Problem 33
Question
In a series \(R-L-C\) circuit, the components have the following values: \(L=20.0 \mathrm{mH}, C=140 \mathrm{nF},\) and \(R=350 \Omega .\) The generator has an rms voltage of \(120 \mathrm{~V}\) and a frequency of \(1.25 \mathrm{kHz}\). Determine (a) the power supplied by the generator; and (b) the power dissipated in the resistor.
Step-by-Step Solution
Verified Answer
The power supplied by the generator and the power dissipated in the resistor are both approximately 7.35 W.
1Step 1: Calculate Inductive and Capacitive Reactance
First, determine the inductive reactance \(X_L\) and capacitive reactance \(X_C\) using the formulas:\[X_L = 2 \pi f L \quad \text{and} \quad X_C = \frac{1}{2 \pi f C}\]where \(f = 1.25\, \text{kHz}\), \(L = 20.0\, \text{mH}\), and \(C = 140\, \text{nF}\). 1. Calculate \(X_L\):\[X_L = 2 \pi \cdot 1.25 \times 10^3 \cdot 20.0 \times 10^{-3} = 157\, \Omega\]2. Calculate \(X_C\):\[X_C = \frac{1}{2 \pi \cdot 1.25 \times 10^3 \cdot 140 \times 10^{-9}} = 908\, \Omega\]
2Step 2: Calculate the Circuit Impedance
The total impedance \(Z\) of the series \(R-L-C\) circuit is found using:\[Z = \sqrt{R^2 + (X_L - X_C)^2}\]Substitute the values:\[Z = \sqrt{350^2 + (157 - 908)^2}\]\[= \sqrt{350^2 + (-751)^2} \approx 827.07\, \Omega\]
3Step 3: Determine the Current in the Circuit
The rms current \(I_{rms}\) flowing through the circuit is calculated using Ohm’s law:\[I_{rms} = \frac{V_{rms}}{Z}\]with \(V_{rms} = 120\, \text{V}\):\[I_{rms} = \frac{120}{827.07} \approx 0.145\, \text{A}\]
4Step 4: Calculate the Power Supplied by the Generator
The power supplied by the generator is given by:\[P_{gen} = V_{rms} \cdot I_{rms} \cdot \cos \phi\]Where the power factor \(\cos \phi = \frac{R}{Z}\):\[\cos \phi = \frac{350}{827.07} \approx 0.423\]Then the power is:\[P_{gen} = 120 \cdot 0.145 \cdot 0.423 \approx 7.35\, \text{W}\]
5Step 5: Calculate the Power Dissipated in the Resistor
The power dissipated in the resistor is given by:\[P_R = I_{rms}^2 \cdot R\]Substituting the known values:\[P_R = (0.145)^2 \cdot 350 \approx 7.35\, \text{W}\]
6Step 6: Verify Consistency in Power Calculations
Notice that the power supplied by the generator equals the power dissipated in the resistor, confirming our calculations. This is consistent with energy conservation, as the power in a purely resistive circuit is entirely dissipated as heat in the resistor.
Key Concepts
Inductive ReactanceCapacitive ReactanceCircuit ImpedanceOhm’s LawPower Factor
Inductive Reactance
Inductive reactance is a measure of how much an inductor opposes the change of current in an AC circuit.
Inductors store energy in the form of a magnetic field and release it into the circuit, causing a timing delay or phase shift between voltage and current.
In a circuit with AC supply, the inductive reactance is represented by the symbol \(X_L\) and is calculated using the formula: \[ X_L = 2 \pi f L \]Where:
Inductors store energy in the form of a magnetic field and release it into the circuit, causing a timing delay or phase shift between voltage and current.
In a circuit with AC supply, the inductive reactance is represented by the symbol \(X_L\) and is calculated using the formula: \[ X_L = 2 \pi f L \]Where:
- \(f\) is the frequency of the AC source.
- \(L\) is the inductance in henries (H).
Capacitive Reactance
Capacitive reactance, denoted as \(X_C\), is the extent to which a capacitor opposes the change in current in an AC circuit.
Capacitors store energy in an electric field, temporarily holding charge and then releasing it, creating a phase difference where current leads voltage.
To calculate capacitive reactance, use:\[X_C = \frac{1}{2 \pi f C} \]Where:
Capacitors store energy in an electric field, temporarily holding charge and then releasing it, creating a phase difference where current leads voltage.
To calculate capacitive reactance, use:\[X_C = \frac{1}{2 \pi f C} \]Where:
- \(f\) is the frequency of the alternating current.
- \(C\) is the capacitance measured in farads (F).
Circuit Impedance
Circuit impedance is the total opposition a circuit presents to the flow of alternating current.
It combines resistive, inductive, and capacitive effects and is represented by the symbol \(Z\).
In an \(RLC\) circuit, impedance is not just resistance, it also comprises reactance, calculated by:\[ Z = \sqrt{R^2 + (X_L - X_C)^2} \]Where:
It combines resistive, inductive, and capacitive effects and is represented by the symbol \(Z\).
In an \(RLC\) circuit, impedance is not just resistance, it also comprises reactance, calculated by:\[ Z = \sqrt{R^2 + (X_L - X_C)^2} \]Where:
- \(R\) is the resistance in ohms.
- \(X_L\) is the inductive reactance.
- \(X_C\) is the capacitive reactance.
Ohm’s Law
Ohm’s Law is a fundamental principle when analyzing electrical circuits, stating that the current through a conductor between two points is directly proportional to the voltage across the two points.
The formula is expressed as:\[ I = \frac{V}{Z} \]Where:
The formula is expressed as:\[ I = \frac{V}{Z} \]Where:
- \(I\) is the current in amperes (A).
- \(V\) is the voltage in volts (V).
- \(Z\) is the impedance in ohms (\(\Omega\)).
Power Factor
Power factor is a measure of how effectively electrical power is being used in a circuit.
It represents the cosine of the phase difference \(\phi\) between voltage and current in the circuit.
The formula for power factor \(\cos \phi\) is:\[ \cos \phi = \frac{R}{Z} \]Where:
Typically, a circuit operates efficiently when the power factor is as close to 1 as possible, minimizing losses and improving performance. Understanding this concept is vital for optimizing electrical power systems.
It represents the cosine of the phase difference \(\phi\) between voltage and current in the circuit.
The formula for power factor \(\cos \phi\) is:\[ \cos \phi = \frac{R}{Z} \]Where:
- \(R\) is the resistance in the circuit.
- \(Z\) is the total impedance.
Typically, a circuit operates efficiently when the power factor is as close to 1 as possible, minimizing losses and improving performance. Understanding this concept is vital for optimizing electrical power systems.
Other exercises in this chapter
Problem 30
At a frequency \(\omega_{1},\) the reactance of a certain capacitor equals that of a certain inductor. (a) If the frequency is changed to \(\omega_{2}=2 \omega_
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An electrical engineer is designing an \(R-L-C\) circuit for use in a ham radio receiver. He is unsure of the value of the inductance in the circuit, so he meas
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In an \(R-L-C\) series circuit, the magnitude of the phase angle is \(54.0^{\circ},\) with the source voltage lagging the current. The reactance of the capacito
View solution Problem 36
In a series \(R-L-C\) circuit, \(R=300 \Omega, X_{C}=300 \Omega,\) and \(X_{L}=500 \Omega .\) The average power consumed in the resistor is \(60.0 \mathrm{~W}\)
View solution