Translated 1.3.16-1.3.30

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+ <meta name="description" content="A spherical tank standing on the ground has a radius of R. What is the lowest speed at which a rock thrown from the ground can fly over the reservoir just by touching its top?">
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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="../../#1.3">$\leftarrow$Back</a></h3>
+
+ <h3> Statement </h3>
+ <p>
+ $1.3.27^*.$ A spherical tank standing on the ground has a radius of $R$. What is the lowest speed at which a rock thrown from the ground can fly over the reservoir just by touching its top?
+ </p>
+
+ <h3>Solution</h3>
+ <p>
+ <p>The stone must be thrown at an angle $\alpha$ to the horizon, satisfying the equations obtained in <a href="../1.3.6" target="_blank">1.3.6</a>:</p>
+<p class="exp">
+$$v_x = v \cos \alpha; \quad v_y = v \sin \alpha - gt;$$
+$$x = vt \cos \alpha; \quad y = vt \sin \alpha - gt^2 / 2.$$
+</p>
+<p>The time it takes for the stone to rise to the maximum height $2R$ is found as</p>
+<p class="exp">
+$$ t_1 = \frac{v_0 \sin \alpha}{g} $$
+</p>
+<p>The maximum height of the stone lift along the vertical axis should be equal to $y_{max} = 2R$, therefore</p>
+<p class="exp">
+$$ \frac{v_0^2 \sin^2 \alpha}{2g} = 2R $$
+</p>
+<p>Determine the value of the initial throw speed</p>
+<p class="exp">
+$$ v_0 = \sqrt{\frac{4gR}{\sin^2 \alpha}} $$
+</p>
+<p>The angle $\alpha$ at which the stone should be thrown is determined from the initial conditions</p>
+<p class="exp">
+$$ v_0t_1 \cos \alpha = \frac{v_0^2 \sin \alpha \cos \alpha}{g}$$
+$$ 2R = \frac{v_0^2 \sin \alpha \cos \alpha}{g}$$
+$$\tan \alpha = 2; \quad \alpha = \text{arctg} \;2 \approx 63^\circ$$
+</p>
+<p>Substituting into the formula for $v_0$</p>
+<p class="exp">
+$$ \fbox{$v_0 = \sqrt{\frac{4gR}{\sin^2 63^\circ}} = \sqrt{5Rg}$} $$
+</p>
+ </p>
+
+ <h4>Answer</h4>
+ <p>
+ $$v = \sqrt{5gR}$$
+ </p>
+
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