Model light travel through real optical materials. Add multiple layers, tilt angles, and wavelengths easily. See total path, delay, and phase in seconds here.
Optical path length (OPL) measures how far light travels in an equivalent vacuum path. For a path element ds in a medium with refractive index n, the optical contribution is:
OPL = ∫ n ds
For planar layers with constant n, the integral becomes a sum: OPL = Σ (ni · si), where si is the geometric path length inside each layer.
With oblique incidence, the geometric path in a layer is related to its thickness t (measured normal to the interface) by: s = t / cos(θ), where θ is the propagation angle inside that layer.
Angles are computed sequentially using Snell’s law: nprev·sin(θprev) = ni·sin(θi). If |sin(θi) > 1, total internal reflection occurs.
| Parameter | Example value |
|---|---|
| Ambient index n0 | 1.0003 |
| Incident angle | 0° |
| Layer 1 thickness | 5 mm |
| Layer 1 index | 1.50 |
| Layer 2 thickness | 2 mm |
| Layer 2 index | 1.33 |
| Wavelength | 632.8 nm |
Optical path length (OPL) converts a real optical journey into an equivalent distance in vacuum. It is the quantity that controls interference and phase, because light accumulates phase in proportion to n·distance. When two beams have different OPL, their relative phase changes even if their geometric lengths look similar.
Thin films, cover slips, immersion liquids, adhesives, protective windows, and sensor stacks are all layered systems. In a multilayer path, each layer contributes its own OPL term, so small thickness changes can create measurable phase shifts—especially for short wavelengths.
At normal incidence, the geometric path equals the physical thickness, and each layer contributes OPLi = ni·ti. For example, a 1.50 index layer that is 5 mm thick adds 7.5 mm of optical distance. This is why higher-index materials “slow” the wave’s phase advance.
At oblique incidence, the beam travels a longer distance inside each layer: s = t / cos(θ). The calculator uses Snell’s law to find θ in each layer, then multiplies by n to build OPL. Even modest tilt angles can raise OPL and time-of-flight, which matters in delay lines and precision metrology.
Refraction is computed sequentially with nprevsinθprev = nisinθi. If the implied sine exceeds one, the transmitted angle is not real and the stack reaches total internal reflection. This helps you test designs before committing to angles and indices.
The tool reports time of flight = OPL / c, plus the extra delay compared with vacuum for the same geometric path. Two effective indices are shown: OPL divided by total thickness and OPL divided by geometric path. These summaries are useful when you need a single “stack index.”
If you enter a wavelength, the calculator computes phase shift φ = 2π·OPL/λ and the number of cycles OPL/λ. These values are directly relevant to interferometers, etalons, and coherent imaging. Use consistent wavelength units to avoid scaling errors.
Start with normal incidence to validate your stack, then introduce angle. Use realistic refractive indices (air ≈ 1.0003, water ≈ 1.33, common glass ≈ 1.45–1.52). Keep units consistent for thickness, and enable only the layers you need. Export CSV or PDF to document lab runs and design iterations.
No. At normal incidence OPL equals n times thickness. With tilt, the beam travels farther inside the layer, so OPL increases even more. OPL is an equivalent vacuum distance controlling phase.
The ambient index sets the starting medium for Snell refraction. If you work in air, n0 is near 1.0003. For immersion setups or gases, using the correct n0 improves angle and OPL accuracy.
If Snell’s law requires sin(θ) greater than one, transmission into that layer is not possible. The calculator flags the layer where this happens so you can reduce angle or adjust refractive indices.
It compares the computed travel time to a vacuum path with the same geometric distance through the layers. It isolates the delay caused by refractive index, which is useful for timing and synchronization estimates.
Use OPL/thickness when you want a stack-average index based on physical build height. Use OPL/geometric path when you want an index referenced to the actual traveled distance through the tilted stack.
No. OPL is computed from indices and geometry. Wavelength is only needed if you want phase in radians or cycles. Enter wavelength when analyzing interference, coherence, or phase-sensitive measurements.
This version supports up to five enabled layers. That covers many practical stacks such as window–adhesive–substrate–coating combinations. If you need more layers, the same method can be extended.
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.