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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+ <p class="author">
+ 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>
+
+ <h3> Statement </h3>
+ <p>
+ $3.2.12.$ Determine the flight time of a stone from one pole of the Earth to the other along a straight tunnel dug through the center. Consider Earth's density constant, its radius equal to $6400$ km.
+</p>
+<center>
+ <figure>
+ <img src="https://savchenkosolutions.com/3/3.2.12/statement.png"
+ loading="lazy" width="150" />
+ <figcaption>
+ For problem $3.2.12$
+ </figcaption>
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+<p>
+ </p>
+
+ <h3>Solution</h3>
+ <p>
+
+</p>
+<center>
+ <figure>
+ <img src="https://savchenkosolutions.com/3/3.2.12/3.2.12_1.png"
+ loading="lazy" width="200" />
+ <figcaption>
+ Body at distance $x$ from the planet's core
+ </figcaption>
+ </figure>
+</center>
+<p>
+The body, at a distance $x$ from the core, will be subject to the gravitational force of attraction caused by the inner layers of the planet of density $\rho$, forming a sphere of radius $x$. The mass of this part of the earth
+$$ M_\oplus = \frac{4}{3} \rho\pi x^3 $$
+Gravitational force acting on a rock at depth $x$
+$$ F_G = \frac{GmM_\oplus}{x^2}=mg\frac{x}{R} $$
+Newton's Second Law
+$$ m\ddot{x}(t)=-\frac{mg}{R}x(t) $$
+Let's write the equation of harmonic oscillations
+$$ \ddot{x}(t)+\frac{g}{R}x(t)=0 $$
+The angular frequency of such oscillations
+$$ \omega=\sqrt{\frac{g}{R}}\Rightarrow T=2\pi\sqrt{\frac{R}{g}} $$
+Since we are interested in the flight time only in one direction, we take half of this period.
+$$ \boxed{t=\frac{T}{2}=\pi\sqrt{\frac{R}{g}}=42\text{ min}} $$
+</p>
+ <p style="text-align: right; font-style: italic; font-size: 14;">
+ Dzikan Mikita<br>
+ Aliaksandr Kanashenka<br>
+ </p>
+
+ <h4>Answer</h4>
+ <p>
+ $$t=42\text{ min}$$
+ </p>
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