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Across a 100 V, 50 Hz supply, a coil with a resistance of 10 and an inductance of 210 mH is connected in series with a variable capacitor. Calculate:

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6 parts
1.1

58.42 Hz58.42 \, \text{Hz}

1.2

15 Ω15 \, \Omega

3.1

48.24 μF48.24 \, \mu\text{F}

3.2

48.24 μF48.24 \, \mu\text{F}

3.3

667.2 V667.2 \, \text{V}

659.7 V659.7 \, \text{V}

3.4
6.60

Step-by-step solution

12 steps

Here are the solutions to the questions from the image.

Part 1

Series RLC Circuit

Given:
Capacitance C=58 μF=58×10−6 FC = 58 \, \mu\text{F} = 58 \times 10^{-6} \, \text{F}
Resistance R=15 ΩR = 15 \, \Omega
Inductance L=128 mH=128×10−3 HL = 128 \, \text{mH} = 128 \times 10^{-3} \, \text{H}
Supply voltage V=100 VV = 100 \, \text{V} (RMS, assumed)

Part 1.1

58.42 Hz58.42 \, \text{Hz}

Calculate the resonant frequency.

  1. Use the formula for resonant frequency in a series RLC circuit.

    The resonant frequency f0f_0 is given by:

    f0=12πLCf_0 = \frac{1}{2\pi\sqrt{LC}}
  2. Substitute the given values and calculate f0f_0.

    f0=12π(128×10−3 H)(58×10−6 F)f_0 = \frac{1}{2\pi\sqrt{(128 \times 10^{-3} \, \text{H})(58 \times 10^{-6} \, \text{F})}} f0=12π7.424×10−6f_0 = \frac{1}{2\pi\sqrt{7.424 \times 10^{-6}}} f0=12π×2.7247×10−3f_0 = \frac{1}{2\pi \times 2.7247 \times 10^{-3}} f0=10.017119f_0 = \frac{1}{0.017119} f0≈58.42 Hzf_0 \approx \boxed{58.42 \, \text{Hz}}

Part 1.2

15 Ω15 \, \Omega

By means of calculations, show that the impedance is equal to the resistance of the coil.

  1. Calculate the inductive reactance (XLX_L) and capacitive reactance (XCX_C) at the resonant frequency f0f_0.

    XL=2πf0LX_L = 2\pi f_0 L XL=2π(58.42 Hz)(128×10−3 H)X_L = 2\pi (58.42 \, \text{Hz})(128 \times 10^{-3} \, \text{H}) XL≈47.05 ΩX_L \approx 47.05 \, \Omega XC=12πf0CX_C = \frac{1}{2\pi f_0 C} XC=12π(58.42 Hz)(58×10−6 F)X_C = \frac{1}{2\pi (58.42 \, \text{Hz})(58 \times 10^{-6} \, \text{F})} XC≈10.02133X_C \approx \frac{1}{0.02133} XC≈46.88 ΩX_C \approx 46.88 \, \Omega

    (Note: The slight difference between XLX_L and XCX_C is due to rounding f0f_0. If f0f_0 is used with full precision, they would be equal.)

  2. Calculate the total impedance ZZ of the series RLC circuit.

    Z=R2+(XL−XC)2Z = \sqrt{R^2 + (X_L - X_C)^2}

    Using the calculated values:

    Z=(15 Ω)2+(47.05 Ω−46.88 Ω)2Z = \sqrt{(15 \, \Omega)^2 + (47.05 \, \Omega - 46.88 \, \Omega)^2} Z=225+(0.17)2Z = \sqrt{225 + (0.17)^2} Z=225+0.0289Z = \sqrt{225 + 0.0289} Z=225.0289Z = \sqrt{225.0289} Z≈15.00096 ΩZ \approx 15.00096 \, \Omega

    Since R=15 ΩR = 15 \, \Omega, the impedance ZZ is approximately equal to the resistance RR at resonance.

    Z≈15 ΩZ \approx \boxed{15 \, \Omega}

    This shows that Z≈RZ \approx R at resonance.

Part 1.3

Draw the phasor diagram.

(Since I cannot draw an image, I will describe the key features of the phasor diagram at resonance).

  • The current phasor (II) is typically drawn along the positive x-axis (reference).
  • The voltage across the resistor (VR=IRV_R = IR) is in phase with the current, so VRV_R is also along the positive x-axis.
  • The voltage across the inductor (VL=IXLV_L = IX_L) leads the current by 90∘90^\circ, so VLV_L points along the positive y-axis.
  • The voltage across the capacitor (VC=IXCV_C = IX_C) lags the current by 90∘90^\circ, so VCV_C points along the negative y-axis.
  • At resonance, VLV_L and VCV_C are equal in magnitude and opposite in direction, so they cancel each other out.
  • The total supply voltage (VV) is equal to VRV_R and is in phase with the current. The diagram would show II and VRV_R on the positive x-axis, VLV_L on the positive y-axis, and VCV_C on the negative y-axis, with VLV_L and VCV_C having equal lengths. The resultant voltage VV would coincide with VRV_R.

Part 2

Parallel RLC Circuit (Implied)

Given:
Coil resistance R=15 ΩR = 15 \, \Omega
Coil inductance L=200 mH=200×10−3 HL = 200 \, \text{mH} = 200 \times 10^{-3} \, \text{H}

Part 2.1

Determine the frequency at which the resulting current is in phase with the source voltage.

Assumption: This question implies a parallel resonant circuit where the coil (R and L in series) is connected in parallel with a capacitor. However, the value of the capacitor is not provided in the question. Without the capacitor value, it is not possible to calculate a specific non-zero resonant frequency.
If the circuit consists only of the coil (R and L in series) connected to the source, the current will always lag the voltage at any non-zero frequency. The current would only be in phase with the voltage if the circuit were purely resistive, which means the inductance LL would have to be zero or the frequency would have to be zero (DC).

Therefore, based on the information given, this question cannot be solved for a non-zero frequency.
Missing information: Value of the parallel capacitor.

Part 2.2

Calculate the related Q factor value.

The Q factor (Quality factor) for a parallel resonant circuit where the coil (R and L in series) is in parallel with a capacitor is given by:

Q=ω0LRQ = \frac{\omega_0 L}{R}

or

Q=1ω0CRQ = \frac{1}{\omega_0 C R}

Since the resonant frequency ω0\omega_0 (or f0f_0) cannot be determined without the capacitor value (as explained in 2.1), the Q factor also cannot be calculated.
Missing information: Value of the parallel capacitor (and thus resonant frequency).

Part 3

Series RLC Circuit with Variable Capacitor

Given:
Supply voltage V=100 VV = 100 \, \text{V} (RMS, assumed)
Supply frequency f=50 Hzf = 50 \, \text{Hz}
Coil resistance R=10 ΩR = 10 \, \Omega
Coil inductance L=210 mH=210×10−3 HL = 210 \, \text{mH} = 210 \times 10^{-3} \, \text{H}
A variable capacitor is connected in series.

Part 3.1

48.24 μF48.24 \, \mu\text{F}

Capacitance required to produce resonance.

  1. Use the formula for resonant frequency in a series RLC circuit.

    At resonance, f0=f=50 Hzf_0 = f = 50 \, \text{Hz}.

    f0=12πLCf_0 = \frac{1}{2\pi\sqrt{LC}}
  2. Rearrange the formula to solve for CC.

    2πf0=1LC2\pi f_0 = \frac{1}{\sqrt{LC}} (2πf0)2=1LC(2\pi f_0)^2 = \frac{1}{LC} C=1L(2πf0)2C = \frac{1}{L(2\pi f_0)^2}
  3. Substitute the given values and calculate CC.

    C=1(210×10−3 H)(2π×50 Hz)2C = \frac{1}{(210 \times 10^{-3} \, \text{H})(2\pi \times 50 \, \text{Hz})^2} C=1(0.210)(314.159)2C = \frac{1}{(0.210)(314.159)^2} C=1(0.210)(98696.04)C = \frac{1}{(0.210)(98696.04)} C=120726.168C = \frac{1}{20726.168} C≈4.824×10−5 FC \approx 4.824 \times 10^{-5} \, \text{F} C≈48.24 μFC \approx \boxed{48.24 \, \mu\text{F}}

Part 3.2

48.24 μF48.24 \, \mu\text{F}

Value of the capacitor.

This is the same as Question 3.1.
The value of the capacitor is 48.24 μF\boxed{48.24 \, \mu\text{F}}.

Part 3.3

667.2 V667.2 \, \text{V}

Voltage drop across the coil and capacitor.

  1. Calculate the inductive reactance (XLX_L) and capacitive reactance (XCX_C) at resonance.

    At resonance, XL=XCX_L = X_C.

    XL=2πfLX_L = 2\pi f L XL=2π(50 Hz)(210×10−3 H)X_L = 2\pi (50 \, \text{Hz})(210 \times 10^{-3} \, \text{H}) XL=2π(50)(0.210)X_L = 2\pi (50)(0.210) XL=65.97 ΩX_L = 65.97 \, \Omega

    So, XC=65.97 ΩX_C = 65.97 \, \Omega.

  2. Calculate the total current (II) in the series circuit at resonance.

    At resonance, the impedance Z=RZ = R.

    I=VZ=VRI = \frac{V}{Z} = \frac{V}{R} I=100 V10 ΩI = \frac{100 \, \text{V}}{10 \, \Omega} I=10 AI = 10 \, \text{A}
  3. Calculate the voltage drop across the coil (VcoilV_{coil}) and the capacitor (VCV_C).

    The coil has resistance RR and inductance LL. The voltage drop across the coil is Vcoil=I⋅ZcoilV_{coil} = I \cdot Z_{coil}, where Zcoil=R2+XL2Z_{coil} = \sqrt{R^2 + X_L^2}.

    Zcoil=(10 Ω)2+(65.97 Ω)2Z_{coil} = \sqrt{(10 \, \Omega)^2 + (65.97 \, \Omega)^2} Zcoil=100+4351.94Z_{coil} = \sqrt{100 + 4351.94} Zcoil=4451.94Z_{coil} = \sqrt{4451.94} Zcoil≈66.72 ΩZ_{coil} \approx 66.72 \, \Omega Vcoil=I⋅Zcoil=(10 A)(66.72 Ω)V_{coil} = I \cdot Z_{coil} = (10 \, \text{A})(66.72 \, \Omega) Vcoil=667.2 VV_{coil} = \boxed{667.2 \, \text{V}}

    The voltage drop across the capacitor is VC=I⋅XCV_C = I \cdot X_C.

    VC=(10 A)(65.97 Ω)V_C = (10 \, \text{A})(65.97 \, \Omega) VC=659.7 VV_C = \boxed{659.7 \, \text{V}}

Part 3.46.60

Quality factor.

  1. Use the formula for the Q factor of a series RLC circuit.

    Q=XLRQ = \frac{X_L}{R}

    or

    Q=1RLCQ = \frac{1}{R}\sqrt{\frac{L}{C}}
  2. Substitute the values for XLX_L and RR.

    Q=65.97 Ω10 ΩQ = \frac{65.97 \, \Omega}{10 \, \Omega} Q=6.60Q = \boxed{6.60}
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