A converging lens f=20cm — object at 30cm — find image position and magnification

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Question

An object is placed 30 cm in front of a converging (convex) lens of focal length 20 cm. Find the position of the image and the magnification produced.

Solution — Step by Step

Identify given values and sign convention

Using the standard sign convention (all distances measured from optical centre; distances in the direction of incident light are positive):

  • Object distance: u=30u = -30 cm (object is on the left of lens, so negative)
  • Focal length: f=+20f = +20 cm (converging lens, so positive)
  • Image distance: v=?v = ?

Apply the lens formula

The lens formula is:

1v1u=1f\frac{1}{v} - \frac{1}{u} = \frac{1}{f}

Substituting:

1v130=120\frac{1}{v} - \frac{1}{-30} = \frac{1}{20}

1v+130=120\frac{1}{v} + \frac{1}{30} = \frac{1}{20}

1v=120130\frac{1}{v} = \frac{1}{20} - \frac{1}{30}

Solve for v

Finding a common denominator (LCM of 20 and 30 is 60):

1v=360260=160\frac{1}{v} = \frac{3}{60} - \frac{2}{60} = \frac{1}{60}

v=+60 cm\boxed{v = +60\text{ cm}}

The positive sign means the image is formed on the opposite side of the lens from the object — this is a real image.

Calculate magnification

Linear magnification:

m=vu=+6030=2m = \frac{v}{u} = \frac{+60}{-30} = -2

Interpretation: The magnitude 2 means the image is twice the size of the object. The negative sign means the image is inverted (real and inverted).

Why This Works

The lens formula 1v1u=1f\frac{1}{v} - \frac{1}{u} = \frac{1}{f} is derived from Snell's law applied to paraxial rays through a thin lens. Each surface of the lens refracts light, and the combined effect is captured in this single formula.

The sign of vv tells us the image type:

  • v>0v > 0: real image (on the transmission side, can be captured on screen)
  • v<0v < 0: virtual image (on the same side as the object, cannot be on screen)

Here, the object is between ff and 2f2f (20 cm and 40 cm), at 30 cm. For a convex lens, an object between ff and 2f2f produces a real, inverted, magnified image beyond 2f2f. Our answer of 60 cm confirms this — 60 cm is beyond 40 cm (2f2f).

Alternative Method — Using Cartesian Form

Some textbooks write the lens formula as 1v1u=1f\frac{1}{v} - \frac{1}{u} = \frac{1}{f} and others as 1f=1v1u\frac{1}{f} = \frac{1}{v} - \frac{1}{u}. These are identical. The key is consistent application of the sign convention. Using u=30u = -30:

1f=1v1u    120=1v+130\frac{1}{f} = \frac{1}{v} - \frac{1}{u} \implies \frac{1}{20} = \frac{1}{v} + \frac{1}{30}

Same calculation, same answer.

Common Mistake

⚠️ Common Mistake

Using u=+30u = +30 (forgetting the negative sign). In the standard sign convention, object distance uu is always negative for a real object (because the object is on the same side as incoming light, which is the negative direction). Using u=+30u = +30 gives 1v=120130=160\frac{1}{v} = \frac{1}{20} - \frac{1}{30} = \frac{1}{60}... accidentally getting the right numerical answer but for the wrong reason. When uu is substituted with wrong sign into other problems, you get completely wrong results.

💡 Expert Tip

Quick check for convex lens: when object is at 2f=402f = 40 cm, image is also at 2f=402f = 40 cm and magnification = 1 (same size). Our object at 30 cm is between ff and 2f2f, so image should be beyond 2f2f and magnified. Our answer: v=60v = 60 cm (beyond 40 cm) and m=2|m| = 2 (magnified). This mental check confirms we're on the right track.

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