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@ -101,16 +101,16 @@ $`\overline{M_T}=-\dfrac{\overline{SA_{ima}}}{\overline{SA_{obj}}}`$ |
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You know $`\overline{SA_{obj}}`$ , calculate $`\overline{SA_{ima}}`$ using (equ. 1) |
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then $`\overline{M_T}`$ with (equ.2), and deduce $`\overline{A_{ima}B_{ima}}`$. |
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! *USEFUL 1° :<br> |
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! *USEFUL 1* :<br> |
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! The conjunction equation and the transverse magnification equation for a plane mirror |
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! are obtained by rewriting these two equations for a spherical mirror in the limit when |
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! $`|\overline{SC}|\longrightarrow\infty`$. |
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! Then we get for a plane mirror : $`\overline{SA_{ima}}=\overline{SA_{obj}}`$ and |
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! $`\overline{M_T}=+1`$. |
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! *USEFUL 2° :<br> |
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! *You can find* the conjunction and the transverse magnification **equations for a plane mirror directly from |
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! those of the spherical mirror**, with the following assumptions :<br> |
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! *USEFUL 2* :<br> |
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! *You can find* the conjunction and the transverse magnification *equations for a plane mirror directly from |
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! those of the spherical mirror*, with the following assumptions :<br> |
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! $`n_{eme}=-n_{inc}`$<br> |
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! (to memorize : medium of incidence=medium of emergence, therefor same speed of light, but direction |
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! of propagation reverses after reflection on the mirror)<br> |
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