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A square coil of wire is rotating at a constant angular speed about a horizontal axis - AQA - A-Level Physics - Question 5 - 2019 - Paper 2

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A square coil of wire is rotating at a constant angular speed about a horizontal axis. Figure 4 shows the coil at one instant when the normal to the plane of the coi... show full transcript

Worked Solution & Example Answer:A square coil of wire is rotating at a constant angular speed about a horizontal axis - AQA - A-Level Physics - Question 5 - 2019 - Paper 2

Step 1

Calculate the number of turns in the coil.

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Answer

To find the number of turns, use the formula for magnetic flux linkage:

Φ=NABcos(θ)\Phi = N A B \cos(\theta)

Where:

  • N\,N is the number of turns,
  • A\,A is the area of the coil (5.0×104 m25.0 \times 10^{-4} \ m²),
  • B\,B is the magnetic flux density (2.5×102T2.5 \times 10^{2} \, T),
  • θ\,\theta is the angle (30°).

First, calculate the maximum flux linkage: Φmax=AimesB\Phi_{max} = A imes B Φmax=(5.0×104 m2)×(2.5×102T)=1.25×101 Wb\Phi_{max} = (5.0 \times 10^{-4} \ m²) \times (2.5 \times 10^{2} \, T) = 1.25 \times 10^{-1} \ Wb

Using the maximum flux linkage: 1.5×103 Wb=N×1.25×101 Wb1.5 \times 10^{3} \ Wb = N \times 1.25 \times 10^{-1} \ Wb

This gives: N=1.5×103 Wb1.25×101 Wb=120 turnsN = \frac{1.5 \times 10^{3} \ Wb}{1.25 \times 10^{-1} \ Wb} = 120 \ turns.

Step 2

Calculate the flux linkage of the coil at the instant shown in Figure 4.

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Answer

Using the previously mentioned formula for flux linkage:

Φ=NABcos(30)\Phi = N A B \cos(30^{\circ})

Substituting the known values:

  • N=120 turns\,N = 120 \ turns,
  • A=5.0×104 m2\,A = 5.0 \times 10^{-4} \ m²,
  • B=2.5×102T\,B = 2.5 \times 10^{2} \, T,
  • cos(30)=32\,\cos(30^{\circ}) = \frac{\sqrt{3}}{2}.

This results in: Φ=120×(5.0×104)×(2.5×102)×32=1.3×103 Wb turns.\Phi = 120 \times (5.0 \times 10^{-4}) \times (2.5 \times 10^{2}) \times \frac{\sqrt{3}}{2} = 1.3 \times 10^{3} \ Wb \ turns.

Step 3

Calculate the peak value of the emf generated.

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Answer

The peak emf (E) generated can be found using Faraday's law: E=NABωsin(θ)E = N A B \omega \sin(\theta)

Where:

  • ω\,\omega is the angular velocity (in radians per second). Assuming an angular speed of 1 Hz (for this calculation): ω=2π×1rad/s\omega = 2\pi \times 1 \, rad/s

Substituting known values: E=120×(5.0×104 m2)×(2.5×102T)×(2π)=0.15 V.E = 120 \times (5.0 \times 10^{-4} \ m²) \times (2.5 \times 10^{2} \, T) \times (2\pi) = 0.15 \ V.

Step 4

Sketch on Figure 6 the variation with time of flux linkage for the same time interval as Figure 5.

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Answer

The graph of flux linkage will mirror the emf graph shown in Figure 5, exhibiting a sinusoidal variation. The flux linkage will oscillate between positive and negative peaks, similarly shaped as the emf curve. A solid or dashed line may be used to outline the curve, depicting a sinusoidal wave pattern within the time frame represented.

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