Translated 9.1.6-9.1.15
en/9.1.11.md
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| + | <meta property="og:title" content="a) A wire frame in the form of a circle with current can rotate about the horizontal axis OO^\prime. The mass of a unit length of the wire is \rho, the current in the frame is I. The frame is in a magnetic field of induction B, directed along the gravitational field. Determine the angle of deviation of the plane of the circle from the vertical. b) A wire frame in the form of a circle has a wire jumper along the diameter, parallel to the horizontal axis OO^\prime, about which the frame can rotate. The mass of a unit length of the frame and the jumper is the same and is equal to \rho. The current entering the frame is equal to I. The frame is in a magnetic field of induction B, directed parallel to the gravitational field. At what angle from the vertical will the frame deviate?"> | ||
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| + | <meta property="og:description" content="a) A wire frame in the form of a circle with current can rotate about the horizontal axis OO^\prime. The mass of a unit length of the wire is \rho, the current in the frame is I. The frame is in a magnetic field of induction B, directed along the gravitational field. Determine the angle of deviation of the plane of the circle from the vertical. b) A wire frame in the form of a circle has a wire jumper along the diameter, parallel to the horizontal axis OO^\prime, about which the frame can rotate. The mass of a unit length of the frame and the jumper is the same and is equal to \rho. The current entering the frame is equal to I. The frame is in a magnetic field of induction B, directed parallel to the gravitational field. At what angle from the vertical will the frame deviate?"> | ||
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| + | <title>a) A wire frame in the form of a circle with current can rotate about the horizontal axis OO^\prime. The mass of a unit length of the wire is \rho, the current in the frame is I. The frame is in a magnetic field of induction B, directed along the gravitational field. Determine the angle of deviation of the plane of the circle from the vertical. b) A wire frame in the form of a circle has a wire jumper along the diameter, parallel to the horizontal axis OO^\prime, about which the frame can rotate. The mass of a unit length of the frame and the jumper is the same and is equal to \rho. The current entering the frame is equal to I. The frame is in a magnetic field of induction B, directed parallel to the gravitational field. At what angle from the vertical will the frame deviate?</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> | ||
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| + | <h3 id="back-link"><a href="../../#9.1">$\leftarrow$Back</a></h3> | ||
| + | |||
| + | <h3> Statement </h3> | ||
| + | <p> | ||
| + | $9.1.11.$ a) A wire frame in the form of a circle with current can rotate about the horizontal axis $OO^\prime$. The mass of a unit length of the wire is $\rho$, the current in the frame is $I$. The frame is in a magnetic field of induction B, directed along the gravitational field. Determine the angle of deviation of the plane of the circle from the vertical. </p><p> | ||
| + | b) A wire frame in the form of a circle has a wire jumper along the diameter, parallel to the horizontal axis $OO^\prime$, about which the frame can rotate. The mass of a unit length of the frame and the jumper is the same and is equal to $\rho$. The current entering the frame is equal to $I$. The frame is in a magnetic field of induction $B$, directed parallel to the gravitational field. At what angle from the vertical will the frame deviate? | ||
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| + | <figcaption> | ||
| + | For problem $9.1.11$ | ||
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| + | <p> | ||
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| + | |||
| + | <h3>Solution</h3> | ||
| + | <p> | ||
| + | a) Using the expression for the moment of magnetic field obtained in <a href="../9.1.10">9.1.10</a>, $\vec{N} = [\vec{M} \times \vec{B}]$ we obtain | ||
| + | $$ N = BIS\cdot \cos\alpha = \pi R^2BI \cdot \cos\alpha $$ | ||
| + | in this case the moment of gravity: | ||
| + | $$ M_{mg} = Rmg\cdot \cos\alpha = 2\pi R^2\rho g\cdot \sin\alpha $$ | ||
| + | these moments are equal: | ||
| + | $$ 2\pi R^2\rho g \cdot \sin\alpha = \pi BI R^2 \cdot \cos\alpha $$ | ||
| + | after transformations, we obtain | ||
| + | $$ \boxed{\tan\alpha = \frac{BI}{2\rho g}} $$ | ||
| + | b) Find the moment of gravity: | ||
| + | $$ M_{mg} = mgR\cdot \sin\alpha = (2\pi R + 2R)\rho gR \cdot \sin\alpha $$ | ||
| + | |||
| + | $$ M_{mg} = 2R^2\rho g(1+\pi ) \cdot \sin\alpha $$ | ||
| + | Now, we represent the initial circuit as two superimposed circuits with currents $I_1$ and $I_2$ such that $I = I_1 + I_2$, the circuit with $I_2$ is a semicircle with a partition, the circuit with $I_1$ is a ring without a partition, then from the parallel connection it follows that: $I_1\cdot \pi R = I_2 \cdot 2R$ then | ||
| + | $$ I_1 = I_2\cdot \frac{2}{\pi} $$ | ||
| + | |||
| + | $$ I = I_1 + I_2 = I_2\left(1+\frac{2}{\pi}\right) $$ | ||
| + | |||
| + | $$ I_1 = I\cdot \frac{2}{\pi +2}; \quad $$ | ||
| + | Then the moments for these contours are: | ||
| + | $$ M_{k1} = BS_1\cdot \cos\alpha =\pi R^2I\cdot \frac{2}{\pi +2}B\cdot \cos\alpha $$ | ||
| + | |||
| + | $$ M_{k2} = BS_2\cdot \cos\alpha = \frac{1}{2}\pi R^2I\cdot \frac{\pi}{\pi +2}B\cdot \cos\alpha $$ | ||
| + | Total moment of the contours: | ||
| + | $$ M_k = \frac{1}{2}\pi R^2 BI \cdot \cos\alpha\cdot \frac{\pi + 4}{\pi +2} $$ | ||
| + | Let's equate this moment and the moment of gravity: | ||
| + | $$ \frac{1}{2}\pi R^2 BI \cdot \cos\alpha\cdot \frac{\pi + 4}{\pi +2} = 2R^2\rho g(1+\pi ) \cdot \sin\alpha $$ | ||
| + | from here | ||
| + | $$ \boxed{\tan\alpha = \frac{\pi (\pi +4)}{4(\pi +2)(\pi +1)} \cdot \frac{BI}{\rho g}} $$ | ||
| + | |||
| + | </p> | ||
| + | |||
| + | <h4>Answer</h4> | ||
| + | <p> | ||
| + | $$\tan\alpha = \frac{\pi (\pi +4)}{4(\pi +2)(\pi +1)} \cdot \frac{BI}{\rho g}$$ | ||
| + | </p> | ||
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| <title>a) A wire frame in the form of a circle with current can rotate about the horizontal axis OO^\prime. The mass of a unit length of the wire is \rho, the current in the frame is I. The frame is in a magnetic field of induction B, directed along the gravitational field. Determine the angle of deviation of the plane of the circle from the vertical. b) A wire frame in the form of a circle has a wire jumper along the diameter, parallel to the horizontal axis OO^\prime, about which the frame can rotate. The mass of a unit length of the frame and the jumper is the same and is equal to \rho. The current entering the frame is equal to I. The frame is in a magnetic field of induction B, directed parallel to the gravitational field. At what angle from the vertical will the frame deviate?</title> | |||
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| </p> | |||
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| <h3 id="back-link"><a href="../../#9.1">$\leftarrow$Back</a></h3> | |||
| <h3> Statement </h3> | |||
| <p> | |||
| $9.1.11.$ a) A wire frame in the form of a circle with current can rotate about the horizontal axis $OO^\prime$. The mass of a unit length of the wire is $\rho$, the current in the frame is $I$. The frame is in a magnetic field of induction B, directed along the gravitational field. Determine the angle of deviation of the plane of the circle from the vertical. </p><p> | |||
| b) A wire frame in the form of a circle has a wire jumper along the diameter, parallel to the horizontal axis $OO^\prime$, about which the frame can rotate. The mass of a unit length of the frame and the jumper is the same and is equal to $\rho$. The current entering the frame is equal to $I$. The frame is in a magnetic field of induction $B$, directed parallel to the gravitational field. At what angle from the vertical will the frame deviate? | |||
| </p> | |||
| <center> | |||
| <figure> | |||
| <img src="https://savchenkosolutions.com/9/9.1.11/statement.png" | |||
| loading="lazy" width="380" /> | |||
| <figcaption> | |||
| For problem $9.1.11$ | |||
| </figcaption> | |||
| </figure> | |||
| </center> | |||
| <p> | |||
| </p> | |||
| <h3>Solution</h3> | |||
| <p> | |||
| a) Using the expression for the moment of magnetic field obtained in <a href="../9.1.10">9.1.10</a>, $\vec{N} = [\vec{M} \times \vec{B}]$ we obtain | |||
| $$ N = BIS\cdot \cos\alpha = \pi R^2BI \cdot \cos\alpha $$ | |||
| in this case the moment of gravity: | |||
| $$ M_{mg} = Rmg\cdot \cos\alpha = 2\pi R^2\rho g\cdot \sin\alpha $$ | |||
| these moments are equal: | |||
| $$ 2\pi R^2\rho g \cdot \sin\alpha = \pi BI R^2 \cdot \cos\alpha $$ | |||
| after transformations, we obtain | |||
| $$ \boxed{\tan\alpha = \frac{BI}{2\rho g}} $$ | |||
| b) Find the moment of gravity: | |||
| $$ M_{mg} = mgR\cdot \sin\alpha = (2\pi R + 2R)\rho gR \cdot \sin\alpha $$ | |||
| $$ M_{mg} = 2R^2\rho g(1+\pi ) \cdot \sin\alpha $$ | |||
| Now, we represent the initial circuit as two superimposed circuits with currents $I_1$ and $I_2$ such that $I = I_1 + I_2$, the circuit with $I_2$ is a semicircle with a partition, the circuit with $I_1$ is a ring without a partition, then from the parallel connection it follows that: $I_1\cdot \pi R = I_2 \cdot 2R$ then | |||
| $$ I_1 = I_2\cdot \frac{2}{\pi} $$ | |||
| $$ I = I_1 + I_2 = I_2\left(1+\frac{2}{\pi}\right) $$ | |||
| $$ I_1 = I\cdot \frac{2}{\pi +2}; \quad $$ | |||
| Then the moments for these contours are: | |||
| $$ M_{k1} = BS_1\cdot \cos\alpha =\pi R^2I\cdot \frac{2}{\pi +2}B\cdot \cos\alpha $$ | |||
| $$ M_{k2} = BS_2\cdot \cos\alpha = \frac{1}{2}\pi R^2I\cdot \frac{\pi}{\pi +2}B\cdot \cos\alpha $$ | |||
| Total moment of the contours: | |||
| $$ M_k = \frac{1}{2}\pi R^2 BI \cdot \cos\alpha\cdot \frac{\pi + 4}{\pi +2} $$ | |||
| Let's equate this moment and the moment of gravity: | |||
| $$ \frac{1}{2}\pi R^2 BI \cdot \cos\alpha\cdot \frac{\pi + 4}{\pi +2} = 2R^2\rho g(1+\pi ) \cdot \sin\alpha $$ | |||
| from here | |||
| $$ \boxed{\tan\alpha = \frac{\pi (\pi +4)}{4(\pi +2)(\pi +1)} \cdot \frac{BI}{\rho g}} $$ | |||
| </p> | |||
| <h4>Answer</h4> | |||
| <p> | |||
| $$\tan\alpha = \frac{\pi (\pi +4)}{4(\pi +2)(\pi +1)} \cdot \frac{BI}{\rho g}$$ | |||
| </p> | |||
| <p style="text-align: right; font-style: italic; font-size: 14;"> | |||
| Andrei Yersh<br> | |||
| </p> | |||
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| <p> | |||
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| <p> | |||
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