16. The 12.0 cm long rod in Figure 23.11 (a) moves at 4.00 m/s. What is the strength of the magnetic field if a 95.0 V emf is induced? ΔΑ-Δx B At (a)

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**Problem Statement:**
The 12.0 cm long rod in Figure 23.11 (a) moves at 4.00 m/s. What is the strength of the magnetic field if a 95.0 V emf is induced?

**Diagrams Explanation:**

**Figure 23.11 (a):**
- A rectangular loop is shown with a rod moving perpendicularly along the top of the loop. 
- The loop is situated within a uniform magnetic field (indicated by 'x'), pointing into the page.
- The motion of the rod is represented by the velocity \( v \), moving towards the right. 
- The area of the loop changes as \( \Delta A = l \times \Delta x \).
- The rod moves by a distance \( \Delta x \) in a time interval \( \Delta t \).

**Figure 23.11 (b):**
- Shows two views explaining the application of Lenz's Law and the use of Right-Hand Rule (RHR).
- The top part of the diagram uses RHR-2 to indicate the direction of the induced current within the loop due to the moving rod.
- Beneath the loop, an equivalent circuit is depicted with a resistor \( R \) and an electromotive force \( \mathcal{E} \).
- The magnetic flux \( \Phi \) is shown to be increasing.

**Important Concepts Illustrated:**
- Right-Hand Rule (RHR) is used to determine the direction of the magnetic force and induced current.
- Lenz’s Law is applied to determine the direction of the induced current as one that opposes the change in magnetic flux.
- The induced emf (\( \mathcal{E} \)) is related to the rate of change of the magnetic flux, demonstrating Faraday's law of electromagnetic induction.

This set-up helps in understanding the principles behind electromagnetic induction and the factors affecting the magnitude of induced emf in a closed circuit.
Transcribed Image Text:**Problem Statement:** The 12.0 cm long rod in Figure 23.11 (a) moves at 4.00 m/s. What is the strength of the magnetic field if a 95.0 V emf is induced? **Diagrams Explanation:** **Figure 23.11 (a):** - A rectangular loop is shown with a rod moving perpendicularly along the top of the loop. - The loop is situated within a uniform magnetic field (indicated by 'x'), pointing into the page. - The motion of the rod is represented by the velocity \( v \), moving towards the right. - The area of the loop changes as \( \Delta A = l \times \Delta x \). - The rod moves by a distance \( \Delta x \) in a time interval \( \Delta t \). **Figure 23.11 (b):** - Shows two views explaining the application of Lenz's Law and the use of Right-Hand Rule (RHR). - The top part of the diagram uses RHR-2 to indicate the direction of the induced current within the loop due to the moving rod. - Beneath the loop, an equivalent circuit is depicted with a resistor \( R \) and an electromotive force \( \mathcal{E} \). - The magnetic flux \( \Phi \) is shown to be increasing. **Important Concepts Illustrated:** - Right-Hand Rule (RHR) is used to determine the direction of the magnetic force and induced current. - Lenz’s Law is applied to determine the direction of the induced current as one that opposes the change in magnetic flux. - The induced emf (\( \mathcal{E} \)) is related to the rate of change of the magnetic flux, demonstrating Faraday's law of electromagnetic induction. This set-up helps in understanding the principles behind electromagnetic induction and the factors affecting the magnitude of induced emf in a closed circuit.
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