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| + | <meta name="author" content="Aliaksandr Melnichenka"> | ||
| + | <meta name="date" content="2023-10" scheme="YYYY-MM"> | ||
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| + | <h2>Solutions of Savchenko Problems in Physics</h2> | ||
| + | <p class="author"> | ||
| + | Aliaksandr Melnichenka <br/> | ||
| + | October 2023 | ||
| + | </p> | ||
| + | </header> | ||
| + | |||
| + | <h3 id="back-link"><a href="../../#1.5">$\leftarrow$Back</a></h3> | ||
| + | |||
| + | <h3> Statement </h3> | ||
| + | <p> | ||
| + | $1.5.10.$ On the inner surface of a fixed cylinder of radius $2r$, a wheel of radius $r$ rolls without slipping. Find the path of the wheel rim point. | ||
| + | </p> | ||
| + | <center> | ||
| + | <figure> | ||
| + | <img src="https://savchenkosolutions.com/1/1.5.10/statement.png" | ||
| + | loading="lazy" width="150" /> | ||
| + | <figcaption> | ||
| + | For problem $1.5.10$ | ||
| + | </figcaption> | ||
| + | </figure> | ||
| + | </center> | ||
| + | <p> | ||
| + | </p> | ||
| + | |||
| + | <h3>Solution</h3> | ||
| + | <p> | ||
| + | <center> | ||
| + | <figure> | ||
| + | <img src="https://savchenkosolutions.com/1/1.5.10/01.gif" | ||
| + | loading="lazy" width="250" /> | ||
| + | <figcaption> | ||
| + | Construction of a hypocycloid at $r= \frac{R}{2}$ | ||
| + | </figcaption> | ||
| + | </figure> | ||
| + | </center> | ||
| + | <p> | ||
| + | This trajectory is the so-called <a href="https://en.wikipedia.org/wiki/Hypocycloid" target="_blank">Hypocycloid</a><br><br> | ||
| + | Given by the parametric equation: | ||
| + | </p> | ||
| + | <p class="exp"> | ||
| + | $$ \begin{gathered}\begin{cases}x=r(k-1)\left(\cos t+\frac{\cos((k-1)t)}{k-1}\right)\\y=r(k-1)\left(\sin t-\frac{\sin((k-1)t)}{k-1}\right)&\end{cases}\end{gathered} $$ | ||
| + | </p> | ||
| + | <p> | ||
| + | For $r= R/2$, this trajectory lies on the diameter | ||
| + | </p> | ||
| + | <h3> Proof: </h3> | ||
| + | <p>Let the circles initially touch at point $A$, lying on the $Ox$ axis, where point $O$ is the center of the large circle. The coordinates of point $A$ are $ (kr, 0) $, where $ k = \frac{R}{r} $. Let us consider how the coordinates of point $A$, tied to the rolling circle ($A$ goes to $ A' $), change. Let the small circle roll so that its center moves from point $ C' $ to point $ C'' $ and rotates relative to point $ O $ by angle $ t $.</p> | ||
| + | <p>First, it can be shown that the rotation of the small circle relative to its center (i.e. the angle between $ CA $ and $ C' A' $) is equal to $ t - kt = -(k-1)t $. Second, the coordinates of point $ C' $ will be as follows: $ (cos(t)(k-1)r, sin(t)(k-1)r) $. Then, knowing where the center of the rolling circle will go and at what angle it has turned relative to this center, we can write down the coordinates of point $ A' $:</p> | ||
| + | <p class="exp"> | ||
| + | $ \begin{cases} | ||
| + | x = cos(t)(k-1)r + cos((k-1)t)r \\ | ||
| + | y = sin(t)(k-1)r - sin((k-1)t)r | ||
| + | \end{cases} $ | ||
| + | </p> | ||
| + | </p> | ||
| + | |||
| + | <h4>Answer</h4> | ||
| + | <p> | ||
| + | The trajectory of the wheel rim point passes along the cylinder diameter. | ||
| + | </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> aliaksandr@savchenkosolutions.com <br></small> | ||
| + | </p> | ||
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| <meta name="description" content="On the inner surface of a fixed cylinder of radius 2r, a wheel of radius r rolls without slipping. Find the path of the wheel rim point."> | |||
| <meta name="author" content="Aliaksandr Melnichenka"> | |||
| <meta name="date" content="2023-10" scheme="YYYY-MM"> | |||
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| </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="../../#1.5">$\leftarrow$Back</a></h3> | |||
| <h3> Statement </h3> | |||
| <p> | |||
| $1.5.10.$ On the inner surface of a fixed cylinder of radius $2r$, a wheel of radius $r$ rolls without slipping. Find the path of the wheel rim point. | |||
| </p> | |||
| <center> | |||
| <figure> | |||
| <img src="https://savchenkosolutions.com/1/1.5.10/statement.png" | |||
| loading="lazy" width="150" /> | |||
| <figcaption> | |||
| For problem $1.5.10$ | |||
| </figcaption> | |||
| </figure> | |||
| </center> | |||
| <p> | |||
| </p> | |||
| <h3>Solution</h3> | |||
| <p> | |||
| <center> | |||
| <figure> | |||
| <img src="https://savchenkosolutions.com/1/1.5.10/01.gif" | |||
| loading="lazy" width="250" /> | |||
| <figcaption> | |||
| Construction of a hypocycloid at $r= \frac{R}{2}$ | |||
| </figcaption> | |||
| </figure> | |||
| </center> | |||
| <p> | |||
| This trajectory is the so-called <a href="https://en.wikipedia.org/wiki/Hypocycloid" target="_blank">Hypocycloid</a><br><br> | |||
| Given by the parametric equation: | |||
| </p> | |||
| <p class="exp"> | |||
| $$ \begin{gathered}\begin{cases}x=r(k-1)\left(\cos t+\frac{\cos((k-1)t)}{k-1}\right)\\y=r(k-1)\left(\sin t-\frac{\sin((k-1)t)}{k-1}\right)&\end{cases}\end{gathered} $$ | |||
| </p> | |||
| <p> | |||
| For $r= R/2$, this trajectory lies on the diameter | |||
| </p> | |||
| <h3> Proof: </h3> | |||
| <p>Let the circles initially touch at point $A$, lying on the $Ox$ axis, where point $O$ is the center of the large circle. The coordinates of point $A$ are $ (kr, 0) $, where $ k = \frac{R}{r} $. Let us consider how the coordinates of point $A$, tied to the rolling circle ($A$ goes to $ A' $), change. Let the small circle roll so that its center moves from point $ C' $ to point $ C'' $ and rotates relative to point $ O $ by angle $ t $.</p> | |||
| <p>First, it can be shown that the rotation of the small circle relative to its center (i.e. the angle between $ CA $ and $ C' A' $) is equal to $ t - kt = -(k-1)t $. Second, the coordinates of point $ C' $ will be as follows: $ (cos(t)(k-1)r, sin(t)(k-1)r) $. Then, knowing where the center of the rolling circle will go and at what angle it has turned relative to this center, we can write down the coordinates of point $ A' $:</p> | |||
| <p class="exp"> | |||
| $ \begin{cases} | |||
| x = cos(t)(k-1)r + cos((k-1)t)r \\ | |||
| y = sin(t)(k-1)r - sin((k-1)t)r | |||
| \end{cases} $ | |||
| </p> | |||
| </p> | |||
| <h4>Answer</h4> | |||
| <p> | |||
| The trajectory of the wheel rim point passes along the cylinder diameter. | |||
| </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> aliaksandr@savchenkosolutions.com <br></small> | |||
| </p> | |||
| </footer> | |||
| </body> | |||
| </html> | |||