To ensure the critical angle incidence in the core-cladding boundary inside the optical fibre, the light should be incident at a certain angle at the end of the optical fiber while entering in to it. This angle is called acceptance angle. It depends on the refractive indices of the core n1, cladding n2 and the outer medium n3. Assume the light is incident at an angle called acceptance angle i at the outer medium and core boundary at A.
The Snell’s law in the product form, equation for this refraction at the point A.

n3sin ia = n1sin ra …(1)
To have the total internal reflection inside optical fibre, the angle of incidence at the corecladding interface at B should be atleast critical angle ic. Snell’s law in the product form, equation for the refraction at point B is,
n1 sin ic = n2 sin 90° …(2)
n1 sin ic = n ∵ sin 90° =1
∴sin ic = \(\frac{n_2}{n_1}\) …(3)
From the right angle triangle ∆ABC,
ic = 90°- ra
Now, equation (3) becomes, sin (90° – ra) = \(\frac{n_2}{n_1}\)
Using trigonometry’ , cos ra =ra = \(\frac{n_2}{n_1}\) ....... (4)
sin ra = \(\sqrt{1-cos^2r_a}\)
Substituting for cos ra

If outer medium is air, then n3 = 1. The acceptance angle ia becomes,

Light can have any angle of incidence from 0 to ia with the normal at the end of the optical fibre forming a conical shape called acceptance cone. In the equation (6), the term (n3 sin ia) is called numerical aperture NA of the optical fibre.

If outer medium is air, then n = 1. The numerical aperture NA becomes,
NA = sin ia = \((\sqrt{n^2_1-n^2_2})\) ............. (11)