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| + | <header style="text-align:center;"> | ||
| + | <h2>Solutions of Savchenko Physics Textbook</h2> | ||
| + | <p class="author"> | ||
| + | Aliaksandr Melnichenka <br/> | ||
| + | October 2023 | ||
| + | </p> | ||
| + | </header> | ||
| + | |||
| + | <h3 id="back-link"><a href="../#2.3">$\leftarrow$Back</a></h3> | ||
| + | |||
| + | <h3> Statement </h3> | ||
| + | <p> | ||
| + | $2.3.41.$ A part of the mass $m$ is detached from the load hanging on the spring of stiffness $k$. To what height will the remaining part of the cargo then rise? | ||
| + | |||
| + | </p> | ||
| + | <center> | ||
| + | <figure> | ||
| + | <img src="statement.png" | ||
| + | loading="lazy" width="100" /> | ||
| + | <figcaption> | ||
| + | For problem $2.3.41$ | ||
| + | </figcaption> | ||
| + | </figure> | ||
| + | </center> | ||
| + | <p> | ||
| + | </p> | ||
| + | |||
| + | <h3>Solution</h3> | ||
| + | <p> | ||
| + | Since there is no interaction with external factors other than breakaway, all the work goes into changing the length of the spring. $E_k=0$! | ||
| + | </p><p> | ||
| + | Small change in the pontential energy of gravity | ||
| + | $$ | ||
| + | dA = mg \, dx | ||
| + | $$ | ||
| + | Small change in the pontential energy of the spring | ||
| + | $$ | ||
| + | dE = kx \, dx | ||
| + | $$ | ||
| + | Law of conservation of energy | ||
| + | $$ | ||
| + | dA = dE | ||
| + | $$ | ||
| + | $$ | ||
| + | mg \, dx = kx \, dx | ||
| + | $$ | ||
| + | $$ | ||
| + | mg \int dx = k \int x \, dx | ||
| + | $$ | ||
| + | From where | ||
| + | $$ | ||
| + | mg \, x = \frac{kx^2}{2} \Rightarrow \boxed{x = \frac{2mg}{k}} | ||
| + | $$ | ||
| + | </p> | ||
| + | |||
| + | <h4>Answer</h4> | ||
| + | <p> | ||
| + | $$x = \frac{2mg}{k}$$ | ||
| + | </p> | ||
| + | |||
| + | <p style="text-align: right; font-style: italic; font-size: 14;"> | ||
| + | Almaskhan Arsen<br> | ||
| + | </p> | ||
| + | |||
| + | |||
| + | <footer class="row container"> | ||
| + | <br> | ||
| + | <p> | ||
| + | <small> © <strong>Savchenko Solutions</strong>, 2023-2024 <br></small> | ||
| + | </p> | ||
| + | <p> | ||
| + | <small>All rights belong to the authors. <br> Commercial use of materials - with the written permission of the authors. <br> astrosander01@gmail.com <br></small> | ||
| + | </p> | ||
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| + | </html> | ||
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| <!DOCTYPE html> | |||
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| <head> | |||
| <meta charset="utf-8"> | |||
| <meta name="viewport" content="width=device-width, initial-scale=1.0"> | |||
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| <meta name="keywords" content="solutions, savchenko, physics problems, olympiad physics, physics book"> | |||
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| <meta property="og:title" content="Savchenko Solutions"> | |||
| <meta property="og:image" content="img/logo.png"> | |||
| <meta property="og:description" content="A website with solutions to physics problems from Savchenko Textbook"> | |||
| <meta name="yandex-verification" content="6cfda41f74038368"> | |||
| <title>Savchenko Solutions</title> | |||
| <link rel="stylesheet" href="https://savchenko-physics.github.io/css/css-latex/style.css"> | |||
| <link rel="icon" href="https://savchenko-physics.github.io/img/logo.png" type="image/png"> | |||
| <script src="https://savchenko-physics.github.io/js/jquery-1.10.1.min.js"></script> | |||
| <script async src="https://cdnjs.cloudflare.com/ajax/libs/mathjax/2.7.7/MathJax.js?config=TeX-MML-AM_CHTML"></script> | |||
| <script type="text/x-mathjax-config"> | |||
| MathJax.Hub.Config({ | |||
| extensions: ['tex2jax.js'], | |||
| jax: ['input/TeX', 'output/HTML-CSS'], | |||
| tex2jax: { | |||
| inlineMath: [['$', '$'], ['$', '$']], | |||
| processEscapes: true, | |||
| processClass: 'tex2jax', | |||
| ignoreClass: 'html' | |||
| }, | |||
| showProcessingMessages: false, | |||
| messageStyle: 'none' | |||
| }); | |||
| </script> | |||
| </head> | |||
| <body style=""> | |||
| <header style="text-align:center;"> | |||
| <h2>Solutions of Savchenko Physics Textbook</h2> | |||
| <p class="author"> | |||
| Aliaksandr Melnichenka <br/> | |||
| October 2023 | |||
| </p> | |||
| </header> | |||
| <h3 id="back-link"><a href="../#2.3">$\leftarrow$Back</a></h3> | |||
| <h3> Statement </h3> | |||
| <p> | |||
| $2.3.41.$ A part of the mass $m$ is detached from the load hanging on the spring of stiffness $k$. To what height will the remaining part of the cargo then rise? | |||
| </p> | |||
| <center> | |||
| <figure> | |||
| <img src="statement.png" | |||
| loading="lazy" width="100" /> | |||
| <figcaption> | |||
| For problem $2.3.41$ | |||
| </figcaption> | |||
| </figure> | |||
| </center> | |||
| <p> | |||
| </p> | |||
| <h3>Solution</h3> | |||
| <p> | |||
| Since there is no interaction with external factors other than breakaway, all the work goes into changing the length of the spring. $E_k=0$! | |||
| </p><p> | |||
| Small change in the pontential energy of gravity | |||
| $$ | |||
| dA = mg \, dx | |||
| $$ | |||
| Small change in the pontential energy of the spring | |||
| $$ | |||
| dE = kx \, dx | |||
| $$ | |||
| Law of conservation of energy | |||
| $$ | |||
| dA = dE | |||
| $$ | |||
| $$ | |||
| mg \, dx = kx \, dx | |||
| $$ | |||
| $$ | |||
| mg \int dx = k \int x \, dx | |||
| $$ | |||
| From where | |||
| $$ | |||
| mg \, x = \frac{kx^2}{2} \Rightarrow \boxed{x = \frac{2mg}{k}} | |||
| $$ | |||
| </p> | |||
| <h4>Answer</h4> | |||
| <p> | |||
| $$x = \frac{2mg}{k}$$ | |||
| </p> | |||
| <p style="text-align: right; font-style: italic; font-size: 14;"> | |||
| Almaskhan Arsen<br> | |||
| </p> | |||
| <footer class="row container"> | |||
| <br> | |||
| <p> | |||
| <small> © <strong>Savchenko Solutions</strong>, 2023-2024 <br></small> | |||
| </p> | |||
| <p> | |||
| <small>All rights belong to the authors. <br> Commercial use of materials - with the written permission of the authors. <br> astrosander01@gmail.com <br></small> | |||
| </p> | |||
| </footer> | |||
| </body> | |||
| </html> | |||