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Question
In the working idea of a telescope's magnifying power, the beam of incident rays is inclined at an angle \[\alpha\] with the principal axis, while the emergent beam is inclined at a greater angle \[\beta\]. This produces:
Options
Linear magnification
Chromatic dispersion
Angular magnification
Resolving power
MCQ
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Solution
The beam of incident rays is inclined at an angle $\alpha$ with the principal axis, and the emergent beam is inclined at a greater angle $\beta$ with the principal axis. Since $\beta > \alpha$, this produces angular magnification, which is the basis of the telescope's magnifying power.
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