Added Luis's English solution of 13.2.11
en/13.2.11.md
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| + | <!DOCTYPE html> | ||
| + | <html lang="en"> | ||
| + | |||
| + | <head> | ||
| + | <meta charset="UTF-8" /> | ||
| + | <meta name="viewport" content="width=device-width, initial-scale=1.0" /> | ||
| + | <meta http-equiv="content-language" content="en"> | ||
| + | <script async src="https://www.googletagmanager.com/gtag/js?id=G-DDMB38YMLD"></script> | ||
| + | |||
| + | <title>Savchenko Solutions</title> | ||
| + | <meta property="og:image" content="img/logo.png"> | ||
| + | <meta property="og:title" content="Savchenko Solutions"/> | ||
| + | <meta name="description" | ||
| + | content="A website with solutions to physics problems from Savenko Textbook" /> | ||
| + | <meta name="keywords" content="physics, olympiads, ipho, savchenko" /> | ||
| + | <link rel="stylesheet" href="https://savchenko-physics.github.io/css/css-latex/style.css" /> | ||
| + | <link rel="icon" type="image/x-icon" href="https://savchenko-physics.github.io/img/favicon.ico"> | ||
| + | </head> | ||
| + | |||
| + | <body id="top"> | ||
| + | <header> | ||
| + | <h2>Solutions of Savchenko Physics Textbook</h2> | ||
| + | <p class="author"> | ||
| + | Aliaksandr Melnichenka <br/> | ||
| + | October 2023 | ||
| + | </p> | ||
| + | </header> | ||
| + | |||
| + | <main> | ||
| + | <article> | ||
| + | <h3 id="back-link"><a href="../">$\leftarrow$Back</a></h3> | ||
| + | |||
| + | <h4>Statement</h4> | ||
| + | <p> | ||
| + | $13.2.11$ | ||
| + | What minimum angle of incidence should have a light ray that incides over a group of plane transparent plates (each one with refraction index decreasing $k$ times respect to the upper to it) such that the ray doesn't pass the group? The refraction index of the upper plate is $n$ and the amount of plates is $N$. | ||
| + | </p> | ||
| + | <center> | ||
| + | <figure> | ||
| + | <img src="statement.png" | ||
| + | loading="lazy" alt="13.2.11" width="300" /> | ||
| + | <figcaption> | ||
| + | For problem 13.2.11 | ||
| + | </figcaption> | ||
| + | </figure> | ||
| + | </center> | ||
| + | <h4>Solution</h4> | ||
| + | <p class="TxtSolutions"> | ||
| + | Let's consider the following figure | ||
| + | </p> | ||
| + | <center> | ||
| + | <figure> | ||
| + | <img src="draw.png" | ||
| + | loading="lazy" alt="13.2.11" width="450" /> | ||
| + | <figcaption> | ||
| + | Ray's path through plates | ||
| + | </figcaption> | ||
| + | </figure> | ||
| + | </center> | ||
| + | <p class ="TxtSolutions"> | ||
| + | Applying Snell's law for each interphase between media | ||
| + | </p> | ||
| + | <center> | ||
| + | $n_0 \sin{\alpha} = n_1 \sin{\alpha_1} = n \sin{\alpha_1}$ | ||
| + | </center> | ||
| + | <center> | ||
| + | $n \sin{\alpha_1} = n_2 \sin{\alpha_2}$ | ||
| + | </center> | ||
| + | <center> | ||
| + | $n_2 \sin{\alpha_2} = n_3 \sin{\alpha_3}$ | ||
| + | </center> | ||
| + | <center> | ||
| + | $\vdots$ | ||
| + | </center><center> | ||
| + | $n_{N-1} \sin{\alpha_{N-1}} = n_N \sin{\frac{\pi}{2}} = n_N$ | ||
| + | </center> | ||
| + | <p calss="TxtSolutions"> | ||
| + | It's known that $n_2 = \frac{n}{k}$, $n_3 = \frac{n_2}{k}=\frac{n}{k^2}$, and so on. Then, $n_N=\frac{n}{k^{N-1}}$. The $N$-th refraction angle is $\frac{\pi}{2}$ beacause the ray doesn't pass this latest plate, i.e., there is a total reflection. | ||
| + | </p> | ||
| + | <center> | ||
| + | $n_m \sin{\alpha} = \frac{n}{k^{N-1}}$ | ||
| + | </center> | ||
| + | <p class="TxtSolutions"> | ||
| + | If exterior medium is air, $n_m = 1$, | ||
| + | </p> | ||
| + | <center> | ||
| + | $\boxed{\sin{\alpha}=\frac{n}{k^{N-1}}}$ | ||
| + | </center> | ||
| + | <p class="TxtSolutions"> | ||
| + | This angle $\alpha$ is the critical angle of the internal total reflection for this group of plates. | ||
| + | </p> | ||
| + | <p class="TxtSolutions" style="text-align: right; font-style: italic; font-size: 14;"> | ||
| + | BSc. Luis Daniel Fernández Quintana<br> | ||
| + | Physics Department (FCNE)<br> | ||
| + | Universidad de Oriente, Cuba<br> | ||
| + | </p> | ||
| + | </article> | ||
| + | </main> | ||
| + | |||
| + | <script> | ||
| + | MathJax = { | ||
| + | tex: { | ||
| + | inlineMath: [['$', '$'],], | ||
| + | }, | ||
| + | } | ||
| + | const typeFaceToggle = document.getElementById('typeface-toggle') | ||
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| + | typeface.textContent = document.body.classList.contains('libertinus') ? 'Libertinus' : 'Latin Modern' | ||
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| + | |||
| + | const darkModeToggle = document.getElementById('dark-mode-toggle') | ||
| + | darkModeToggle.addEventListener('click', () => { | ||
| + | document.body.classList.toggle('latex-dark') | ||
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| + | </body> | ||
| + | |||
| + | </html> | ||
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| <!DOCTYPE html> | |||
| <html lang="en"> | |||
| <head> | |||
| <meta charset="UTF-8" /> | |||
| <meta name="viewport" content="width=device-width, initial-scale=1.0" /> | |||
| <meta http-equiv="content-language" content="en"> | |||
| <script async src="https://www.googletagmanager.com/gtag/js?id=G-DDMB38YMLD"></script> | |||
| <title>Savchenko Solutions</title> | |||
| <meta property="og:image" content="img/logo.png"> | |||
| <meta property="og:title" content="Savchenko Solutions"/> | |||
| <meta name="description" | |||
| content="A website with solutions to physics problems from Savenko Textbook" /> | |||
| <meta name="keywords" content="physics, olympiads, ipho, savchenko" /> | |||
| <link rel="stylesheet" href="https://savchenko-physics.github.io/css/css-latex/style.css" /> | |||
| <link rel="icon" type="image/x-icon" href="https://savchenko-physics.github.io/img/favicon.ico"> | |||
| </head> | |||
| <body id="top"> | |||
| <header> | |||
| <h2>Solutions of Savchenko Physics Textbook</h2> | |||
| <p class="author"> | |||
| Aliaksandr Melnichenka <br/> | |||
| October 2023 | |||
| </p> | |||
| </header> | |||
| <main> | |||
| <article> | |||
| <h3 id="back-link"><a href="../">$\leftarrow$Back</a></h3> | |||
| <h4>Statement</h4> | |||
| <p> | |||
| $13.2.11$ | |||
| What minimum angle of incidence should have a light ray that incides over a group of plane transparent plates (each one with refraction index decreasing $k$ times respect to the upper to it) such that the ray doesn't pass the group? The refraction index of the upper plate is $n$ and the amount of plates is $N$. | |||
| </p> | |||
| <center> | |||
| <figure> | |||
| <img src="statement.png" | |||
| loading="lazy" alt="13.2.11" width="300" /> | |||
| <figcaption> | |||
| For problem 13.2.11 | |||
| </figcaption> | |||
| </figure> | |||
| </center> | |||
| <h4>Solution</h4> | |||
| <p class="TxtSolutions"> | |||
| Let's consider the following figure | |||
| </p> | |||
| <center> | |||
| <figure> | |||
| <img src="draw.png" | |||
| loading="lazy" alt="13.2.11" width="450" /> | |||
| <figcaption> | |||
| Ray's path through plates | |||
| </figcaption> | |||
| </figure> | |||
| </center> | |||
| <p class ="TxtSolutions"> | |||
| Applying Snell's law for each interphase between media | |||
| </p> | |||
| <center> | |||
| $n_0 \sin{\alpha} = n_1 \sin{\alpha_1} = n \sin{\alpha_1}$ | |||
| </center> | |||
| <center> | |||
| $n \sin{\alpha_1} = n_2 \sin{\alpha_2}$ | |||
| </center> | |||
| <center> | |||
| $n_2 \sin{\alpha_2} = n_3 \sin{\alpha_3}$ | |||
| </center> | |||
| <center> | |||
| $\vdots$ | |||
| </center><center> | |||
| $n_{N-1} \sin{\alpha_{N-1}} = n_N \sin{\frac{\pi}{2}} = n_N$ | |||
| </center> | |||
| <p calss="TxtSolutions"> | |||
| It's known that $n_2 = \frac{n}{k}$, $n_3 = \frac{n_2}{k}=\frac{n}{k^2}$, and so on. Then, $n_N=\frac{n}{k^{N-1}}$. The $N$-th refraction angle is $\frac{\pi}{2}$ beacause the ray doesn't pass this latest plate, i.e., there is a total reflection. | |||
| </p> | |||
| <center> | |||
| $n_m \sin{\alpha} = \frac{n}{k^{N-1}}$ | |||
| </center> | |||
| <p class="TxtSolutions"> | |||
| If exterior medium is air, $n_m = 1$, | |||
| </p> | |||
| <center> | |||
| $\boxed{\sin{\alpha}=\frac{n}{k^{N-1}}}$ | |||
| </center> | |||
| <p class="TxtSolutions"> | |||
| This angle $\alpha$ is the critical angle of the internal total reflection for this group of plates. | |||
| </p> | |||
| <p class="TxtSolutions" style="text-align: right; font-style: italic; font-size: 14;"> | |||
| BSc. Luis Daniel Fernández Quintana<br> | |||
| Physics Department (FCNE)<br> | |||
| Universidad de Oriente, Cuba<br> | |||
| </p> | |||
| </article> | |||
| </main> | |||
| <script> | |||
| MathJax = { | |||
| tex: { | |||
| inlineMath: [['$', '$'],], | |||
| }, | |||
| } | |||
| const typeFaceToggle = document.getElementById('typeface-toggle') | |||
| const typeface = document.getElementById('typeface') | |||
| typeFaceToggle.addEventListener('click', () => { | |||
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| typeface.textContent = document.body.classList.contains('libertinus') ? 'Libertinus' : 'Latin Modern' | |||
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| darkModeToggle.addEventListener('click', () => { | |||
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