Explain the term inductance with reference to RLC circuits connected to an AC supply - NSC Electrical Technology Power Systems - Question 3 - 2022 - Paper 1
Question 3
Explain the term inductance with reference to RLC circuits connected to an AC supply.
Inductance is the created back-emf in an inductor that tends to oppose a chang... show full transcript
Worked Solution & Example Answer:Explain the term inductance with reference to RLC circuits connected to an AC supply - NSC Electrical Technology Power Systems - Question 3 - 2022 - Paper 1
Step 1
3.2 Draw the phasor diagrams for FIGURES 3.2.1 and 3.2.2 in the ANSWER BOOK.
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Answer
The phasor diagrams for the voltage and current waveforms can be illustrated as follows:
Phasor Diagram for Figure 3.2.1:
The voltage waveform (V) is represented on the vertical axis.
The current waveform (I) lags behind the voltage waveform
Phasor Diagram for Figure 3.2.2:
The voltage across the capacitor (Vc) leads the current waveform (I) by 90 degrees.
Both waveforms are plotted in a sinusoidal manner.
Step 2
3.3.1 Calculate the impedance of the circuit.
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Answer
To calculate the impedance (Z) of the circuit, we use the formula:
Z=R2+(XL−XC)2
Substituting the given values:
R=25Ω
XC=13Ω
XL=94Ω
Z=252+(94−13)2=252+812≈84.77Ω
Step 3
3.3.2 Calculate the phase angle of the circuit.
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Answer
The phase angle (θ) can be calculated using the formula:
θ=tan−1(RXL−XC)
Substituting the given values:
θ=tan−1(2594−13)=tan−1(2581)≈72.85∘
Step 4
3.3.3 Calculate the value of the inductor.
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The value of the inductor (L) can be calculated with the formula:
L=2πfXL
Substituting the values:
XL=94Ω
f=60Hz
L=2×π×6094≈0.25H=250mH
Step 5
3.3.4 Explain what is meant by a lagging power factor.
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Answer
A lagging power factor occurs when the current lags behind the voltage in an RLC circuit. This is typically due to the inductive nature of the circuit, where the inductive load causes the current to delay relative to the applied voltage.
Step 6
3.3.5 Explain why the current and the voltage waveforms are in phase in a series RLC resonance circuit.
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At resonance, the inductive reactance (XL) and capacitive reactance (XC) cancel each other out. This results in the circuit becoming purely resistive, causing the current and voltage waveforms to be in phase with each other.
Step 7
3.4.1 Calculate the total current.
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Answer
To calculate the total current (IT) in the circuit, use the formula:
IT=IR2+(IL−IC)2
Substituting the values:
IR=11A
IC=7A
IL=9A
IT=112+(9−7)2=112+22≈11.18A
Step 8
3.4.2 Calculate the power factor.
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The power factor (cosϕ) can be calculated using:
cosϕ=ITIR
Substituting:
cosϕ=11.1811≈0.98
Step 9
3.4.3 Calculate the total power.
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The total power (P) can be calculated with:
P=VT×IT×cosϕ
Substituting:
P=110×11.18×0.98≈1205.20W
Step 10
3.4.4 State, with a reason, whether the circuit has a leading or lagging power factor.
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The circuit has a lagging power factor because the inductive current is greater than the capacitive current, indicating that the current lags the voltage.
Step 11
3.5.1 Name the circuit that produces the response at A and B in FIGURE 3.5.
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A parallel RLC circuit produces the response at points A and B in Figure 3.5.
Step 12
3.5.2 Discuss the difference between the impedance and current.
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The impedance (Z) represents the total opposition to the flow of alternating current in a circuit, while the current (I) is the actual flow of electric charge. Impedance, being a complex quantity, considers both resistance and reactance.
Step 13
3.5.3 Describe what happens to impedance when the frequency increases in FIGURE 3.5 A.
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As the frequency increases, the impedance decreases in Figure 3.5 A. This is because the inductive reactance increases with frequency, while the capacitive reactance decreases, thus affecting the total impedance of the circuit.