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A rectangular, a square , a circular and...

A rectangular, a square , a circular and an elliptical loop, all in the `(x-y)` plane, are moving out of a uniform magnetic field with a constant velocity `vec(v)=vhati` . The magnetic field is directed along the negative `z`-axis direction. The induced emf, during the passage of these loops , out of the field region, will not remain constant for :

A

the rectangular, circular and elliptical loops

B

the circular and the elliptical loops

C

only the elliptical loop

D

any of the four loops

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To solve the problem, we need to analyze the induced electromotive force (emf) in the different shapes of loops as they move out of a uniform magnetic field. The key point here is to understand how the area of the loops that is within the magnetic field changes over time. ### Step-by-Step Solution: 1. **Understand the Setup**: - We have four types of loops: rectangular, square, circular, and elliptical. - All loops are in the (x-y) plane and moving out of a uniform magnetic field directed along the negative z-axis with a constant velocity \( \vec{v} = v \hat{i} \). 2. **Induced EMF Formula**: - The induced emf (\( \mathcal{E} \)) in a loop moving out of a magnetic field can be calculated using Faraday's law of electromagnetic induction: \[ \mathcal{E} = -\frac{d\Phi_B}{dt} \] - Where \( \Phi_B \) is the magnetic flux through the loop, given by: \[ \Phi_B = B \cdot A \] - Here, \( B \) is the magnetic field strength and \( A \) is the area of the loop within the magnetic field. 3. **Analyze Each Loop**: - **Rectangular Loop**: - As it moves out of the magnetic field, the area \( A \) that is within the field decreases uniformly. Therefore, \( \frac{dA}{dt} \) is constant, leading to a constant induced emf. - **Square Loop**: - Similar to the rectangular loop, the area decreases uniformly as it exits the magnetic field. Thus, \( \mathcal{E} \) remains constant. - **Circular Loop**: - As the circular loop exits the magnetic field, the area that is within the field changes in a non-linear manner. The rate of change of area \( \frac{dA}{dt} \) is not constant throughout the motion, leading to a variable induced emf. - **Elliptical Loop**: - The situation is similar to the circular loop. The area changes non-linearly as it exits the magnetic field, resulting in a variable induced emf. 4. **Conclusion**: - The induced emf will not remain constant for the circular and elliptical loops due to the non-linear change in area as they exit the magnetic field. In contrast, the rectangular and square loops have a constant rate of change of area and thus a constant induced emf. ### Final Answer: The induced emf will not remain constant for the **circular and elliptical loops**. ---

To solve the problem, we need to analyze the induced electromotive force (emf) in the different shapes of loops as they move out of a uniform magnetic field. The key point here is to understand how the area of the loops that is within the magnetic field changes over time. ### Step-by-Step Solution: 1. **Understand the Setup**: - We have four types of loops: rectangular, square, circular, and elliptical. - All loops are in the (x-y) plane and moving out of a uniform magnetic field directed along the negative z-axis with a constant velocity \( \vec{v} = v \hat{i} \). ...
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