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en/2.7.27.md
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| + | <title>A light rod with weights of mass m_1 and m_2 fixed to its ends rests with its middle on a rigid support. At the initial moment, the rod is held horizontally and then released. With what force does it press on the support immediately after it is released?</title> | ||
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| + | <span><img src="../../img/book.png"></span><span>Savchenko Solutions</span> | ||
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| + | Solutions of Savchenko Problems in Physics <br> | ||
| + | <i><b>knowledge must be free</b></i> | ||
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| + | <h3 id="back-link"><a href="../../#2.7">$\leftarrow$Back</a></h3> | ||
| + | |||
| + | <h3> Statement </h3> | ||
| + | <p> | ||
| + | $2.7.27^*.$ A light rod with weights of mass $m_1$ and $m_2$ fixed to its ends rests with its middle on a rigid support. At the initial moment, the rod is held horizontally and then released. With what force does it press on the support immediately after it is released? | ||
| + | </p> | ||
| + | <center> | ||
| + | <figure> | ||
| + | <img src="2.7.27.png" | ||
| + | loading="lazy" width="230" /> | ||
| + | <figcaption> | ||
| + | For problem $2.7.27^*$ | ||
| + | </figcaption> | ||
| + | </figure> | ||
| + | </center> | ||
| + | <p> | ||
| + | </p> | ||
| + | |||
| + | <h3>Solution</h3> | ||
| + | <p> | ||
| + | Newton's second law for a rotational movement | ||
| + | $$M = I\varepsilon$$ | ||
| + | $$m_1gR - m_2 g R = I\varepsilon\quad(1)$$ | ||
| + | Since there is no slippage: | ||
| + | $$\varepsilon = \frac{a}{R}$$ | ||
| + | Substituting into $(1)$ | ||
| + | $$\boxed{(m_1 - m_2) g R^2 = Ia}\quad(2)$$ | ||
| + | Conservation of angular momentum | ||
| + | $$I\omega = m_1vR + m_2vR\quad(3)$$ | ||
| + | Let's express velocity through angular velocity | ||
| + | $$v=\omega R\quad(4)$$ | ||
| + | After substituting $(4)$ into $(3)$ | ||
| + | $$\boxed{I = (m_1+m_2)R^2} \quad (5)$$ | ||
| + | Let's equate the expressions $(2)$ and $(5)$ | ||
| + | $$(m_1 - m_2) g R^2 = (m_1+m_2)aR^2$$ | ||
| + | After mathematical transformations | ||
| + | $$a = g \frac{m_1 - m_2}{m_1 + m_2}\quad(6)$$ | ||
| + | Describe the forces acting on the vertical axis | ||
| + | $$N = (m_1+m_2)g - a (m_1-m_2)\quad(7)$$ | ||
| + | Substituting the acceleration $(6)$ into expression $(7)$ | ||
| + | $$N = g\cdot\left((m_1+m_2)+ \frac{(m_1-m_2)^2}{m_1+m_2}\right)$$ | ||
| + | From here we find the support reaction force: | ||
| + | $$\boxed{N = \frac{4m_1m_2g}{m_1+m_2}}$$ | ||
| + | </p> | ||
| + | |||
| + | <h4>Answer</h4> | ||
| + | <p> | ||
| + | $$N = 4m_1m_2g/(m_1 + m_2)$$ | ||
| + | </p> | ||
| + | <p style="text-align: right; font-style: italic; font-size: 14;"> | ||
| + | Bakhodirov Mustafa<br> | ||
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| <meta name="description" content="A light rod with weights of mass m_1 and m_2 fixed to its ends rests with its middle on a rigid support. At the initial moment, the rod is held horizontally and then released. With what force does it press on the support immediately after it is released?"> | |||
| <meta name="author" content="Aliaksandr Melnichenka"> | |||
| <meta name="date" content="2023-10" scheme="YYYY-MM"> | |||
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| <a href="../../" style="text-decoration: none;"> | |||
| <div id="logo"> | |||
| <span><img src="../../img/book.png"></span><span>Savchenko Solutions</span> | |||
| </div> | |||
| </a> | |||
| <p class="author"> | |||
| Solutions of Savchenko Problems in Physics <br> | |||
| <i><b>knowledge must be free</b></i> | |||
| </p> | |||
| </header> | |||
| <h3 id="back-link"><a href="../../#2.7">$\leftarrow$Back</a></h3> | |||
| <h3> Statement </h3> | |||
| <p> | |||
| $2.7.27^*.$ A light rod with weights of mass $m_1$ and $m_2$ fixed to its ends rests with its middle on a rigid support. At the initial moment, the rod is held horizontally and then released. With what force does it press on the support immediately after it is released? | |||
| </p> | |||
| <center> | |||
| <figure> | |||
| <img src="2.7.27.png" | |||
| loading="lazy" width="230" /> | |||
| <figcaption> | |||
| For problem $2.7.27^*$ | |||
| </figcaption> | |||
| </figure> | |||
| </center> | |||
| <p> | |||
| </p> | |||
| <h3>Solution</h3> | |||
| <p> | |||
| Newton's second law for a rotational movement | |||
| $$M = I\varepsilon$$ | |||
| $$m_1gR - m_2 g R = I\varepsilon\quad(1)$$ | |||
| Since there is no slippage: | |||
| $$\varepsilon = \frac{a}{R}$$ | |||
| Substituting into $(1)$ | |||
| $$\boxed{(m_1 - m_2) g R^2 = Ia}\quad(2)$$ | |||
| Conservation of angular momentum | |||
| $$I\omega = m_1vR + m_2vR\quad(3)$$ | |||
| Let's express velocity through angular velocity | |||
| $$v=\omega R\quad(4)$$ | |||
| After substituting $(4)$ into $(3)$ | |||
| $$\boxed{I = (m_1+m_2)R^2} \quad (5)$$ | |||
| Let's equate the expressions $(2)$ and $(5)$ | |||
| $$(m_1 - m_2) g R^2 = (m_1+m_2)aR^2$$ | |||
| After mathematical transformations | |||
| $$a = g \frac{m_1 - m_2}{m_1 + m_2}\quad(6)$$ | |||
| Describe the forces acting on the vertical axis | |||
| $$N = (m_1+m_2)g - a (m_1-m_2)\quad(7)$$ | |||
| Substituting the acceleration $(6)$ into expression $(7)$ | |||
| $$N = g\cdot\left((m_1+m_2)+ \frac{(m_1-m_2)^2}{m_1+m_2}\right)$$ | |||
| From here we find the support reaction force: | |||
| $$\boxed{N = \frac{4m_1m_2g}{m_1+m_2}}$$ | |||
| </p> | |||
| <h4>Answer</h4> | |||
| <p> | |||
| $$N = 4m_1m_2g/(m_1 + m_2)$$ | |||
| </p> | |||
| <p style="text-align: right; font-style: italic; font-size: 14;"> | |||
| Bakhodirov Mustafa<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> alex@savchenkosolutions.com <br></small> | |||
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