Lensmaker's Equation Calculator

Use the lensmaker's equation to find focal length, optical power, and image distance from lens curvature, refractive index, and thickness.

Lens Type
Converging (+)
Determined by sign of focal length
Thin Lens Focal Length
48.375 mm
1/f = (n/n_m − 1)(1/R₁ − 1/R₂) — zero-thickness approximation
Thick Lens Focal Length
49.213 mm
Includes thickness correction term for real lenses
Optical Power
20.3198 m⁻¹ (diopters)
Reciprocal of focal length in meters
Surface 1 Power
10.3360 m⁻¹
Refractive power of the first surface alone
Surface 2 Power
10.3360 m⁻¹
Refractive power of the second surface alone
Image Distance
65.27 mm
Real, inverted — from thin lens equation 1/f = 1/d_o + 1/d_i
Magnification
-0.3264×
M = −d_i/d_o (negative = inverted)
Lens Diagram
R₁
R₂
f = 49.2 mm
MaterialnFocal Length (mm)Power (m⁻¹)
Crown Glass (BK7)1.516848.3720.6720
Flint Glass (SF11)1.784731.8631.3880
Fused Silica1.458554.5318.3400
Polycarbonate1.58642.6623.4400
Diamond2.41717.6456.6800
Water1.33375.0813.3200
ZnSe (IR)2.40317.8256.1200
Planning notes, formulas, and examples

About the Lensmaker's Equation Calculator

The lensmaker's equation is the fundamental relationship connecting a lens's physical properties — its two surface curvatures, refractive index, and thickness — to its optical power and focal length. First derived for thin lenses, the equation 1/f = (n−1)(1/R₁ − 1/R₂) shows that steeper curvatures and higher refractive indices produce shorter focal lengths and stronger focusing. The thick-lens form adds a correction for the finite separation between the two refracting surfaces.

Understanding the lensmaker's equation is essential for optical design, from simple magnifiers to complex multi-element camera objectives. It governs the relationship between lens shape (biconvex, plano-convex, meniscus), material choice, and optical performance. The sign convention for radii of curvature follows the standard optics convention: positive if the center of curvature is to the right of the surface, negative if to the left.

This calculator supports both thin-lens and thick-lens calculations, computes surface powers, optical power in diopters, and (when an object distance is provided) uses the thin-lens equation to find image location and magnification. A material comparison table shows how different glasses and crystals affect the focal length for the same lens geometry, helping optical designers choose materials efficiently.

When This Page Helps

Use this calculator when you need a fast focal-length estimate from lens geometry without switching to a full optical design package.

It is useful for classroom optics, rough lens selection, and early-stage design work where curvature, material, and thickness choices need to be compared quickly. It also gives a consistent first-pass answer before you move into thicker lenses, material swaps, or more detailed ray tracing.

How to Use the Inputs

  1. Select a preset lens configuration or enter custom radii of curvature.
  2. Enter "inf" for a flat surface (plano-convex or plano-concave lenses).
  3. Input the lens refractive index (or select from common materials).
  4. Enter the center thickness for thick-lens correction (use 0 for thin approximation).
  5. Optionally enter an object distance to compute image location and magnification.
  6. Review the focal length, power, and material comparison table.
Formula used
Thin lens: 1/f = (n/n_m − 1)(1/R₁ − 1/R₂). Thick lens: 1/f = (n−1)[1/R₁ − 1/R₂ + (n−1)d/(nR₁R₂)]. Image: 1/f = 1/d_o + 1/d_i. M = −d_i/d_o.

Example Calculation

Result: f ≈ 48.4 mm (thick), 48.5 mm (thin)

A symmetric biconvex BK7 lens (n=1.5168) with R₁=50mm, R₂=−50mm: thin-lens f ≈ 1/[0.5168×(1/50−1/(−50))]mm ≈ 48.4 mm.

Tips & Best Practices

  • Lock down the sign convention before entering radii because a single sign error flips the result immediately.
  • Use the thick-lens form when center thickness is not negligible relative to focal length.
  • Compare candidate glass indices at the design wavelength because refractive index changes with color.
  • Treat the result as paraxial first-pass optics; aberrations and principal plane shifts still need a fuller design check.

Practical Guidance

The lensmaker's equation is best used as a geometry-driven estimate. It is ideal for checking whether a planned curvature and glass choice land near the target focal length before you move into a more complete model with principal planes, wavelength dependence, and aberration control. That makes it a good first check for lab setups, classroom examples, and simple optical prototypes.

Common Pitfalls

Most errors come from sign convention mistakes and from mixing thin-lens intuition with a lens that is not actually thin. If the lens is strongly curved, thick, or used across a wide field, you should treat this result as a starting point rather than the final design value. Material dispersion and coating choices can also shift real performance away from the paraxial estimate.

Sources & Methodology

Last updated:

Frequently Asked Questions

  • R is positive if the center of curvature is to the right (toward the image side), negative if to the left. For a biconvex lens: R₁ > 0, R₂ < 0.