Mirror Equation Calculator

Solve for focal length, image or object distance using 1/f = 1/dₒ + 1/dᵢ for curved mirrors.

🪞 Optics📐 Mirror Equation💡 Reflection
Focal length (f) cm
Object distance (dₒ) cm

Sign convention: concave f > 0; convex f < 0; real image dᵢ > 0 (same side as object for mirrors)

⚠️ Check values and sign conventions.

What Is Mirror Equation?

The mirror equation 1/f = 1/dₒ + 1/dᵢ has the same form as the thin lens equation but with different sign conventions. For mirrors, the focal length f = R/2 where R is the radius of curvature. Concave mirrors have positive f; convex mirrors have negative f. Real images form in front of the mirror (same side as object), with positive dᵢ.

Concave mirrors can form both real and virtual images depending on object position. Beyond 2f: real, inverted, smaller image. At 2f: real, inverted, same size. Between f and 2f: real, inverted, magnified. At f: no image (parallel rays). Inside f: virtual, upright, magnified (like a makeup mirror). Convex mirrors always form virtual, upright, smaller images.

Magnification m = −dᵢ/dₒ. For mirrors, the sign convention gives m positive for upright images and negative for inverted images. |m| > 1 means enlarged; |m| < 1 means reduced. A makeup mirror (concave, object inside f) gives m > 1 and upright; a car side mirror (convex) gives m < 1 with a wide field of view.

Mirror applications span from cosmetics to astronomy. Concave mirrors focus parallel rays (satellite dishes, solar concentrators, telescope primaries, searchlights). Convex mirrors diverge rays and show wide-angle views (security mirrors, car door mirrors, the inside of spherical lamp globes). Parabolic mirrors avoid spherical aberration for point objects at infinity.

Formula Reference Table

Solve ForFormulaNotes
Image distance1/dᵢ = 1/f − 1/dₒdᵢ > 0: real; dᵢ < 0: virtual
Object distance1/dₒ = 1/f − 1/dᵢdₒ > 0: real object
Focal length1/f = 1/dₒ + 1/dᵢf = R/2 (R = radius of curvature)
Magnificationm = −dᵢ/dₒ−: inverted; + : upright
Concavef > 0Can form real or virtual images
Convexf < 0Only virtual, upright, smaller images

3 Worked Examples

Example 1
Concave Mirror — Shaving/Makeup

Face 15 cm from concave mirror, f = 25 cm.

  • 1/dᵢ = 1/25 − 1/15 = 3/75 − 5/75 = −2/75
  • dᵢ = −37.5 cm (virtual, behind mirror)
  • m = −(−37.5)/15 = +2.5 (upright, 2.5× magnified)
✓ Virtual image 37.5 cm behind mirror; m = +2.5 (enlarged, upright)
Example 2
Concave Mirror — Telescope Primary

Parallel starlight (dₒ → ∞) on concave f = 500 mm mirror.

  • 1/dᵢ = 1/f − 1/∞ = 1/500
  • dᵢ = 500 mm = f (light focuses at focal point)
  • A small secondary mirror redirects light to the eyepiece
✓ Image forms at focal point, dᵢ = f = 500 mm
Example 3
Convex Security Mirror

Object 3 m from convex mirror, f = −0.5 m.

  • 1/dᵢ = 1/(−0.5) − 1/3 = −2 − 0.333 = −2.333
  • dᵢ = −0.429 m (virtual, behind mirror)
  • m = −(−0.429)/3 = +0.143 (upright, much smaller — wide field of view)
✓ dᵢ = −43 cm; m = +0.143 — small upright wide-angle image

Real-World Applications

🔭
Telescopes
Reflecting telescopes use concave primary mirrors (f up to 10+ m). Hubble's 2.4 m mirror focuses starlight; secondary mirror redirects to instruments. Parabolic primaries eliminate spherical aberration for parallel starlight.
🌞
Solar Concentrators
Parabolic trough mirrors focus sunlight to a line (linear concentrator) or point (dish concentrator). Solar thermal plants use large concave mirrors to concentrate sunlight, generating steam for turbines at 400°C.
💄
Makeup/Shaving Mirrors
Concave mirrors with object inside f produce virtual, magnified, upright images. Typical f = 20–40 cm gives 2–5× magnification at comfortable viewing distance.
🚗
Rearview Mirrors
Passenger side car mirrors are convex (f = −R/2 with R ≈ −0.8 to −1.2 m). Wide field of view at the cost of image size: objects appear smaller and farther than they are (warning text on mirror).
🔦
Searchlights & Headlights
A bulb at the focal point of a concave mirror produces a parallel beam. Parabolic reflectors maximize beam intensity for flashlights, headlights, and searchlights.

Common Mistakes to Avoid

⚠️
Wrong sign for convex vs concave

Concave: f > 0 (center of curvature and focus are on the same side as the object). Convex: f < 0. Getting this wrong completely changes the result.

⚠️
Using lens sign convention for mirrors

For mirrors, real images have positive dᵢ (on same side as object). For lenses, real images have positive dᵢ (on opposite side from object). The magnitude formula is the same but sign conventions differ.

⚠️
Not recognizing virtual image from negative dᵢ

dᵢ < 0 for mirrors means the image is virtual (behind the mirror, where reflected rays appear to diverge from). It cannot be projected on a screen.

⚠️
Forgetting f = R/2

The focal length of a spherical mirror is half the radius of curvature. A concave mirror with R = 20 cm has f = 10 cm.

⚠️
Sign of magnification

m = −dᵢ/dₒ. For concave mirror with real image: dᵢ > 0, so m < 0 (inverted). For virtual image: dᵢ < 0, so m > 0 (upright).

Frequently Asked Questions

How does a mirror form an image?
Concave mirrors obey the law of reflection at each point on the curved surface. Parallel rays converge at the focal point (f). Diverging rays from objects at various distances converge at image points satisfying 1/f = 1/dₒ + 1/dᵢ. This is derived from geometry of paraxial rays (small angles to the optical axis).
Why is a convex mirror's image always virtual and smaller?
For convex f < 0: 1/dᵢ = 1/f − 1/dₒ = negative − positive = more negative → dᵢ < 0 always. So image is always virtual. Magnification m = −dᵢ/dₒ: dᵢ is small and negative, dₒ is large and positive → |m| < 1. Convex mirrors always produce smaller, upright, virtual images.
What is the center of curvature?
For a spherical mirror, the center of curvature C is at distance R = 2f from the mirror surface. Objects placed at C produce real, inverted, same-size images at C. Objects between C and f produce real, inverted, magnified images beyond C. This is the basis of all reflecting astronomical telescopes.
How is a parabolic mirror different from a spherical mirror?
Spherical mirrors have spherical aberration — rays far from the center focus at slightly different distances, blurring the image. Parabolic mirrors focus all parallel rays to exactly the same focal point (no spherical aberration). Telescopes and searchlights use parabolic mirrors; household mirrors (approximately flat) and makeup mirrors (slow spherical) don't need parabolic precision.
What is the difference between concave and convex mirror image types?
Concave mirror: objects outside f → real, inverted, variable size; object inside f → virtual, upright, magnified. Convex mirror: always virtual, upright, smaller regardless of object position. The sign of f determines which case applies.
How do satellite dish antennas use mirror optics?
A satellite dish is a concave parabolic reflector. Microwave signals from satellites are parallel rays (source at ∞), and the dish focuses them to the feedhorn at the focal point (dᵢ = f). The dish size relative to λ determines gain and angular resolution.
What are Cassegrain and Newtonian telescope designs?
Newtonian: large concave primary, small flat secondary deflects beam to the side — eyepiece at the side of the tube. Cassegrain: concave primary, small convex secondary reflecting beam back through a hole in the primary — eyepiece at the back. Hubble uses Ritchey-Chrétien (hyperbolic primary and secondary) to eliminate coma.
Why does a spoon show an inverted image?
A spoon's bowl is a concave mirror. When held at arm's length (dₒ > 2f), the image is real, inverted, and reduced. Bringing it closer (dₒ < f) gives a virtual, upright, magnified image. The transition near f gives a blurry, infinite-distance image.

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Formula Explorer connections

Interpretation: This relationship connects light propagation, geometry, wavelength, refraction, interference or image formation. Assumption: Use a consistent sign convention and units. Paraxial rays, thin elements, coherent light, vacuum wavelength or ideal optical components may be assumed.

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