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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:

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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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