Thin lens equation and microscope: Difference between revisions
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== Theory == | == Theory == | ||
We have <math>\frac1{i_1} = \ | We have <math>\frac1{i_1} = \frac1{f_1} - \frac1{o_1} </math>. The distance between the lenses is <math>L</math>, thus <math>i_1 + o_2 = L</math> which gives <math>o_2 = L-i_1</math>. Thus we have for the image distance of the second lens | ||
<math>\begin{align*} | |||
\frac1{i_2} &= \frac1{f_2} - \frac1{o_2} \\ | |||
&= \frac1{f_2} - \frac1{L-i_1} \\ | |||
&= \frac1{f_2} - \frac1{L-(i_1)} \\ | |||
\end{align*}</math> | |||
Magnification (for the thin lens) is <math>m = - \frac io</math>. | Magnification (for the thin lens) is <math>m = - \frac io</math>. |
Revision as of 20:20, 11 August 2021
Introduction
The thin lens equation to compound microscope with two lenses. The lens that is closer to the object is called objective and the the one closer to the eye is called ocular. The distance between the lenses is .
Theory
We have . The distance between the lenses is , thus which gives . Thus we have for the image distance of the second lens
Failed to parse (syntax error): {\displaystyle \begin{align*} \frac1{i_2} &= \frac1{f_2} - \frac1{o_2} \\ &= \frac1{f_2} - \frac1{L-i_1} \\ &= \frac1{f_2} - \frac1{L-(i_1)} \\ \end{align*}}
Magnification (for the thin lens) is .