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Signed Mirror Equation and Image Magnification

Relate object and image distances, focal length, curvature and signed or areal magnification for concave, convex and plane mirrors using a declared Cartesian sign convention.

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How to use this calculator

  1. Enter the known values in the units shown. Results update as you type.
  2. Where results are editable, change one to solve backwards. Lock a value to hold it fixed.
  3. Use the worked example to check the method. Reset restores the starting fields.

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Formula and method

For a concave mirror with an object at u=βˆ’30 cm and focal length f=βˆ’10 cm, the image is at v=βˆ’15 cm. Signed magnification is βˆ’0.5 and areal magnification is 0.25.

1/f=1/u+1/v; r=2f; m=βˆ’v/u; A=(v/u)Β². For a plane mirror, v=βˆ’u, m=A=1 and focal length/radius are unbounded.

Worked example

Enter these known values and leave the other values blank.

Mirror type
Concave mirror
Object distance (βˆ’)
-30 cm
Focal length (βˆ’)
-10 cm
Image distance (+/βˆ’)
-15 cm
Radius of curvature (βˆ’)
-20 cm
Areal magnification (+)
0.25
Linear magnification (+/βˆ’)
-0.5

Assumptions and limitations

  • The source uses Cartesian signed distances, not the convention in which real object distance and concave focal length are positive. Keep one convention throughout: real-object u<0, concave f<0, convex f>0; image v<0 is real and v>0 virtual. Signed magnification m=βˆ’v/u indicates orientation, while areal magnification A=mΒ² discards orientation.
  • The spherical-mirror relations use the paraxial approximation and r=2f. Large apertures, off-axis rays and spherical aberration are outside this scalar model.
  • A finite convex mirror with a real object gives 0<m<1 and 0<A<1. A concave mirror gives negative m for a real inverted image, or m>1 for an upright virtual image. A plane mirror gives m=A=1, v=βˆ’u and has unbounded focal length and radius; the two original forced infinity outputs are represented by this explicit note.
  • Areal magnification alone cannot determine signed image orientation. The retained concave inverse v=u√A chooses the real-image negative-v branch. Supply signed linear magnification or focal length to identify a virtual-image branch. Given signed v and A, u=βˆ’|v|/√A is the unique real-object distance. No claim of a unique image branch from A alone is made.
  • An object at the focal position has no finite image distance. That singular result remains an error; the plane-mirror presentation correction does not hide nonfinite results in other controls.
  • Controls use bounded exact finite-decimal preflight. Nonzero values below 10⁻¹⁰⁰⁰⁰ in equation base units are unsupported. Arithmetic uses 64 significant digits; tiny finite results use scientific notation and an overflowing or zero-losing unit conversion is withheld with an error. Near the focal singularity, rounding can limit the reliable image distance.

Common questions

Why are object distances negative?

The declared Cartesian axis points in the direction of incident light. The real object lies on the negative side of the mirror vertex. Other textbooks use another convention; transform every signed distance consistently when comparing answers.

Can I determine orientation from areal magnification?

No. A=mΒ² loses the sign of the linear magnification. The concave area-only image inverse uses the captured real-image branch; use signed m or focal length to specify a virtual image.

Why are plane focal length and curvature not numeric fields?

A perfect plane mirror is the infinite-radius limit. Its focal length and radius are unbounded; a finite numeric value would contradict that model. Object distance, image distance and magnification remain usable.

References

Correct unique physical signs in convex/plane areal inverses for u<0,v>0, and concave object inverse u=-abs(v)/sqrt(A) for both real and virtual images. Preserve the captured concave image-from-area negative-v branch and all signed linear magnification/focal length inverse controls. All13originalequations/variants are pinned. Preserve all17originalcondition bodies; replace sign comparisons equivalently and append physical image/magnification domains. Plane f/r are FORCED output-only and never finite in the original graph: only these exact two display fields become hidden, while the authored sign-convention note preserves the unbounded curvature/focal-length meaning. No generic nonfinite suppression.

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