Thin lens equation
1/F = 1/d + 1/f, so f = d·F / (d − F). Converging lens F > 0, diverging F < 0; f > 0 is a real image behind the lens, f < 0 a virtual one on the object side. Magnification Γ = |f| / d; optical power D = 1/F in dioptres (F in metres).
Drawing the image
- A ray parallel to the axis passes through the focus F′ after a converging lens;
- a ray through the optical centre is undeviated;
- a ray through the front focus leaves parallel to the axis.
Where the refracted rays meet is the image; if only their extensions meet, the image is virtual.
Converging lens cases
- d > 2F — real, inverted, diminished;
- d = 2F — real, inverted, same size;
- F < d < 2F — real, inverted, magnified;
- d = F — no image;
- d < F — virtual, upright, magnified (magnifier).
Spherical mirrors
The same equation holds with F = R/2: concave F > 0, convex F < 0. Real images form in front of the mirror, virtual ones behind it.