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Q.(a) Draw the ray diagram of a (astronomical) telescope when the final image is focused at the least distance of distinct vision.

(b) A small object is placed at a depth 'd' inside a tank full of liquid of refractive index μ. Show that the radius of the base of the cone (on the liquid's upper surface) through which light from the object escapes the liquid is r = d / √(μ² - 1). OR
(a) Explain how the focal length of a lens depends on
(i) the colour of the incident light and
(ii) the nature of the surrounding medium.
(b) An object of height 3 cm is placed 60 cm from a convex mirror of focal length 30 cm. Determine the position and size of the image formed.
Tripura TbseHigher Secondary (+2 Stage) Examination 2025Subjective· 5mImportance★★★★★
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Figure — Part (a) says 'Draw the ray diagram of a (astronomical) telescope when the final image is focused at the least
Figure — Part (a) says 'Draw the ray diagram of a (astronomical) telescope when the final image is focused at the least

The astronomical telescope's objective always forms a small real image at its focal plane; when the eyepiece is adjusted to view that image from just inside its own focal length, the final virtual image lands at the near point. Separately, light escaping a liquid surface from a submerged point source forms a circle of radius r = d*tan(theta_c) = d/root(mu^2-1), where theta_c is the critical angle.

(a) Ray diagram (final image at near point D): Parallel rays from a distant object are collected by the objective lens (large aperture, long focal length fof_o), which converges them to form a real, inverted, diminished intermediate image at its focal plane. For normal adjustment this image would sit exactly at the eyepiece's focal point too (giving a final image at infinity), but to place the FINAL image at the near point D, the eyepiece is moved slightly CLOSER to the intermediate image (a distance a little less than fef_e) -- the eyepiece then acts as a simple magnifier, taking rays diverging from a point just inside its focus and bending them into a diverging beam that appears to the eye to come from a large, virtual, inverted image at distance D. (The full ray diagram shows: parallel rays -> objective -> converge to a point on its focal plane -> diverge again toward the eyepiece -> emerge as a diverging beam reaching the eye, traced back to a large virtual image at D.)

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