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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

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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.png

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 XCX_C) 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 au is the time constant, ff is the frequency, and CC is the capacitance in farads.

Step 2

2.1.2 Inductive reactance

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Inductive reactance (denoted by XLX_L) 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=2imesauimesfimesLX_L = 2 imes au imes f imes L

where LL is the inductance in henries.

Step 3

2.2.1 Inductive reactance

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Answer

To calculate the inductive reactance:

Using the formula:

XL=2imesauimesfimesLX_L = 2 imes au imes f imes L Substituting the given values:

XL=2imes3.14159imes60imes0.044=16.59extΩX_L = 2 imes 3.14159 imes 60 imes 0.044 = 16.59 ext{ Ω}

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:

X_C = rac{1}{2 imes 3.14159 imes 60 imes 120 imes 10^{-6}} = 22.11 ext{ Ω}

Step 5

2.2.3 Impedance of the circuit

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To find the impedance of the circuit, use the formula:

ewline \\ \\ \\ \\ \\\ \\\ \\ \\ \\ Z = ewline \\ \\ R + j(X_L - X_C)$$ Calculating: $$Z = ewline \\ \\ \\ \\ \\ = ewline \\ \\\ \\ \\ \\Z = ewline \\ \\ \\ = ewline \\25 ext{Ω}^2 + (22.11 - 16.59) ^ 2$$ Evaluating: $$Z = 25.6 Ω$$

Step 6

2.3.1 the current through the capacitor.

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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 (ILI_L) through the inductor can be found by:

IL=ItICI_L = I_t - I_C Given It=6AI_t = 6 A:

IL=63.67=2.33AI_L = 6 - 3.67 = 2.33 A

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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Answer

At resonance in an RLC circuit, the capacitive reactance (XCX_C) equals the inductive reactance (XLX_L). Therefore, this state results in:\n XC=XLX_C = X_L

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.

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