Thin-lens lensmaker equation
1/f = (n−1)(1/R₁ − 1/R₂)
Signed surface curvatures determine ideal optical power in air.
Estimate thin-lens focal length for the same spherical lens forms used by the Multi-Stage Lens Ray Simulator.
Access: Free to use, no installation, and No account required.
The result uses the simulator’s thin-lens lensmaker estimate. Finite thickness, wavelength dispersion, aspheres, aberrations, aperture, and surrounding media other than air require a fuller optical model.
For a thin lens in air, optical power depends on refractive index and the signed curvatures of the two surfaces. Positive focal length indicates convergence; negative focal length indicates divergence.
Use the Lens Focal Length Calculator to estimate thin-lens focal length and optical power for the spherical biconvex, biconcave, plano, and meniscus geometries used by the Lens Ray Simulator.
1/f = (n−1)(1/R₁ − 1/R₂)
Signed surface curvatures determine ideal optical power in air.
Φ = 1/f
When f is expressed in metres, optical power is in diopters.
The thin-lens lensmaker relation connects refractive index with the signed radii of the two refracting surfaces. The sign of optical power determines whether the idealized lens converges or diverges paraxial rays.
The focused model assumes a thin lens in air and uses a compact geometry parameterization. Real optical design can require finite center thickness, wavelength-dependent refractive index, aspheric surfaces, aperture, aberrations, decenter/tilt, and surrounding media.
Choose biconvex, R = 250 mm, refractive index n = 1.517, and no flip.
Result: The positive sign indicates a converging thin lens in the simulator's sign convention.
In this sign convention, negative focal length indicates a diverging lens.
A larger refractive-index contrast bends rays more strongly at the same surface curvature, increasing optical power and reducing focal-length magnitude.
Not by itself. Multi-element photographic optics require surface-by-surface ray tracing with thickness, spacing, glass dispersion, aperture, and aberration analysis.
Case: Move refractive index toward 1 while keeping curvature fixed.
Expected: Optical power should approach zero and focal length magnitude should grow very large.
Case: Double both signed radius magnitudes for the same lens form and index.
Expected: Focal length magnitude should approximately double in the thin-lens model.
Shared with the Geometrical Optics Workbench, which traces rays surface by surface.
Open the source workbench →Read calculation and source methodology →