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en/11.2.3.md
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| + | ### Statement | ||
| + | |||
| + | $11.2.3.$ [Insert the problem statement] | ||
| + | |||
| + | ### Solution | ||
| + | |||
| + | A long solenoid with current produces a magnetic field with the following characteristics: | ||
| + | |||
| + | · Inside, far from the ends, the field is uniform and parallel to the axis (position C). | ||
| + | · Near the ends (positions A and B), the field is non‑uniform: the field lines spread out and there is both a radial and an axial gradient. The intensity decreases as one moves away from the center. | ||
| + | |||
| + | Taking this into account, let us analyze the motion of the ring and the magnetic flux. | ||
| + | |||
| + | The ring moves horizontally, keeping its plane perpendicular to the axis of the solenoid. | ||
| + | |||
| + | · At A and B (ends): when the ring moves, it passes through regions where the field intensity varies with position. Therefore, the magnetic flux through the area of the ring changes with time. | ||
| + | |||
| + | At C (center): the field is uniform. When shifting the ring laterally, the value of$ \mathbf{B}$ at every point on its surface is the same, and the flux then remains constant. | ||
| + | |||
| + | We apply Faraday's Law. | ||
| + | |||
| + | The electromotive force induced in the closed circuit (ring + bridge) is: | ||
| + | |||
| + | $\mathcal{E} = -\frac{d\Phi}{dt}$ | ||
| + | |||
| + | · At A and B | ||
| + | $ d\Phi/dt \neq 0 $ → an emf is induced → current flows through the bulb → it lights up. | ||
| + | · At C | ||
| + | $ d\Phi/dt = 0$ → there is no emf → no current flows → the bulb turns off. | ||
| + | |||
| + | #### Answer | ||
| + | |||
| + | [Insert a concise answer or boxed result] | ||
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| ### Statement | |||
| $11.2.3.$ [Insert the problem statement] | |||
| ### Solution | |||
| A long solenoid with current produces a magnetic field with the following characteristics: | |||
| · Inside, far from the ends, the field is uniform and parallel to the axis (position C). | |||
| · Near the ends (positions A and B), the field is non‑uniform: the field lines spread out and there is both a radial and an axial gradient. The intensity decreases as one moves away from the center. | |||
| Taking this into account, let us analyze the motion of the ring and the magnetic flux. | |||
| The ring moves horizontally, keeping its plane perpendicular to the axis of the solenoid. | |||
| · At A and B (ends): when the ring moves, it passes through regions where the field intensity varies with position. Therefore, the magnetic flux through the area of the ring changes with time. | |||
| At C (center): the field is uniform. When shifting the ring laterally, the value of$ \mathbf{B}$ at every point on its surface is the same, and the flux then remains constant. | |||
| We apply Faraday's Law. | |||
| The electromotive force induced in the closed circuit (ring + bridge) is: | |||
| $\mathcal{E} = -\frac{d\Phi}{dt}$ | |||
| · At A and B | |||
| $ d\Phi/dt \neq 0 $ → an emf is induced → current flows through the bulb → it lights up. | |||
| · At C | |||
| $ d\Phi/dt = 0$ → there is no emf → no current flows → the bulb turns off. | |||
| #### Answer | |||
| [Insert a concise answer or boxed result] | |||