Describe the characteristics of an image formed by a converging lens

Published by Patrick Mutisya · 14 days ago

IGCSE Physics 0625 – Thin Lenses: Converging Lens Image Characteristics

3.2.3 Thin Lenses – Converging Lens

Learning Objective

Describe the characteristics of an image formed by a converging (convex) lens.

Key Concepts

  • Converging lenses are thicker at the centre than at the edges and cause parallel rays to converge.
  • Image characteristics depend on the object distance (\$u\$) relative to the focal length (\$f\$).
  • Two fundamental equations:

    • Lens formula: \$\frac{1}{f} = \frac{1}{v} + \frac{1}{u}\$
    • Magnification: \$m = \frac{h'}{h} = -\frac{v}{u}\$ where \$h'\$ is image height and \$h\$ is object height.

  • Sign convention (Cartesian):

    • Object distance \$u\$ is negative (object is on the incoming‑light side).
    • Image distance \$v\$ is positive for real images (formed on the opposite side) and negative for virtual images.
    • Focal length \$f\$ is positive for converging lenses.

Image Characteristics for Different Object Positions

Object PositionRelation to Focal LengthImage Position (\$v\$)Image SizeOrientationNature
Beyond \$2f\$ (farther than twice the focal length)\$u > 2f\$Between \$f\$ and \$2f\$ (real, on opposite side)Reduced (\$|m| < 1\$)InvertedReal
At \$2f\$ (centre of curvature)\$u = 2f\$At \$2f\$ (real)Same size (\$|m| = 1\$)InvertedReal
Between \$f\$ and \$2f\$\$f < u < 2f\$Beyond \$2f\$ (real)Magnified (\$|m| > 1\$)InvertedReal
At \$f\$ (object at focal point)\$u = f\$Image at infinity (parallel rays)Highly magnified (theoretically infinite)InvertedReal (practically not formed)
Inside \$f\$ (closer than focal length)\$0 < u < f\$Virtual, on same side as objectMagnified (\$|m| > 1\$)UprightVirtual

Ray Diagram Description

To construct a ray diagram for a converging lens, use three principal rays:

  1. Parallel Ray: A ray parallel to the principal axis emerges from the lens passing through the focal point on the opposite side.
  2. Focal Ray: A ray directed towards the focal point on the object side emerges from the lens parallel to the principal axis.
  3. Centre Ray: A ray passing through the optical centre of the lens continues in a straight line without deviation.

The point where the refracted rays intersect (or appear to intersect) determines the image position, size, and nature.

Suggested diagram: Ray diagram for a converging lens showing the three principal rays for an object placed between \$f\$ and \$2f\$, producing a real, inverted, magnified image beyond \$2f\$.

Practical Applications

  • Camera lenses (real, inverted images recorded on film or sensor).
  • Magnifying glasses (object placed within \$f\$, producing a virtual, upright, magnified image).
  • Projectors (object placed beyond \$f\$, projecting a real, inverted image onto a screen).

Common Misconceptions

  • “All images formed by converging lenses are inverted.” – Not true for objects placed within the focal length; those produce upright virtual images.
  • “A larger object always gives a larger image.” – Image size also depends on object distance; a small object far from the lens can produce a larger image than a larger object placed near the focal point.
  • “The focal length changes with object distance.” – The focal length is a property of the lens and remains constant for a given medium.

Summary Checklist

  • Identify the object distance relative to \$f\$ and \$2f\$.
  • Use the lens formula to calculate image distance \$v\$.
  • Calculate magnification \$m = -v/u\$ to determine size and orientation.
  • Classify the image as real or virtual, upright or inverted, magnified or reduced.
  • Confirm the result with a ray diagram.