Problem 24
Question
\(\bullet\) In a series \(R-L-C\) circuit, \(R=400 \Omega, L=0.350 \mathrm{H},\) and \(C=0.0120 \mu \mathrm{F}\) (a) What is the resonance angular frequency of the circuit? (b) The capacitor can withstand a peak voltage of 550 \(\mathrm{V}\) . If the voltage source operates at the resonance frequency, what maximum voltage amplitude can it have if the maximum capacitor voltage is not exceeded?
Step-by-Step Solution
Verified Answer
(a) \( \omega_0 \approx 4885.8 \, \text{rad/s} \); (b) Maximum voltage amplitude is approximately 2351.25 V.
1Step 1: Understand the Resonant Frequency Formula
The resonance angular frequency \( \omega_0 \) of a series \( R-L-C \) circuit is given by the formula \[ \omega_0 = \frac{1}{\sqrt{LC}} \]where \( L \) is the inductance and \( C \) is the capacitance. This formula describes the frequency at which the impedance of the circuit is minimized.
2Step 2: Substitute the Values
Substitute the given values \( L = 0.350 \, \text{H} \) and \( C = 0.0120 \, \mu \text{F} = 0.0120 \times 10^{-6} \, \text{F} \) into the formula.\[ \omega_0 = \frac{1}{\sqrt{0.350 \times 0.0120 \times 10^{-6}}} \]
3Step 3: Calculate the Resonant Frequency
Calculate using the substitution from the previous step:\[ \omega_0 = \frac{1}{\sqrt{0.350 \times 0.012 \times 10^{-6}}} = \frac{1}{\sqrt{4.2 \times 10^{-9}}} \]Then simplify to find:\[ \omega_0 \approx \frac{1}{2.049 \times 10^{-4}} \approx 4885.8 \, \text{rad/s} \]
4Step 4: Maximum Voltage Amplitude Calculation
Given that the capacitor can withstand a peak voltage of 550 V and that the circuit is at resonance, the maximum source voltage amplitude \( V_0 \) can be determined by:\[ V_c = \frac{V_0}{Q} = 550 \]where \( Q \) is the quality factor calculated by:\[ Q = \frac{\omega_0 L}{R} \]
5Step 5: Compute the Quality Factor
Substitute the known values into the quality factor equation:\[ Q = \frac{4885.8 \times 0.350}{400} \approx \frac{1710.03}{400} \approx 4.275 \]
6Step 6: Solve for Maximum Voltage Amplitude
Solving the equation from Step 4 using the value of \( Q \),\[ 550 = \frac{V_0}{4.275} \]Solving for \( V_0 \) gives:\[ V_0 = 550 \times 4.275 \approx 2351.25 \, \text{V} \]
Key Concepts
Series RLC CircuitQuality FactorMaximum Voltage AmplitudeCapacitor Voltage
Series RLC Circuit
A series RLC circuit is a type of electrical circuit that combines three fundamental components: a resistor (R), an inductor (L), and a capacitor (C), all connected in a series alignment. This configuration is crucial in the study of resonance in electrical circuits.
Understanding the series RLC circuit is vital because it is the foundation for many applications, including filters and oscillators. In such circuits, the impedance, or total resistance to the flow of current, can be described by the combination of individual impedances offered by the resistor, inductor, and capacitor.
At resonance, the circuit behaves uniquely. The inductive and capacitive reactances cancel each other out, making the impedance minimal. This means the circuit can efficiently transfer energy with minimal resistance from the inductor and capacitor.
Series RLC circuits are valued for their ability to control current flow at certain frequencies, making them indispensable in tuning circuits for radios and other communication devices.
Understanding the series RLC circuit is vital because it is the foundation for many applications, including filters and oscillators. In such circuits, the impedance, or total resistance to the flow of current, can be described by the combination of individual impedances offered by the resistor, inductor, and capacitor.
At resonance, the circuit behaves uniquely. The inductive and capacitive reactances cancel each other out, making the impedance minimal. This means the circuit can efficiently transfer energy with minimal resistance from the inductor and capacitor.
Series RLC circuits are valued for their ability to control current flow at certain frequencies, making them indispensable in tuning circuits for radios and other communication devices.
Quality Factor
The quality factor, often represented by the letter \(Q\), is a dimensionless parameter that describes the sharpness of the resonance of the circuit. It is linked to how efficiently a series RLC circuit can store and transfer energy. Let's dive deeper into this concept.
The quality factor is determined by the ratio of the resonance frequency times the inductance to the resistance, given by the formula:
\[ Q = \frac{\omega_0 L}{R} \]
where:
On the other hand, a low \(Q\) factor indicates wider bandwidth and less resonance sharpness, which can be beneficial in applications requiring the passage of a range of frequencies. Understanding the quality factor helps in designing circuits to meet specific performance criteria.
The quality factor is determined by the ratio of the resonance frequency times the inductance to the resistance, given by the formula:
\[ Q = \frac{\omega_0 L}{R} \]
where:
- \(\omega_0\) is the resonance angular frequency
- \(L\) is the inductance
- \(R\) is the resistance
On the other hand, a low \(Q\) factor indicates wider bandwidth and less resonance sharpness, which can be beneficial in applications requiring the passage of a range of frequencies. Understanding the quality factor helps in designing circuits to meet specific performance criteria.
Maximum Voltage Amplitude
The maximum voltage amplitude for a series RLC circuit is an important concept because it determines the highest voltage that the circuit can handle while still maintaining optimal performance.
In resonance conditions, the voltage across the inductor and capacitor can increase substantially. The relationship between the maximum source voltage amplitude \(V_0\) and the peak voltage \(V_c\) of the capacitor is defined as:
\[ V_c = \frac{V_0}{Q} \]
This formula helps ensure that the source voltage amplitude does not exceed what the capacitor can withstand. Here's why it's essential to manage this:
In resonance conditions, the voltage across the inductor and capacitor can increase substantially. The relationship between the maximum source voltage amplitude \(V_0\) and the peak voltage \(V_c\) of the capacitor is defined as:
\[ V_c = \frac{V_0}{Q} \]
This formula helps ensure that the source voltage amplitude does not exceed what the capacitor can withstand. Here's why it's essential to manage this:
- Preventing over-voltage conditions can help avoid damage to the capacitor, leading to circuit failure.
- Ensuring the maximum voltage amplitude stays within limits keeps the circuit operating effectively and efficiently.
Capacitor Voltage
In a series RLC circuit, the capacitor voltage is significant, especially when running at its resonance frequency. At resonance, the voltages across the inductor and capacitor can be much larger than the source voltage.
This phenomenon occurs due to the low net impedance at resonance, leading to higher currents and subsequently higher voltages across these reactive components. However, it's crucial to ensure that the capacitor's voltage does not exceed its threshold, as this can result in the failure of the capacitor.
To maintain safety and performance, one must calculate and monitor the capacitor voltage using the quality factor and resonance facts:
This phenomenon occurs due to the low net impedance at resonance, leading to higher currents and subsequently higher voltages across these reactive components. However, it's crucial to ensure that the capacitor's voltage does not exceed its threshold, as this can result in the failure of the capacitor.
To maintain safety and performance, one must calculate and monitor the capacitor voltage using the quality factor and resonance facts:
- Understand the relationship: \( V_c = \frac{V_0}{Q} \)
- Assess the component ratings to prevent over-voltage.
- Implement safeguards, such as protective circuits, to maintain voltages within safe levels.
Other exercises in this chapter
Problem 21
\(\bullet\) In an \(R-L-C\) series circuit, \(R=150 \Omega, L=0.750 \mathrm{H},\) and \(C=0.0180 \mu \mathrm{F}\) . The source has voltage amplitude \(V=150 \ma
View solution Problem 23
A series circuit consists of an ac source of variable frequency, a 115\(\Omega\) resistor, a 1.25\(\mu\) capacitor, and a 4.50 \(\mathrm{mH}\) inductor. Find th
View solution Problem 25
\(\bullet\) In a series \(R-L-C\) circuit, \(L=0.200 \mathrm{H}, C=80.0 \mu \mathrm{F},\) and the voltage amplitude of the source is 240 \(\mathrm{V}\) . (a) Wh
View solution Problem 26
\(\bullet\) In an \(R-L-C\) series circuit, \(R=300 \Omega, L=0.400 \mathrm{H},\) and \(C=6.00 \times 10^{-8} \mathrm{F}\) . When the ac source operates at the
View solution