A ray parallel to the principal axis passes through the focal point of a convex lens (or appears to diverge from the focus of a concave lens).
A ray through the optical center travels undeviated.
A ray directed toward the focus emerges parallel to the axis.
Image position and size follow from the lens formula:
\[ \frac{1}{f} = \frac{1}{v} - \frac{1}{u} \]
and magnification:
\[ m = \frac{v}{u} \]
Step 1: Refraction at a Thin Lens. Using the small-angle (paraxial) approximation, a lens redirects rays according to Snell’s law at each surface. For a convex lens, rays converge; for a concave lens, rays diverge.
Step 2: Principal Rays (Construction). To locate images quickly:
Parallel ray → passes through \( F \) (convex) / appears from \( F \) (concave).
Central ray → through optical center \( O \), undeviated.
Focal ray → aimed at \( F \), emerges parallel to the axis.
Step 3: Nature of Images.
Convex Lens:
Object beyond \( 2F \): real, inverted, diminished (image between \( F \) and \( 2F \)).
Object at \( 2F \): real, inverted, same size (image at \( 2F \)).
Object between \( F \) and \( 2F \): real, inverted, magnified (image beyond \( 2F \)).
Object inside \( F \): virtual, erect, magnified (image on same side).
Concave Lens: always forms virtual, erect, and diminished images.