3.1 Explain the term reactance with reference to an alternating current circuit - NSC Electrical Technology Electronics - Question 3 - 2024 - Paper 1
Question 3
3.1 Explain the term reactance with reference to an alternating current circuit.
3.2 FIGURE 3.2 below shows the circuit diagram, waveforms and a partial phasor diag... show full transcript
Worked Solution & Example Answer:3.1 Explain the term reactance with reference to an alternating current circuit - NSC Electrical Technology Electronics - Question 3 - 2024 - Paper 1
Step 1
3.1 Explain the term reactance with reference to an alternating current circuit.
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Answer
Reactance is defined as the opposition offered to the flow of alternating current in an AC circuit by an inductor or capacitor. It represents the phase difference between voltage and current, when they are not in phase.
Step 2
3.2.1 State whether the circuit is predominantly inductive or capacitive. Motivate your answer.
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Answer
The circuit is predominantly capacitive because the voltage across the capacitor (Vc = 15 V) is greater than the voltage across the inductor (Vl = 10 V). This indicates that the reactive component is larger and leads to a capacitive behavior.
Step 3
3.2.2 Calculate the supply voltage.
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Answer
The supply voltage can be calculated using the formula:
VT=sqrtVR2+(VC−VL)2
Substituting in the values:
VT=sqrt182+(15−10)2=sqrt324+25=sqrt349≈18.68V
Step 4
3.2.3 Calculate the phase angle.
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The phase angle can be calculated using:
θ=cos−1(VTVR)
By substituting the values:
θ=cos−1(18.6818)≈15.51∘
Step 5
3.2.4 Redraw and complete the phasor diagram in the ANSWER BOOK.
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Answer
A phasor diagram should be drawn showing:
V_R along the horizontal axis.
V_C leading V_R, indicating a capacitive circuit.
V_T as the resultant vector drawn from the origin.
Step 6
3.2.5 Explain why it could be assumed that the supply current is leading the supply voltage.
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In a capacitive circuit, the supply current (I_R) is always in phase with the voltage across the resistance (V_R), while the supply voltage (V_T) lags behind. Thus, it is safe to assume that I_R leads V_T due to the inherent nature of capacitive reactance.
Step 7
3.3.1 Calculate the current flow through the inductor.
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The current through the inductor (I_L) can be calculated using:
IL=XLVT
Substituting the given values:
IL=62.83230≈3.66A
Step 8
3.3.2 Total current flow.
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The total current flow (I_T) can be calculated by:
IT=IR2+(IL−IC)2
Substituting the values:
IT=1.152+(3.66−1.59)2≈2.37A
Step 9
3.3.3 Power factor.
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The power factor (pf) can be calculated using:
cos(ϕ)=ITIR
Substituting the values:
cos(ϕ)=2.371.15≈0.49
Step 10
3.3.4 Value of capacitance that would cause resonance when the frequency and inductor remain constant.
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At resonance, the inductive reactance equals the capacitive reactance (X_L = X_C). Using:
XC=2πfC1
Rearranged to find C:
C=2πfXC1
Where:
XL=62.83Ω
f=50Hz
Substituting the values:
C=2π(50)(62.83)1≈50.66μF
Step 11
3.4.1 State how a decrease in resistance affects the Q-factor of the circuit.
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A decrease in resistance increases the Q-factor of the circuit, which indicates improved selectivity and greater energy stored relative to energy dissipated.
Step 12
3.4.2 Calculate the Q factor when R = 50 Ω.
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The Q factor (Q) is calculated as:
Q=RXL=502000=40
Step 13
3.4.3 Calculate the resonant frequency when f1 = 200 Hz and f2 = 2100 Hz.
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The resonant frequency occurs at the point where the inductive and capacitive reactances are equal. However, specific calculations would depend on additional provided formulas or values.