2.1 Define the following terms:
2.1.1 Capacitive reactance
2.1.2 Inductive reactance
2.2 FIGURE 2.2 below represents an RLC series circuit that consists of a 25 Ω resistor, a 44 mH inductor and a 120 μF capacitor, all connected across a 120 V/60 Hz supply - NSC Electrical Technology Power Systems - Question 2 - 2019 - Paper 1
Question 2
2.1 Define the following terms:
2.1.1 Capacitive reactance
2.1.2 Inductive reactance
2.2 FIGURE 2.2 below represents an RLC series circuit that consists of a 25 Ω... show full transcript
Worked Solution & Example Answer:2.1 Define the following terms:
2.1.1 Capacitive reactance
2.1.2 Inductive reactance
2.2 FIGURE 2.2 below represents an RLC series circuit that consists of a 25 Ω resistor, a 44 mH inductor and a 120 μF capacitor, all connected across a 120 V/60 Hz supply - NSC Electrical Technology Power Systems - Question 2 - 2019 - Paper 1
Step 1
2.1.1 Capacitive reactance
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Capacitive reactance (denoted by XC) is defined as the opposition to alternating current by the reactive component of a capacitor in an AC circuit. It can be mathematically expressed as:
X_C = rac{1}{2 imes au imes f imes C}
where au is the time constant, f is the frequency, and C is the capacitance in farads.
Step 2
2.1.2 Inductive reactance
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Inductive reactance (denoted by XL) is the opposition to alternating current by the reactive component of an inductor in an AC circuit. It can be expressed with the following formula:
XL=2imesauimesfimesL
where L is the inductance in henries.
Step 3
2.2.1 Inductive reactance
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To calculate the inductive reactance:
Using the formula:
XL=2imesauimesfimesL
Substituting the given values:
XL=2imes3.14159imes60imes0.044=16.59extΩ
Step 4
2.2.2 Capacitive reactance
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To calculate the capacitive reactance:
Using the formula:
X_C = rac{1}{2 imes au imes f imes C}
Substituting the given values:
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To find the current through the capacitor, use:
I_C = rac{V_s}{X_C}
Substituting:
I_C = rac{220}{60} = 3.67 A
Step 7
2.3.2 Calculate the reactive current.
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The reactive current (IL) through the inductor can be found by:
IL=It−IC
Given It=6A:
IL=6−3.67=2.33A
Step 8
2.3.3 State, with a reason, whether the phase angle is leading or lagging.
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In an RLC circuit, if the capacitive current is higher than the inductive current, the voltage across the capacitor leads the current; thus, the phase angle is leading. Conversely, if the inductive current dominates, the phase angle lags.
Step 9
2.4.1 State the value of the capacitive reactance at resonance.
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At resonance in an RLC circuit, the capacitive reactance (XC) equals the inductive reactance (XL). Therefore, this state results in:\n
XC=XL
Step 10
2.4.2 Calculate the value of the capacitor at resonance.
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Using the formula at resonance:
f = rac{1}{2 au ext{C}}
Rearranging gives:
C = rac{1}{2 imes au imes f} = rac{1}{2 imes 3.14159 imes 1000} = 159.15 ext{ μF}
Step 11
2.4.3 Explain how the value of the current can be affected by the voltage across the inductor being greater than the supply voltage.
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In a series RLC circuit, the voltage across the inductor can be greater than the supply voltage due to resonance effects. When this occurs, it can lead to increased current through the circuit as the total impedance decreases, causing a rise in voltage across the inductor as compared to the supply voltage.