1. Loop moving into a Constant Magnetic Field. Consider a square loop with side length 1m moving at a rate 0.1 m/s in the +x-direction into a magnetic field 6m long with constant strength and direction of B = 1 T 2 (into the page). a. Sketch a diagram of the magnetic flux vs. time with t=0 when the right edge of the square loop just starts to enter the magnetic field. b. Sketch a diagram of the induced electromotive force.

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### Loop Moving into a Constant Magnetic Field

Consider a square loop with a side length of 1 m moving at a rate of 0.1 m/s in the +x direction into a magnetic field 6 m long with constant strength and direction of B = 1 T \( \hat{z} \) (into the page).

**a. Magnetic Flux vs. Time Diagram**

Sketch a diagram of the magnetic flux vs. time with \( t = 0 \) when the right edge of the square loop just starts to enter the magnetic field.

- **Description**:
  - The magnetic flux (Φ) through the loop will change as the loop moves into the magnetic field.
  - When \( t = 0 \), the right edge of the loop just starts to enter the magnetic field.
  - As the loop continues to move into the field, the area inside the loop that is exposed to the magnetic field increases, causing the magnetic flux to increase.
  - When the entire loop is within the magnetic field, the magnetic flux reaches a maximum value.
  - Once the loop starts to exit the magnetic field, the magnetic flux begins to decrease.
  - The graph should show a linear increase in flux as the loop enters the field, a constant maximum flux when the loop is fully in the field, and a linear decrease as the loop exits the field.

- **Graph Details**:
  - **X-axis**: Time (t) in seconds.
  - **Y-axis**: Magnetic Flux (Φ) in Weber (Wb).

**b. Induced Electromotive Force (emf) Diagram**

Sketch a diagram of the induced electromotive force (emf).

- **Description**:
  - The induced emf in the loop is related to the rate of change of magnetic flux through Faraday's Law of Induction: \( \mathcal{E} = -\frac{dΦ}{dt} \).
  - When the loop first enters the magnetic field, the rate of change of flux is positive, inducing a positive emf.
  - When the loop is fully within the magnetic field, the flux is constant, and thus the induced emf is zero.
  - As the loop exits the magnetic field, the rate of change of flux is negative, inducing a negative emf.
  - The graph should show a positive peak when entering, zero when the entire loop is within the field, and a negative peak when exiting.

- **
Transcribed Image Text:### Loop Moving into a Constant Magnetic Field Consider a square loop with a side length of 1 m moving at a rate of 0.1 m/s in the +x direction into a magnetic field 6 m long with constant strength and direction of B = 1 T \( \hat{z} \) (into the page). **a. Magnetic Flux vs. Time Diagram** Sketch a diagram of the magnetic flux vs. time with \( t = 0 \) when the right edge of the square loop just starts to enter the magnetic field. - **Description**: - The magnetic flux (Φ) through the loop will change as the loop moves into the magnetic field. - When \( t = 0 \), the right edge of the loop just starts to enter the magnetic field. - As the loop continues to move into the field, the area inside the loop that is exposed to the magnetic field increases, causing the magnetic flux to increase. - When the entire loop is within the magnetic field, the magnetic flux reaches a maximum value. - Once the loop starts to exit the magnetic field, the magnetic flux begins to decrease. - The graph should show a linear increase in flux as the loop enters the field, a constant maximum flux when the loop is fully in the field, and a linear decrease as the loop exits the field. - **Graph Details**: - **X-axis**: Time (t) in seconds. - **Y-axis**: Magnetic Flux (Φ) in Weber (Wb). **b. Induced Electromotive Force (emf) Diagram** Sketch a diagram of the induced electromotive force (emf). - **Description**: - The induced emf in the loop is related to the rate of change of magnetic flux through Faraday's Law of Induction: \( \mathcal{E} = -\frac{dΦ}{dt} \). - When the loop first enters the magnetic field, the rate of change of flux is positive, inducing a positive emf. - When the loop is fully within the magnetic field, the flux is constant, and thus the induced emf is zero. - As the loop exits the magnetic field, the rate of change of flux is negative, inducing a negative emf. - The graph should show a positive peak when entering, zero when the entire loop is within the field, and a negative peak when exiting. - **
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