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9.1 A simplified diagram of an electric generator is shown below - NSC Physical Sciences - Question 9 - 2019 - Paper 1

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9.1 A simplified diagram of an electric generator is shown below. When the coil is rotated with a constant speed, an emf is induced in the coil. 9.1.1 Is this an AC... show full transcript

Worked Solution & Example Answer:9.1 A simplified diagram of an electric generator is shown below - NSC Physical Sciences - Question 9 - 2019 - Paper 1

Step 1

9.1.1 Is this an AC generator or a DC generator?

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Answer

This is an AC generator. An AC generator produces alternating current (AC) by inducing an electromotive force (emf) in the coil as it rotates within a magnetic field.

Step 2

9.1.2 Briefly explain how an emf is generated in the coil when the coil is rotated by referring to the principle of electromagnetic induction.

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Electromagnetic induction occurs when a conductor, such as a coil of wire, moves through a magnetic field or when the magnetic field around a conductor changes. According to Faraday's law of electromagnetic induction, the induced emf in the coil is directly proportional to the rate of change of the magnetic flux through the coil. When the coil rotates in the magnetic field, the angle between the magnetic field lines and the normal to the coil changes, leading to a change in magnetic flux and thereby inducing an emf.

Step 3

9.1.3 Draw a sketch graph of the output voltage versus time for this generator. Show ONE complete cycle.

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The output voltage graph for an AC generator is sinusoidal in shape. It typically varies between a positive peak and a negative peak over time. It can be represented as follows:

Voltage
  |
  |     /\         /\
  |    /  \       /  \
  |   /    \     /    \
  |  /      \   /      \
  |_/        \_/        \_
  ----------------------------------
                    Time

One complete cycle corresponds to one full rotation of the coil.

Step 4

9.2.1 Define the term rms voltage of an AC source.

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The rms (root mean square) voltage of an AC source is defined as the effective voltage which dissipates the same amount of energy in a resistive load as an equivalent DC voltage. Mathematically, it is expressed as: Vrms=Vmax2V_{rms} = \frac{V_{max}}{\sqrt{2}} where VmaxV_{max} is the peak voltage of the AC source.

Step 5

9.2.2 Calculate the maximum (peak) voltage of the AC source.

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To find the maximum peak voltage VmaxV_{max} of the AC source, we first calculate the rms voltage:

Given that the energy dissipated in 10 s is 500 J in a 200 Ω resistor:

Using the formula for power: P=WtP = \frac{W}{t} P=500J10s=50WP = \frac{500 \, J}{10 \, s} = 50 \, W

Next, using the formula for power in terms of rms voltage: P=Vrms2RP = \frac{V_{rms}^2}{R}

Substituting R=200ΩR = 200 \Omega: 50=Vrms220050 = \frac{V_{rms}^2}{200}

This gives us: Vrms2=50×200=10000V2V_{rms}^2 = 50 \times 200 = 10000 \, V^2 Vrms=100VV_{rms} = 100 \, V

Finally, we can determine the peak voltage: Vmax=Vrms×2=100×2141.42VV_{max} = V_{rms} \times \sqrt{2} = 100 \times \sqrt{2} \approx 141.42 \, V

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