Explore NA, acceptance cone, and index contrast accurately. Switch between solving NA, angles, or indices. Export results, compare examples, and validate fiber specs fast.
| n1 | n2 | NA | n0 | θmax (deg) | a (μm) | λ (nm) | V |
|---|---|---|---|---|---|---|---|
| 1.468200 | 1.462000 | 0.134854 | 1.000 | 7.747 | 25 | 850 | 24.93 |
| 1.450000 | 1.444000 | 0.131394 | 1.333 | 5.648 | 4.1 | 1550 | 2.18 |
| 1.470000 | 1.460000 | 0.170000 | 1.000 | 9.781 | 31.25 | 1310 | 25.45 |
Numerical aperture (NA) is a compact way to describe how strongly a step‑index fiber guides light. Higher NA means a wider acceptance cone, easier coupling, and usually more supported modes. For many silica links, NA values around 0.12–0.14 are common in single‑mode designs, while many multimode systems use roughly 0.20–0.30 for relaxed alignment.
This calculator uses NA = √(n1² − n2²), where n1 is the core index and n2 is the cladding index. Small changes in indices matter: with n1 = 1.4682 and n2 = 1.4620, NA is about 0.1349. That corresponds to a modest index contrast suitable for low‑loss glass guidance.
In an external medium with refractive index n0, the acceptance half‑angle is θmax = sin⁻¹(NA/n0). In air (n0 ≈ 1), NA = 0.14 gives θmax near 8 degrees, while NA = 0.22 gives about 12.7 degrees. A larger cone helps LED/VCSEL coupling but may increase modal dispersion in multimode links.
The relative index difference Δ = (n1 − n2)/n1 summarizes how close the indices are. Typical Δ for silica fibers is on the order of 0.2%–1%. The calculator also reports the critical angle at the core‑cladding boundary, helping confirm total internal reflection conditions.
Add core radius a and wavelength λ to compute V = (2πa/λ)·NA. V captures how “large” the guided field is relative to the core. For example, a = 25 μm, λ = 850 nm, and NA ≈ 0.135 yields V around 25, clearly multimode. A smaller core (a ≈ 4.1 μm) at λ = 1550 nm with NA near 0.13 can push V toward the single‑mode region.
For step‑index fibers, the common single‑mode cutoff is V < 2.405. Above that, additional modes can propagate. When V is large, the approximate guided mode count is M ~ V²/2. This estimate helps compare designs, especially for multimode bandwidth planning.
Use realistic indices: silica near 1.44–1.48 depending on wavelength and doping. Keep n1 > n2 for a valid step‑index model, and ensure NA ≤ n0 if you are interpreting θmax in that surrounding medium. If NA exceeds n0, the calculator flags the acceptance angle as not physically valid.
NA is used in connector tolerances, lens coupling design, and link budgeting where launch conditions matter. Exporting results to CSV supports documentation and comparison across candidate fibers. Use the PDF print export for clean lab notes, procurement specs, or design reviews.
Many single‑mode designs use NA around 0.10–0.14. The exact value depends on core size, wavelength, and target bend performance. Always confirm with the V-number cutoff for your geometry.
NA sets the acceptance cone. A larger cone captures rays over a wider range of angles, improving alignment tolerance and coupling from sources like LEDs, but it can increase modal dispersion in multimode links.
For acceptance angle calculations, you typically need NA ≤ n0 because θmax uses sin⁻¹(NA/n0). If NA exceeds n0, the angle relation breaks, and the result is not physically meaningful.
Δ summarizes index contrast and relates to confinement strength. Small Δ often means lower dispersion and weaker confinement, while larger Δ improves confinement and bend tolerance but can increase sensitivity to profile details.
Compute V = (2πa/λ)·NA. If V is below 2.405 for a step‑index design, it is likely single‑mode. If it is higher, multiple modes can propagate.
No. The M ~ V²/2 result is an approximation that works best for large V in step‑index multimode fibers. Real mode counts depend on refractive index profile, wavelength, and launch conditions.
Common operating windows include 850 nm for short‑reach multimode, and 1310 nm or 1550 nm for many single‑mode links. Wavelength affects indices, V-number, dispersion, and loss.