Analyze core and cladding optics with confidence. Visualize acceptance limits and transmission trends more clearly. Use precise inputs to model real fiber behavior today.
The page stays in a single-column flow, while the calculator form uses three columns on large screens, two on smaller screens, and one on mobile.
NA = √(n12 − n22)
NA = n0 sin(θa)
Δ = (n1 − n2) / n1n2 = n1(1 − Δ)
V = (2πa / λ) × NA
Pout = Pin × 10−(αL/10)
Here, n1 is core index, n2 is cladding index, n0 is surrounding medium index, a is core radius, λ is wavelength, α is attenuation, and L is fiber length.
| Case | n1 | n2 | n0 | Wavelength (nm) | Core Radius (µm) | NA | Half-Angle (deg) |
|---|---|---|---|---|---|---|---|
| Silica multimode example | 1.480 | 1.460 | 1.000 | 850 | 25 | 0.2425 | 14.03 |
| Higher contrast design | 1.500 | 1.470 | 1.000 | 850 | 31.25 | 0.2985 | 17.37 |
| Low contrast fiber | 1.460 | 1.455 | 1.000 | 1310 | 4.5 | 0.1207 | 6.93 |
| Wide launch cone example | 1.490 | 1.400 | 1.000 | 650 | 50 | 0.5100 | 30.66 |
These examples are provided for learning, comparison, and quick testing of the page layout and export tools.
Numerical aperture measures the light-gathering ability of a fiber. A larger value means the fiber can accept rays over a wider entrance cone and is usually easier to couple with light sources.
Total internal reflection happens only when light travels from a higher-index core toward a lower-index cladding. If the cladding index equals or exceeds the core index, guided propagation will not occur as expected.
In fiber optics, the acceptance half-angle is measured from the fiber axis. The full acceptance cone is simply twice that half-angle.
The surrounding medium changes the launch condition because the relation becomes NA = n0 sin(θa). Air, water, and immersion fluids can give different acceptance angles for the same fiber.
The V number helps classify whether the fiber operates in a single-mode or multimode regime. It also supports quick estimates of the number of guided modes.
Not always. Higher NA improves coupling tolerance, but it can also increase modal dispersion in multimode fibers. The best value depends on your source, distance, bandwidth target, and system design.
NA alone does not describe transmission loss. Adding attenuation and length gives a practical view of how much launched optical power may remain after the fiber span.
They help save results for reports, lab notes, classroom exercises, and design comparisons. CSV is useful for spreadsheets, while PDF is convenient for printable summaries.
Important Note: All the Calculators listed in this site are for educational purpose only and we do not guarentee the accuracy of results. Please do consult with other sources as well.