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Exercises · 9.14

Q.(a) A giant refracting telescope at an observatory has an objective lens of focal length 15 m15\ \text{m}. If an eyepiece of focal length 1.0 cm1.0\ \text{cm} is used, what is the angular magnification of the telescope?

(b) If this telescope is used to view the moon, what is the diameter of the image of the moon formed by the objective lens? The diameter of the moon is 3.48×106 m3.48 \times 10^{6}\ \text{m}, and the radius of lunar orbit is 3.8×108 m3.8 \times 10^{8}\ \text{m}.
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For a telescope in normal adjustment, angular magnification is the ratio of objective to eyepiece focal lengths. The image diameter formed by the objective is found using the small-angle approximation: θ≈object sizedistance\theta \approx \frac{\text{object size}}{\text{distance}}, and then d=fo⋅θd = f_o \cdot \theta. Here, M=1500M = 1500 and the image diameter is 13.7 cm13.7\ \text{cm}.

Concept and Intuition

A refracting telescope works by collecting light from a distant object with a large objective lens, forming a real, inverted image at its focal plane. The eyepiece then acts as a magnifying glass to view that image. The angular magnification tells us how many times larger the angle subtended at the eye becomes compared to the naked eye.

For a distant object, the angle subtended at the naked eye is essentially the same as the angle subtended at the objective. The eyepiece then magnifies the intermediate image. In normal adjustment (final image at infinity), the angular magnification is simply:

M=fofeM = \frac{f_o}{f_e}

where fof_o is the focal length of the objective and fef_e is the focal length of the eyepiece.

For part (b), the objective forms an image of the moon at its focal plane. Since the moon is very far away, we can use the small-angle approximation: the angle subtended by the moon at the objective is θ≈diameter of moondistance to moon\theta \approx \frac{\text{diameter of moon}}{\text{distance to moon}}. The image size hih_i is then hi=fo⋅θh_i = f_o \cdot \theta.


Step-by-step Solution

1. Convert units to be consistent.

The objective focal length is fo=15 mf_o = 15\ \text{m}. The eyepiece focal length is fe=1.0 cm=0.01 mf_e = 1.0\ \text{cm} = 0.01\ \text{m}.

2. Calculate angular magnification.

Using the formula for normal adjustment:

M=fofe=150.01=1500M = \frac{f_o}{f_e} = \frac{15}{0.01} = 1500

This means the telescope makes the moon appear 1500 times larger in angular size than with the naked eye.

Watch out

A common mistake is to forget unit conversion — using fe=1.0f_e = 1.0 without converting to metres would give M=15M = 15, which is wrong by a factor of 100.

3. Find the angle subtended by the moon at the objective.

The moon’s diameter Dm=3.48×106 mD_m = 3.48 \times 10^6\ \text{m}.

The distance to the moon (radius of lunar orbit) R=3.8×108 mR = 3.8 \times 10^8\ \text{m}.

Since the moon is very far, the angle θ\theta (in radians) is:

θ≈DmR=3.48×1063.8×108\theta \approx \frac{D_m}{R} = \frac{3.48 \times 10^6}{3.8 \times 10^8}

Calculate: …

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