For R2 (right surface): positive = bulging right, negative = bulging left.
Results
Lens Visualization
Parameter Sensitivity
Lens Comparison
| Design | n | R₁ | R₂ | d | f (m) | P (D) | Type |
|---|
Lensmaker Reference
| Symbol | Quantity | SI Unit | Description |
|---|---|---|---|
| f | Focal length | m | Distance from lens to focal point |
| n | Refractive index | — | Optical index ratio (lens / medium) |
| R₁ | First surface radius | m | Curvature radius of left surface |
| R₂ | Second surface radius | m | Curvature radius of right surface |
| d | Center thickness | m | Lens thickness (thick-lens mode) |
| P | Optical power | D (m⁻¹) | P = 1/f (f in meters) |
| C | Surface curvature | m⁻¹ | C = 1/R |
Refractive Index Reference
| Material | n (approx.) | Notes |
|---|---|---|
| Air | 1.000 | Standard reference |
| Water | 1.333 | At 20°C, 589 nm |
| Fused silica | 1.458 | At 589 nm |
| Crown glass | 1.517 | Typical BK7 |
| Acrylic (PMMA) | 1.490 | Common optical plastic |
| Polycarbonate | 1.585 | High-index plastic |
| Flint glass | 1.620 | Dense flint |
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Object / Image Analysis
How to Use This Tool
- Select Thin Lens or Thick Lens mode.
- Choose what variable to Solve For (f, P, n, R₁, or R₂).
- Select a lens material preset or enter a custom refractive index.
- Enter R₁ and R₂ with your preferred units.
- Follow the sign convention shown above — positive = convex, negative = concave.
- In Thick Lens mode, enter the center thickness d.
- Select the surrounding medium (air, water, or custom).
- Click Calculate to see results, steps, visualization, and sensitivity chart.
- Use Geometry Presets to quickly explore common lens shapes.
- Add designs to the Comparison table to study different configurations.
What This Tool Offers
Assumptions & Limitations
- Paraxial approximation — rays are close to the optical axis.
- Spherical surfaces — assumes perfect spherical curvature.
- Homogeneous, isotropic material — uniform refractive index.
- Monochromatic light — single wavelength (dispersion not modeled).
- Thin-lens approximation — lens thickness is negligible (d → 0).
- Thick-lens model — includes center thickness but neglects higher-order effects.
- No aberrations — spherical, chromatic, and other aberrations are not modeled.
- Manufacturing tolerances — real lenses vary from ideal values.
- Environmental effects — temperature, pressure, and humidity are ignored.
References & Further Reading
- Hecht, E. (2017). Optics, 5th ed. Pearson.
- Born, M., & Wolf, E. (2019). Principles of Optics, 7th ed. Cambridge.
- Smith, W. J. (2007). Modern Optical Engineering, 4th ed. McGraw-Hill.
- NIST (2023). Refractive Index Database. nist.gov.
- Schott AG. (2023). Optical Glass Data Sheets. schott.com.
Variables
| Symbol | Quantity | Unit |
|---|---|---|
| f | Focal length | m |
| n | Lens refractive index | |
| R1 | Radius of curvature of first surface | m |
| R2 | Radius of curvature of second surface | m |
What it means
The lensmaker’s equation relates the focal length of a thin lens to its refractive index (n) and the radii of curvature of its surfaces (R₁ and R₂). The sign convention is important. This equation is used by optical designers to calculate lens curvatures for desired focal lengths. It is fundamental for designing camera lenses, eyeglasses, microscope objectives, and many other optical systems. Understanding this equation is essential for lens manufacturing and optical engineering. It assumes the lens is in air and is thin; for thick lenses, a more complex form is used.
Worked example
Lensmaker's Equation – Two Detailed Examples
Real‑World| Parameter | Value |
|---|---|
| n | 1.5 |
| R1 (cm) | 20 |
| R2 (cm) | −20 |
| Parameter | Value |
|---|---|
| n | 1.5 |
| f (cm) | 30 |
| R2 | ∞ |
Common mistakes
- Lensmaker’s equation: 1/f = (n−1)·(1/R₁ − 1/R₂) – for a thin lens in air.
- Sign convention for radii: R₁ is the radius of curvature of the first surface (light incidence side). R₂ of the second. Positive if the centre of curvature is on the outgoing side (for light).
- n: Refractive index of the lens material relative to air – must be > 1.
- Units: R₁, R₂, and f in the same units (e.g., metres).
- Assumes: Thin lens in air – for lenses in other media, adjust (n_lens/n_medium − 1).
Applications
The lensmaker's equation, 1/f = (n−1)(1/R₁ − 1/R₂), relates the focal length of a thin lens to its refractive index (n) and the radii of curvature (R₁, R₂) of its two surfaces. This is used by optical engineers to design lenses with specific focal lengths, to select materials, and to optimise lens shapes for aberration control. It is essential in designing lenses for cameras, microscopes, telescopes, and eyeglasses. By choosing appropriate radii and glass types, engineers can achieve the desired optical properties. This equation also underpins the design of complex lens systems. Understanding it is fundamental for anyone involved in lens manufacturing or optical system design.
- Optical lens design and manufacturing
- Selection of glass materials for desired focal lengths
- Design of achromatic and apochromatic lens systems
- Camera lens and microscope objective design
- Educational understanding of lens curvature effects
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