Translated 9.2.10-9.2.17

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+ <meta name="author" content="Aliaksandr Melnichenka">
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+ <span><img src="../../img/book.png"></span><span>Savchenko Solutions</span>
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+ <h3 id="back-link"><a href="../../#9.2">$\leftarrow$Back</a></h3>
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+ <h3> Statement </h3>
+ <p>
+ $9.2.11.$ How many times will the magnetic field induction in the center of a ring with current decrease if it is bent at an angle $\alpha$? The current in the ring does not change.
+ </p>
+
+ <h3>Solution</h3>
+ <p>
+
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+<center>
+ <figure>
+ <img src="https://savchenkosolutions.com/9/9.2.11/9.2.11_1.png"
+ loading="lazy" width="200" />
+ <figcaption>
+ Magnetic field induction at the center of a bent ring
+ </figcaption>
+ </figure>
+</center>
+<p>
+In <a href="../9.2.10">9.2.10</a> we obtained an expression for the magnetic induction at the center of the ring
+$$ B_0 = \frac{\mu_0 I}{2R}\quad(1) $$
+Due to superposition, the magnetic induction at the center of one semicircle will be half of this value:
+$$ B_1 = B_2 = \frac{B_0}{2} = \frac{\mu_0 I}{4R}\quad(2) $$
+From the drawing, it is clear that the angle between the vectors $\vec{B}_1$ and $\vec{B}_2$ is equal to $\alpha$
+$$ (\vec{B_1},\vec{B_2})=\alpha $$
+The total vector of magnetic induction is equal to the vector sum of the components of magnetic induction of two rings $\vec{B}_1$ and $\vec{B}_2$
+$$ \vec{B} = \vec{B_1} + \vec{B_2} $$
+We will find the modulus of this vector using the cosine law.
+$$ B = \sqrt{{B_1}^2 + {B_2}^2 - 2B_1 B_2 \cos\alpha} $$
+Taking into account the expression $(2)$, we find the total magnetic induction as
+$$ B= \frac{\mu_0 I}{4R}\sqrt{2-2\cos\alpha} = \frac{\mu_0 I}{2R}\cdot\sin\frac{\alpha}{2}\quad(3) $$
+Dividing the expression $(3)$ by $(1)$, we obtain the desired ratio
+$$ \boxed{\frac{B}{B_0} = \sin\frac{\alpha}{2}} $$
+
+ </p>
+
+ <h4>Answer</h4>
+ <p>
+ $$\frac{B}{B_0} =\sin\frac{\alpha}{2}$$
+ </p>
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