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For the band-pass filter shown in Figure \(30.25,\) how can the width of the frequency response be increased? a) increase \(R_{1}\) b) decrease \(C_{1}\) c) increase \(R_{2}\) d) increase \(C_{2}\) e) do any of the above

Short Answer

Expert verified
Answer: Decrease \(C_{1}\).

Step by step solution

01

Option a) Increase \(R_{1}\)

Increasing \(R_1\) will increase the time constant of the low-pass filter section \(\tau_1 = R_1C\). In the case of a series resonant circuit, \(\tau = RC\). Thus, increasing \(\tau\) will decrease the width of the frequency response. So, this option is incorrect.
02

Option b) Decrease \(C_{1}\)

Decreasing \(C_1\) will decrease the time constant of the low-pass filter section \(\tau_1 = R_1C_1\). In case of a series resonant circuit, \(\tau = RC\). Thus, decreasing \(\tau\) will increase the width of the frequency response. So, this option is correct.
03

Option c) Increase \(R_{2}\)

Increasing \(R_2\) will increase the time constant of the high-pass filter section \(\tau_2 = R_2C_2\). In case of a series resonant circuit, \(\tau = RC\). Thus, increasing \(\tau\) will decrease the width of the frequency response. So, this option is incorrect.
04

Option d) Increase \(C_{2}\)

Increasing \(C_2\) will increase the time constant of the high-pass filter section \(\tau_2 = R_2C_2\). In case of a series resonant circuit, \(\tau = RC\). Thus, increasing \(\tau\) will decrease the width of the frequency response. So, this option is incorrect.
05

Option e) Do any of the above

As we have seen previously, option b) is the correct answer. Option e) implies that all the other options are viable to increase the width of the frequency response, which is not accurate. Therefore, this option is incorrect. To summarize, to increase the width of the frequency response of the band-pass filter, we should decrease \(C_{1}\). The correct answer is option b).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Electrical Resonance
Electrical resonance occurs when a system's inductive reactance and capacitive reactance are equal in magnitude, but opposite in phase, resulting in a net reactive impedance of zero at a particular frequency. This frequency is known as the resonant frequency. In filters, like the band-pass filter mentioned in the exercise, resonance dictates the central frequency where the passband is centered.

In context with the exercise provided, electrical resonance plays a crucial role in determining the operating frequency range of the band-pass filter. Implementing changes in the circuit components can shift the resonance point, affecting the filter's ability to select a narrower or wider band of frequencies.
Time Constant
The time constant, typically denoted as \( \tau \), is a measure of the time it takes for a system to respond to changes. In electrical circuits, the time constant is the product of resistance (R) and capacitance (C), expressed as \( \tau = RC \). It reflects how quickly a capacitor charges to approximately 63% of its maximum charge or discharges to about 37% of its initial charge.

Regarding the band-pass filter from the exercise, by adjusting the time constant you influence the filter's frequency response. Decreasing the capacitance \( C_1 \) for the low-pass portion, as shown in the solution, lowers its time constant, which in turn increases the width of the frequency response, allowing a broader range of frequencies to pass through.
High-Pass Filter
A high-pass filter is designed to allow frequencies above a certain cutoff frequency to pass through while attenuating frequencies below this threshold. The behavior of a high-pass filter is characterized by its time constant \( \tau = R_2C_2 \). This time constant determines how quickly the filter responds to changes in frequency.

In the step-by-step solution to the exercise, increasing the resistance \( R_2 \) is identified as a method that would actually reduce the width of the frequency response, not increase it. This is because a larger time constant results in a slower response of the high-pass section of the band-pass filter, leading to a narrower frequency range being passed.
Low-Pass Filter
A low-pass filter allows frequencies below a certain cutoff frequency to pass through while reducing the amplitude of frequencies above this threshold. Similar to the high-pass filter, its behavior is also defined by a time constant \( \tau = R_1C_1 \) for the low-pass section of the band-pass filter.

In terms of the exercise, reducing the capacitance \( C_1 \) decreases the time constant, which is the correct solution to increase the width of the frequency response. This change allows the low-pass part of the band-pass filter to allow a wider range of frequencies to pass, thereby expanding the bandwidth of the filter.

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Most popular questions from this chapter

An LC circuit consists of a capacitor, \(C=2.50 \mu \mathrm{F},\) and an inductor, \(L=4.00 \mathrm{mH} .\) The capacitor is fully charged using a battery and then connected to the inductor. An oscilloscope is used to measure the frequency of the oscillations in the circuit. Next, the circuit is opened, and a resistor, \(R\), is inserted in series with the inductor and the capacitor. The capacitor is again fully charged using the same battery and then connected to the circuit. The angular frequency of the damped oscillations in the RLC circuit is found to be \(20.0 \%\) less than the angular frequency of the oscillations in the LC circuit. a) Determine the resistance of the resistor. b) How long after the capacitor is reconnected in the circuit will the amplitude of the damped current through the circuit be \(50.0 \%\) of the initial amplitude? c) How many complete damped oscillations will have occurred in that time?

A 75,000 -W light bulb (yes, there are such things!) operates at \(I_{\mathrm{rms}}=200 . \mathrm{A}\) and \(V_{\mathrm{rms}}=440 . \mathrm{V}\) in a \(60.0-\mathrm{Hz} \mathrm{AC}\) circuit. Find the resistance, \(R,\) and self- inductance, \(L,\) of this bulb. Its capacitive reactance is negligible.

A \(4.00-\mathrm{mF}\) capacitor is connected in series with a \(7.00-\mathrm{mH}\) inductor. The peak current in the wires between the capacitor and the inductor is \(3.00 \mathrm{~A}\). a) What is the total electric energy in this circuit? b) Write an expression for the charge on the capacitor as a function of time, assuming the capacitor is fully charged at \(t=0 \mathrm{~s}\).

The discussion of \(\mathrm{RL}, \mathrm{RC},\) and \(\mathrm{RLC}\) circuits in this chapter has assumed a purely resistive resistor, one whose inductance and capacitance are exactly zero. While the capacitance of a resistor can generally be neglected, inductance is an intrinsic part of the resistor. Indeed, one of the most widely used resistors, the wire-wound resistor, is nothing but a solenoid made of highly resistive wire. Suppose a wire-wound resistor of unknown resistance is connected to a DC power supply. At a voltage of \(V=10.0 \mathrm{~V}\) across the resistor, the current through the resistor is \(1.00 \mathrm{~A}\) Next, the same resistor is connected to an AC power source providing \(V_{\mathrm{rms}}=10.0 \mathrm{~V}\) at a variable frequency. When the frequency is \(20.0 \mathrm{kHz}, \mathrm{a}\) current, \(I_{\mathrm{rms}}=0.800 \mathrm{~A},\) is measured through the resistor. a) Calculate the resistance of the resistor. b) Calculate the inductive reactance of the resistor. c) Calculate the inductance of the resistor. d) Calculate the frequency of the AC power source at which the inductive reactance of the resistor exceeds its resistance.

A \(200-\Omega\) resistor, a \(40.0-\mathrm{mH}\) inductor and a \(3.0-\mu \mathrm{F}\) capacitor are connected in series with a source of time-varying emf that provides \(10.0 \mathrm{~V}\) at a frequency of \(1000 \mathrm{~Hz}\). What is the impedance of the circuit? a) \(200 \Omega\) b) \(228 \Omega\) c) \(342 \Omega\) d) \(282 \Omega\)

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