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Question 1.1: RLC Circuit Calculations

Physics

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Question 1.1: RLC Circuit Calculations

Given:

  • Resistance, R=13 ΩR = 13 \, \Omega
  • Inductive Reactance, XL=47.13 ΩX_L = 47.13 \, \Omega (given in Ω\Omega, so it's reactance)
  • Capacitance, C=100 μF=100×10−6 FC = 100 \, \mu F = 100 \times 10^{-6} \, F
  • Supply Voltage, Vsupply=100 VV_{supply} = 100 \, V
  • Frequency, f=50 Hzf = 50 \, Hz

Step 1: Calculate Capacitive Reactance (XCX_C)

XC=12πfCX_C = \frac{1}{2 \pi f C} XC=12π(50 Hz)(100×10−6 F)X_C = \frac{1}{2 \pi (50 \, \text{Hz}) (100 \times 10^{-6} \, \text{F})} XC=10.0314159X_C = \frac{1}{0.0314159} XC≈31.83 ΩX_C \approx 31.83 \, \Omega

Step 2: Calculate Total Impedance (ZZ)

Z=R2+(XL−XC)2Z = \sqrt{R^2 + (X_L - X_C)^2} Z=(13 Ω)2+(47.13 Ω−31.83 Ω)2Z = \sqrt{(13 \, \Omega)^2 + (47.13 \, \Omega - 31.83 \, \Omega)^2} Z=169 Ω2+(15.3 Ω)2Z = \sqrt{169 \, \Omega^2 + (15.3 \, \Omega)^2} Z=169 Ω2+234.09 Ω2Z = \sqrt{169 \, \Omega^2 + 234.09 \, \Omega^2} Z=403.09 Ω2Z = \sqrt{403.09 \, \Omega^2} Z≈20.08 ΩZ \approx 20.08 \, \Omega

1.1.1 Draw the circuit diagram.
A series RLC circuit consists of a resistor, an inductor, and a capacitor connected in series to an AC voltage source.

      R           L           C
---[ R ]---[ L ]---[ C ]---
    |                   |
    +---( ~ )-----------+
        AC Source

1.1.2 Calculate the total current flowing in the circuit.

I=VsupplyZI = \frac{V_{supply}}{Z} I=100 V20.08 ΩI = \frac{100 \, \text{V}}{20.08 \, \Omega} I≈4.98 AI \approx 4.98 \, \text{A}

The total current flowing in the circuit is 4.98 A\boxed{\text{4.98 A}}.

1.1.3 Calculate the voltage drop across the resistor.

VR=I⋅RV_R = I \cdot R VR=(4.98 A)⋅(13 Ω)V_R = (4.98 \, \text{A}) \cdot (13 \, \Omega) VR≈64.74 VV_R \approx 64.74 \, \text{V}

The voltage drop across the resistor is 64.74 V\boxed{\text{64.74 V}}.

1.1.4 Calculate the voltage drop across the inductor.

VL=I⋅XLV_L = I \cdot X_L VL=(4.98 A)⋅(47.13 Ω)V_L = (4.98 \, \text{A}) \cdot (47.13 \, \Omega) VL≈234.71 VV_L \approx 234.71 \, \text{V}

The voltage drop across the inductor is 234.71 V\boxed{\text{234.71 V}}.

1.1.5 Calculate the voltage drop across the capacitor.

VC=I⋅XCV_C = I \cdot X_C VC=(4.98 A)⋅(31.83 Ω)V_C = (4.98 \, \text{A}) \cdot (31.83 \, \Omega) VC≈158.52 VV_C \approx 158.52 \, \text{V}

The voltage drop across the capacitor is 158.52 V\boxed{\text{158.52 V}}.

1.1.6 Calculate the phase angle.

ϕ=arctan⁡(XL−XCR)\phi = \arctan\left(\frac{X_L - X_C}{R}\right) ϕ=arctan⁡(47.13 Ω−31.83 Ω13 Ω)\phi = \arctan\left(\frac{47.13 \, \Omega - 31.83 \, \Omega}{13 \, \Omega}\right) ϕ=arctan⁡(15.3 Ω13 Ω)\phi = \arctan\left(\frac{15.3 \, \Omega}{13 \, \Omega}\right) ϕ=arctan⁡(1.1769)\phi = \arctan(1.1769) ϕ≈49.64∘\phi \approx 49.64^\circ

The phase angle is 49.64∘\boxed{\text{49.64}^\circ}.

1.1.7 Draw the phase diagram of the above circuit.
The phase diagram (phasor diagram) shows the voltage phasors relative to the current. Since XL>XCX_L > X_C, the circuit is inductive, and the total voltage leads the current.

  • VRV_R is in phase with the current II.
  • VLV_L leads the current II by 90∘90^\circ.
  • VCV_C lags the current II by 90∘90^\circ.
  • VsupplyV_{supply} is the vector sum of VRV_R and (VL−VC)(V_L - V_C).
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