\(\text{NA} = \sqrt{n_1^2 - n_2^2}\). For \(n_1 = 1.52,\ n_2 = 1.41\): critical angle ≈ 68.07° and NA ≈ 0.568.
Derivation
A ray enters the fibre end face from air (\(n_0 = 1\)) at angle \(\theta_0\) to the axis and refracts into the core at angle \(\theta_r\). It then meets the core–cladding boundary at angle \(\phi = 90^\circ - \theta_r\).
1. Snell's law at the end face:
\[n_0 \sin\theta_0 = n_1 \sin\theta_r\]
2. For total internal reflection the ray must strike the core–cladding surface at least at the critical angle \(\phi_c\), where
\[\sin\phi_c = \frac{n_2}{n_1}\]
3. The largest acceptance angle \(\theta_{max}\) corresponds to \(\phi = \phi_c\), i.e. \(\theta_r = 90^\circ - \phi_c\):
\[n_0\sin\theta_{max} = n_1\cos\phi_c\]
\[= n_1\sqrt{1 - \frac{n_2^2}{n_1^2}}\]
\[= \sqrt{n_1^2 - n_2^2}\]
Numerical aperture is defined as \(\text{NA} = n_0\sin\theta_{max}\), so with \(n_0 = 1\):
\[\text{NA} = \sqrt{n_1^2 - n_2^2}\]
Numerical
Critical angle:
\[\sin\phi_c = \frac{1.41}{1.52} = 0.9276\]
\[\phi_c = 68.07^\circ\]
Numerical aperture:
\[\text{NA} = \sqrt{1.52^2 - 1.41^2}\]
\[= \sqrt{2.3104 - 1.9881} = \sqrt{0.3223}\]
\[\text{NA} \approx 0.568\]
(The acceptance angle is \(\sin^{-1}(0.568) \approx 34.6^\circ\).)