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Exercises · 9.9

Q.An object of size 3.0 cm3.0\ \text{cm} is placed 14 cm14\ \text{cm} in front of a concave lens of focal length 21 cm21\ \text{cm}. Describe the image produced by the lens. What happens if the object is moved further away from the lens?

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Using the lens formula and magnification for a concave lens, the image is virtual, erect, diminished (size 1.8 cm1.8\ \text{cm}), and located 8.4 cm8.4\ \text{cm} from the lens on the same side as the object. Moving the object farther makes the image even smaller and closer to the lens (approaching the focal point).

Why the Lens Formula Works for Concave Lenses

A concave lens always diverges incoming light rays. No matter where you place the object in front of it, the refracted rays never actually meet — they only appear to come from a point on the same side as the object. That means the image is always virtual, erect, and diminished.

The standard lens formula 1f=1v−1u\frac{1}{f} = \frac{1}{v} - \frac{1}{u} works for all thin lenses if you follow the sign convention strictly. For a concave lens, the focal length is taken as negative. The object distance uu is always negative (object is on the incident side). The image distance vv comes out negative, confirming the image is on the same side as the object — virtual.

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

Sign convention: distances measured from the optical centre. Distances against the incident light direction are negative.


Step-by-step solution

1. Write down the given data with proper signs

Object size ho=+3.0 cmh_o = +3.0\ \text{cm} (positive by convention for erect object).

Object distance u=−14 cmu = -14\ \text{cm} (negative because object is in front of the lens, against incident light).

Focal length of concave lens f=−21 cmf = -21\ \text{cm} (negative for diverging lens).

2. Apply the lens formula to find vv

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

Substitute:

1−21=1v−1−14\frac{1}{-21} = \frac{1}{v} - \frac{1}{-14}

That minus sign on uu is crucial — careful:

1−21=1v+114\frac{1}{-21} = \frac{1}{v} + \frac{1}{14}

Now isolate 1v\frac{1}{v}:

1v=−121−114\frac{1}{v} = -\frac{1}{21} - \frac{1}{14}

Find a common denominator (42):

1v=−242−342=−542\frac{1}{v} = -\frac{2}{42} - \frac{3}{42} = -\frac{5}{42}

So:

v=−425=−8.4 cmv = -\frac{42}{5} = -8.4\ \text{cm}

The negative sign tells us the image is on the same side as the object — virtual.

Watch out

A common mistake is forgetting that uu is negative. If you plug u=+14u = +14, you get v=+8.4v = +8.4, which would wrongly suggest a real image on the opposite side. Always check the sign convention.

3. Find the magnification and image size

Magnification m=hiho=vum = \frac{h_i}{h_o} = \frac{v}{u}

m=−8.4−14=+0.6m = \frac{-8.4}{-14} = +0.6

The positive sign means the image is erect (same orientation as object). The magnitude 0.60.6 means the image is smaller than the object.

Image height:

hi=m×ho=0.6×3.0=1.8 cmh_i = m \times h_o = 0.6 \times 3.0 = 1.8\ \text{cm}

4. Describe the image fully

The image is:

  • Virtual (rays appear to diverge from it)
  • Erect (same orientation as object)
  • Diminished (size 1.8 cm1.8\ \text{cm})
  • Located 8.4 cm8.4\ \text{cm} from the lens on the same side as the object
Tip

For any concave lens, the image always lies between the optical centre and the focal point on the object side. Here ∣v∣=8.4 cm|v| = 8.4\ \text{cm} is less than ∣f∣=21 cm|f| = 21\ \text{cm}, which matches this rule.

5. What happens when the object moves farther away?

Let the object distance increase (more negative, say u=−30 cmu = -30\ \text{cm}). From the lens formula:

1v=1f+1u(with signs)\frac{1}{v} = \frac{1}{f} + \frac{1}{u} \quad \text{(with signs)} …

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