Formula & Calculator
Thin Lens Equation
Relates focal length to object and image distances for a thin lens.
Interpretation
1/f = 1/d_o + 1/d_i. Relates focal length f, object distance d_o, and image distance d_i. Used to determine image location for thin lenses.
Variables
| Symbol | Quantity | Unit |
|---|---|---|
| f | Focal length | m |
| d_o | Object distance | m |
| d_i | Image distance | m |
What it means
The thin lens equation is the fundamental formula for locating images formed by thin lenses. It uses the sign convention: positive for real objects and images. It applies to converging and diverging lenses. This equation is used in designing cameras, projectors, microscopes, telescopes, and eyeglasses. It also helps understand the optics of the human eye. The magnification is related: m = −d_i/d_o. Understanding this equation is crucial for optical engineers and anyone working with imaging systems. It is derived from geometry and Fermat’s principle. The equation is also used in ray tracing and in optical design software.
Worked example
Thin Lens Equation – Two Detailed Examples
Real‑World| Parameter | Value |
|---|---|
| do (cm) | 20 |
| f (cm) | 12 |
| Parameter | Value |
|---|---|
| do | 10 |
| f | 8 |
Common mistakes
- Thin lens equation: 1/f = 1/d_o + 1/d_i – sign convention matters.
- Sign convention: For real objects, d_o is positive. For real images, d_i is positive. For virtual images, d_i is negative.
- Focal length f: Positive for converging (convex) lenses, negative for diverging (concave).
- Units: All distances must be in the same units (e.g., cm, m).
- Lens thickness: The equation assumes a thin lens (thickness ≪ radii of curvature) – for thick lenses, use the lensmaker’s equation with principal planes.
Applications
The thin lens equation, 1/f = 1/d_o + 1/d_i, relates the focal length (f) of a thin lens to the object distance (d_o) and image distance (d_i). This is the central formula in geometrical optics for determining image formation. Engineers, opticians, and photographers use it to design camera lenses, eyeglasses, microscopes, and telescopes. By solving for the required focal length, they can achieve the desired magnification or focus. It is also used in machine vision systems to set up proper focus and field of view. The equation assumes thin lenses, but is a good approximation for many practical systems. Understanding this formula is essential for anyone designing or using optical imaging devices.
- Design and selection of camera lenses and projectors
- Prescribing corrective lenses in optometry
- Design of microscopes, telescopes, and magnifiers
- Setting up machine vision and inspection systems
- Educational demonstration of image formation
Frequently Asked Questions
It relates the focal length (f) of a thin lens to the object distance (dₒ) and image distance (dᵢ): 1/f = 1/dₒ + 1/dᵢ. It is the basis for imaging calculations in optics.
f = focal length (positive for converging, negative for diverging).
dₒ = object distance (positive for real objects).
dᵢ = image distance (positive for real images on the opposite side).
Using the Cartesian sign convention: distances are positive in the direction of incident light. For a converging lens, f > 0; for diverging, f < 0. Real images have dᵢ > 0; virtual images have dᵢ < 0.
It is derived from the paraxial approximation using Snell's Law and the geometry of spherical surfaces, assuming the lens thickness is negligible.
Linear magnification m = −dᵢ/dₒ. If |m| > 1, the image is magnified; if negative, the image is inverted.
A converging lens has f = 10 cm. An object is placed 30 cm from the lens. Find the image distance: 1/10 = 1/30 + 1/dᵢ → 1/dᵢ = 1/10 − 1/30 = 2/30 → dᵢ = 15 cm (real image).
It assumes a thin lens (negligible thickness) and paraxial rays (small angles). It does not account for lens aberrations or thick lens effects.
To compute the required focal length for a given field of view and to determine the lens-to-sensor distance to achieve focus at various object distances.
A convex lens is thicker in the middle, converges light, and has positive f. A concave lens is thinner in the middle, diverges light, and has negative f.
By measuring object and image distances and solving the equation, or by using the method of distant object (dₒ ≈ ∞) where f ≈ dᵢ.