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| + | <meta name="description" content="Calculate the inductance of a long solenoid of radius r and length l placed inside a long superconducting tube of radius R along its axis. Number of turns of the solenoid N."> | ||
| + | <meta name="author" content="Aliaksandr Melnichenka"> | ||
| + | <meta name="date" content="2023-10" scheme="YYYY-MM"> | ||
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| + | <title>Calculate the inductance of a long solenoid of radius r and length l placed inside a long superconducting tube of radius R along its axis. Number of turns of the solenoid N.</title> | ||
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| + | <header style="text-align:center;"> | ||
| + | <h2>Solutions of Savchenko Problems in Physics</h2> | ||
| + | <p class="author"> | ||
| + | Aliaksandr Melnichenka <br/> | ||
| + | October 2023 | ||
| + | </p> | ||
| + | </header> | ||
| + | |||
| + | <h3 id="back-link"><a href="../../#11.5">$\leftarrow$Back</a></h3> | ||
| + | |||
| + | <h3> Statement </h3> | ||
| + | <p> | ||
| + | $11.5.11^*.$ Calculate the inductance of a long solenoid of radius $r$ and length $l$ placed inside a long superconducting tube of radius $R$ along its axis. Number of turns of the solenoid $N$. | ||
| + | </p> | ||
| + | <center> | ||
| + | <figure> | ||
| + | <img src="statement.png" | ||
| + | loading="lazy" width="200" /> | ||
| + | <figcaption> | ||
| + | For problem $11.5.11^*$ | ||
| + | </figcaption> | ||
| + | </figure> | ||
| + | </center> | ||
| + | <p> | ||
| + | </p> | ||
| + | |||
| + | <h3>Solution</h3> | ||
| + | <p> | ||
| + | |||
| + | </p> | ||
| + | <center> | ||
| + | <figure> | ||
| + | <img src="draw1.png" | ||
| + | loading="lazy" width="280" /> | ||
| + | <figcaption> | ||
| + | Direction of currents inside the solenoid | ||
| + | </figcaption> | ||
| + | </figure> | ||
| + | </center> | ||
| + | <p> | ||
| + | The following expressions follow from the figure | ||
| + | $$i_\perp=i\cos\alpha$$ | ||
| + | $$i_\parallel=i\sin\alpha$$ | ||
| + | </p> | ||
| + | <center> | ||
| + | <figure> | ||
| + | <img src="draw2.png" | ||
| + | loading="lazy" width="280" /> | ||
| + | <figcaption> | ||
| + | Geometry of the solenoid | ||
| + | </figcaption> | ||
| + | </figure> | ||
| + | </center> | ||
| + | <p> | ||
| + | From the geometry of the solenoid, follows the aspect ratio | ||
| + | $$\sin\alpha = \frac{r}{R}$$ | ||
| + | $$\cos\alpha = \sqrt{1-\frac{r^2}{R^2}}$$ | ||
| + | Ampère's circuital law | ||
| + | $$\oint B\,dl=\mu_0\sum_{k=1}^{N}i_k\Rightarrow B\cdot l=\mu_0 i_\perp N$$ | ||
| + | By definition of the magnetic flux | ||
| + | $$\left\{\begin{matrix} | ||
| + | \Phi=L i \\ | ||
| + | \Phi=NBS\cos\alpha | ||
| + | \end{matrix}\right.$$ | ||
| + | Equating the two equations | ||
| + | $$L i=\mu_0 i \cos\alpha \frac{N}{l}NS\cos\alpha$$ | ||
| + | $$L=\mu_0 \frac{N^2}{l}S\cos^2\alpha$$ | ||
| + | Given the formula for the area of a circle $S=\pi r^2$, we substitute the value of $\cos\alpha$ | ||
| + | $$\boxed{L=\mu_{0}\pi r^{2}\left(1-\frac{r^{2}}{R^{2}}\right)\frac{N^{2}}{l}}$$ | ||
| + | </p> | ||
| + | |||
| + | <h4>Answer</h4> | ||
| + | <p> | ||
| + | $$L=\mu_{0}\pi r^{2}\left(1-\frac{r^{2}}{R^{2}}\right)\frac{N^{2}}{l}$$ | ||
| + | </p> | ||
| + | <p style="text-align: right; font-style: italic; font-size: 14;"> | ||
| + | Lutfulloyev Shukurullo<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> | ||
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| <meta charset="utf-8"> | |||
| <meta name="viewport" content="width=device-width, initial-scale=1.0"> | |||
| <meta http-equiv="content-language" content="en"> | |||
| <meta name="keywords" content="Savchenko Problems in Physics, Savchenko solutions, physics problems, physics olympiad preparation, IPhO, Jaan Kalda"> | |||
| <meta name="description" content="Calculate the inductance of a long solenoid of radius r and length l placed inside a long superconducting tube of radius R along its axis. Number of turns of the solenoid N."> | |||
| <meta name="author" content="Aliaksandr Melnichenka"> | |||
| <meta name="date" content="2023-10" scheme="YYYY-MM"> | |||
| <meta property="og:title" content="Calculate the inductance of a long solenoid of radius r and length l placed inside a long superconducting tube of radius R along its axis. Number of turns of the solenoid N."> | |||
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| <title>Calculate the inductance of a long solenoid of radius r and length l placed inside a long superconducting tube of radius R along its axis. Number of turns of the solenoid N.</title> | |||
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| }); | |||
| </script> | |||
| </head> | |||
| <body style=""> | |||
| <header style="text-align:center;"> | |||
| <h2>Solutions of Savchenko Problems in Physics</h2> | |||
| <p class="author"> | |||
| Aliaksandr Melnichenka <br/> | |||
| October 2023 | |||
| </p> | |||
| </header> | |||
| <h3 id="back-link"><a href="../../#11.5">$\leftarrow$Back</a></h3> | |||
| <h3> Statement </h3> | |||
| <p> | |||
| $11.5.11^*.$ Calculate the inductance of a long solenoid of radius $r$ and length $l$ placed inside a long superconducting tube of radius $R$ along its axis. Number of turns of the solenoid $N$. | |||
| </p> | |||
| <center> | |||
| <figure> | |||
| <img src="statement.png" | |||
| loading="lazy" width="200" /> | |||
| <figcaption> | |||
| For problem $11.5.11^*$ | |||
| </figcaption> | |||
| </figure> | |||
| </center> | |||
| <p> | |||
| </p> | |||
| <h3>Solution</h3> | |||
| <p> | |||
| </p> | |||
| <center> | |||
| <figure> | |||
| <img src="draw1.png" | |||
| loading="lazy" width="280" /> | |||
| <figcaption> | |||
| Direction of currents inside the solenoid | |||
| </figcaption> | |||
| </figure> | |||
| </center> | |||
| <p> | |||
| The following expressions follow from the figure | |||
| $$i_\perp=i\cos\alpha$$ | |||
| $$i_\parallel=i\sin\alpha$$ | |||
| </p> | |||
| <center> | |||
| <figure> | |||
| <img src="draw2.png" | |||
| loading="lazy" width="280" /> | |||
| <figcaption> | |||
| Geometry of the solenoid | |||
| </figcaption> | |||
| </figure> | |||
| </center> | |||
| <p> | |||
| From the geometry of the solenoid, follows the aspect ratio | |||
| $$\sin\alpha = \frac{r}{R}$$ | |||
| $$\cos\alpha = \sqrt{1-\frac{r^2}{R^2}}$$ | |||
| Ampère's circuital law | |||
| $$\oint B\,dl=\mu_0\sum_{k=1}^{N}i_k\Rightarrow B\cdot l=\mu_0 i_\perp N$$ | |||
| By definition of the magnetic flux | |||
| $$\left\{\begin{matrix} | |||
| \Phi=L i \\ | |||
| \Phi=NBS\cos\alpha | |||
| \end{matrix}\right.$$ | |||
| Equating the two equations | |||
| $$L i=\mu_0 i \cos\alpha \frac{N}{l}NS\cos\alpha$$ | |||
| $$L=\mu_0 \frac{N^2}{l}S\cos^2\alpha$$ | |||
| Given the formula for the area of a circle $S=\pi r^2$, we substitute the value of $\cos\alpha$ | |||
| $$\boxed{L=\mu_{0}\pi r^{2}\left(1-\frac{r^{2}}{R^{2}}\right)\frac{N^{2}}{l}}$$ | |||
| </p> | |||
| <h4>Answer</h4> | |||
| <p> | |||
| $$L=\mu_{0}\pi r^{2}\left(1-\frac{r^{2}}{R^{2}}\right)\frac{N^{2}}{l}$$ | |||
| </p> | |||
| <p style="text-align: right; font-style: italic; font-size: 14;"> | |||
| Lutfulloyev Shukurullo<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> | |||