Translated 3.2.1-3.2.17

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+ <span><img src = "../../img/book.png"><span><span>Savchenko Solutions</span>
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+ Solutions&nbsp;of&nbsp;Savchenko Problems&nbsp;in&nbsp;Physics <br>
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+ <h3 id="back-link"><a href="../../#3.2">$\leftarrow$Back</a></h3>
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+ <h3> Statement </h3>
+ <p>
+ $3.2.10.$ Measurements of the circular frequency of oscillations of a body of mass $m$, fixed in the middle of a tensioned string with length $2 l$, gave the value $\omega$. Find the force of tension of the string.
+ </p>
+
+ <h3>Solution</h3>
+ <p>
+ The total external force acting on the system
+$$ F=2T\sin\varphi $$
+Newton's second law
+$$ m\ddot{x}(t)+2T\sin\varphi=0 $$
+Let's use the approximation for small angles $(\varphi \ll 1)$:
+$$ \sin\varphi\approx\varphi=\frac{x}{l} $$
+Harmonic oscillation equation
+$$ \ddot{x}(t)+\frac{2T}{ml}x(t)=0 $$
+Where does the period of oscillation come from?
+$$ \omega^{*2}=\frac{2T}{ml}\Rightarrow \boxed{T=\frac{ml\omega^{*2}}{2}} $$
+ </p>
+ <p style="text-align: right; font-style: italic; font-size: 14;">
+ Dzikan Mikita<br>
+Aliaksandr Kanashenka
+ </p>
+
+ <h4>Answer</h4>
+ <p>
+ $$T=\frac{ml\omega^{*2}}{2}$$
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