}{a} > a,\)
where z > \(\frac{a^2}{\lambda}\)
We call \(\frac{a^2}{\lambda}\) = zF, Fresnel distance.
Now, for a = 3 mm = 3 x 10-3 m
λ = 5000 Å = 5 x 10-7 m
zF = \(\frac{a^2}{\lambda}\) = \(\frac{(3 \times 10^{-3})^2}{5 \times 10^{-7}}\) = 18 m
This means width of beam due to diffraction remains equal to the size of the width of the slit (3 x 10-3) i.e. diffraction effect can be neglected (upto 18 m) and ray optics is valid.