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A number of factors play a role in determining the focal length ofa lens. First and foremost is the shape of the lens. As a general rule,a lens that is thicker in the middle will converge light, a lens that isthinner in the middle will diverge light. Another important factor is the index of refraction of the lensmaterial, $n_{\text { lens. }}$ For example, imagine comparing two lenses withidentical shapes but made of different materials. The lens with the larger index of refraction bends light more, bringing it to a focus in ashorter distance. As a result, a larger index of refraction implies a focallength with a smaller magnitude. In fact, the focal length of a lenssurrounded by air $(n=1)$ is given by the lens maker's formula:$$\frac{1}{f_{\text { in air }}}=\left(n_{\text { lens }}-1\right)\left(\frac{1}{R_{1}}-\frac{1}{R_{2}}\right)$$A lens is not always surrounded by air, however. More generally, the fluid in which the lens is immersed may have an index ofrefraction given by $n_{\text { finid }} .$ In this case, the focal length is given by$$\frac{1}{f_{\text { in fluid }}}=\left(\frac{n_{\text { lens }}-n_{\text { fluid }}}{n_{\text { fluid }}}\right)\left(\frac{1}{R_{1}}-\frac{1}{R_{2}}\right)$$It follows, then, that the focal lengths of a lens surrounded by airor by a general fluid are related by$$f_{\text { in fluid }}=\left[\frac{\left(n_{\text { lens }}-1\right) n_{\text { fluid }}}{n_{\text { lens }}-n_{\text { fluid }}}\right] f_{\text { in air }}$$This relation shows that the surrounding fluid can change themagnitude of the focal length, or even cause it to become infinite.The fluid can also change the sign of the focal length, which determines whether the lens is diverging or converging.A converging lens with a focal length in air of $f=+5.25 \mathrm{cm}$ is made from ice. What is the focal length of this lens if it isimmersed in benzene? (Refer to Table 26 -2.)$\begin{array}{ll}{\text { A. }-20.7 \mathrm{cm}} & {\text { B. }-18.1 \mathrm{cm}} \\ {\text { C. }-12.8 \mathrm{cm}} & {\text { D. }-11.2 \mathrm{cm}}\end{array}$
$-12.8 \mathrm{cm}$
Physics 103
Chapter 26
Geometrical Optics
Wave Optics
University of Michigan - Ann Arbor
University of Washington
University of Sheffield
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this question. It is about finding the focal line off the lands, uh, off certain reflective index. And that is being, uh, so that's being placed in a fluid, uh, which has, uh, certain effective index as well. Okay, so in this particular question, we are given a converging lens. There is made of ice. Okay. And then the focal hang in air is given to be 5.25 year. Okay, so ah, and it is emerging benzene. Hey. Okay, so you want to find a focal line off this lens? Okay, Shane, we'll be using a formula. The focal line through it is equal to on lens minus one times the refractive index off to it. Divide by the difference and lands minus and to it. Yeah, and then multiplied by the focal length in air. Okay, so the effective index off eyes is 1.31 Is that the sister lens and then the refractive index on fanzine? Yes. You go to 1.50 and then this is a to win. And then the focal lining air is given to be 5.25 p. M. So we can calculate that local and into it. Yes. 1.31 minus one times 1.50 If I buy 1.31 minus 1.50 a multiplied by 5.25 yen. You calculate days you get minus shop. Point it. Yeah, OK. And the answer is C. Right, that's all.
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