Frequency Response of CE/CS Amplifiers Considering High Frequency Models of BJT and MOSFET (Part B) - 41.1.5 | 41. Frequency Response of CE/CS Amplifiers Considering High Frequency Models of BJT and MOSFET (Part B) | Analog Electronic Circuits - Vol 2
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Interactive Audio Lesson

Listen to a student-teacher conversation explaining the topic in a relatable way.

Generalized Model of CE/CS Amplifiers

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0:00
Teacher
Teacher

Today, we'll start by examining the generalized model of CE and CS amplifiers. Can anyone name the key components in our model?

Student 1
Student 1

I believe we have input and output resistors, coupling capacitors, and a voltage dependent voltage source.

Teacher
Teacher

Exactly! The input resistance is represented by R1, and our source resistance is Rs. We also have capacitors C3 and C4 which play crucial roles. Remember, you can think of the coupling capacitors as allowing the AC signals to pass while blocking DC. This leads us to our next point: calculating equivalent capacitances.

Student 3
Student 3

How do we calculate those equivalent capacitive values?

Teacher
Teacher

Great question! The input capacitance, Cin, can be expressed in terms of C3 and C4, factoring in the gain A. We can write this as Cin = C3(1 - A). Remember this relation; it will help with circuit analysis!

Transfer Function and Frequency Response

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Teacher
Teacher

Now let’s derive the transfer function for our amplifier. Why do you think it’s important to obtain this function?

Student 2
Student 2

I think it helps us understand how the amplifier behaves at different frequencies.

Teacher
Teacher

Exactly! By considering the impedance across various components, we can determine how voltage gains change with frequency. Can anyone point out what might happen in the high-frequency range?

Student 4
Student 4

I assume the gain will decrease due to capacitance effects, right?

Teacher
Teacher

Correct! This drop in gain indicates the amplifier’s bandwidth limit. Remember, knowing the locations of poles and zeros within the transfer function informs about stability too.

Mid-Frequency Gain and Its Significance

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Teacher
Teacher

Now let's focus on mid-frequency gain. Can anyone summarize what we mean by mid-frequency?

Student 1
Student 1

Mid-frequency refers to where the frequency terms dominate, and we do not see much attenuation?

Teacher
Teacher

Exactly right! In this range, the gain stabilizes and we see a consistent attenuation of approximately -20 dB per decade. Keep in mind the role of resistors and how they interact with capacitors.

Student 3
Student 3

Are we able to calculate this mid-frequency gain?

Teacher
Teacher

Yes, indeed! The mid-frequency gain can be deduced directly from the ratio of input to output resistance.

Overall Frequency Response and Poles

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Teacher
Teacher

Finally, let's discuss how to analyze overall frequency response. What factors should we consider?

Student 2
Student 2

We need to look at the poles from our individual sections and how they interact.

Teacher
Teacher

Correct! The location of each pole dictates cutoff frequencies. For instance, if we find one pole appears before another, it can become our lower cutoff frequency.

Student 4
Student 4

So, we can find the upper cutoff as well?

Teacher
Teacher

Yes! By determining the minimum value between different pole frequencies, we can chart out our effective bandwidth.

Introduction & Overview

Read a summary of the section's main ideas. Choose from Basic, Medium, or Detailed.

Quick Overview

This section discusses the frequency response characteristics of Common Emitter (CE) and Common Source (CS) amplifiers using high-frequency models of BJTs and MOSFETs.

Standard

The section delves into the generalized models of CE and CS amplifiers, emphasizing the analysis of frequency response by incorporating relevant capacitive effects and resistances. It explains how different parameters affect the gain and the role of coupling capacitors in defining the frequency response.

Detailed

Frequency Response of CE/CS Amplifiers

In this section, we explore the frequency response of Common Emitter (CE) and Common Source (CS) amplifiers while considering the high-frequency models of BJTs and MOSFETs. The main points of focus include:

  • Generalized Model: We begin with a complete circuit model comprising input resistor (R1), source resistance (Rs), coupling capacitors (C3, C4), and output resistance (R2).
  • Capacitance Calculations: The equivalent input and output capacitances are discussed, where the input capacitance (Cin) and output capacitance (Cout) are derived from the coupling capacitors. The relationship between these capacitances and the voltage gain (A) is critical in analyzing frequency response.
  • Frequency Response Characteristics: By employing Laplace transforms, the transfer function is obtained for analyzing how the amplifier responds across a range of frequencies. Key features include the poles and zeroes associated with the frequency response, introducing terms like dominant pole approximation and the implications for stability and bandwidth.
  • Mid-Frequency Analysis: The mid-frequency region behavior of the amplifier and its gain characteristics are elaborated, highlighting the significance of reactive components like capacitors on the frequency response.

This compact yet comprehensive examination facilitates a deeper understanding of how amplifier design and component selection influence overall circuit performance in both low and high-frequency domains.

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Analog Electronic Circuits _ by Prof. Shanthi Pavan
Analog Electronic Circuits _ by Prof. Shanthi Pavan

Audio Book

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Generalized Model of CE/CS Amplifiers

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Yeah. So, welcome after the break. So, we are talking about the, in fact, what we got it is the generalized model of CE and CS amplifier here. What it is having here it is the input signal source, having the source resistance of R, and then signal coupling capacitor C, and then if I consider this is the main amplifier where we do have the input resistance represented by this R. And then we do have voltage dependent voltage source, which means that this is the core of the amplifier, then we do have the output resistance R. And then C and C, they are representing you know either C, C or C and C based on whether the circuit it is CE amplifier or CS amplifier.

Detailed Explanation

Here, we are introduced to the generalized model of CE (Common Emitter) and CS (Common Source) amplifiers. The model includes essential components such as the input signal source, source resistance, coupling capacitors, input resistance, output resistance, and voltage-dependent voltage sources. These variables are crucial for understanding how the amplifier operates under different conditions. The presence of capacitors C and C showcases the adaptability of the model for both transistor types (BJT and MOSFET), effectively demonstrating how the design can change based on specific circuit requirements.

Examples & Analogies

Think of the analog amplifier as a water distribution system. The input signal source is like a water main, source resistance acts like a narrowing pipe that limits flow, while the coupling capacitors ensure water only flows when the pressure (voltage) is appropriate. Just as different pipes can carry water differently based on their diameter and material, different transistor types influence the performance of the amplifier.

Capacitance Contributions

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So, this particular this capacitor it can be converted into two equivalent capacitance; one is for the input port, the other one is for the output port. And then, the input port part coming out of the C it is what we said is that C (1 β€’ A ) or in this case A is equal to A. In fact, if you see here we are putting a β€’ sign here assuming that the polarity of the voltage dependent voltage source, here it is +ve.

Detailed Explanation

In this section, we discuss the role of capacitors in the circuit. They're transformed into equivalent capacitances for both the input and output ports. This is vital for analyzing how signals pass through the amplifier. The term C(1 - A) highlights that the input capacitance is affected by the gain of the amplifier (A). The negative sign indicates an inverted relationship based on the voltage source polarity, which is an essential concept in understanding signal processing within amplifiers.

Examples & Analogies

Imagine a dam that holds water (signal) and releases it downstream. The capacitors serve as adjustable gates in this dam. The input capacitance changes based on the amount of water being let through (gain). If more water is released too quickly (high gain), it may affect the pressure in the remaining pipes, akin to how signal inversion impacts the amplifier's performance.

Effective Load Capacitance

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So, in summary what we have it is at this node we do have the C and then at this node we do have the net C. Now, to get the frequency response of this circuit namely starting from this point till the primary output what we have it is we do have one network here and then we do have of course, the main amplifier starting from this point to this point and then of course, at this point we do have the C.

Detailed Explanation

Here, the focus is on understanding the total effective load capacitance at a specific node in the circuit. This capacitance affects the circuit's frequency response, as capacitive loads impact how quickly the circuit can respond to changes in input signals. By establishing connections between network nodes and the main amplifier, the analysis of how the complete system behaves at different frequencies can begin.

Examples & Analogies

Consider a car hitting a speed bump (the load capacitance) on a road. The car’s ability to respond (frequency response) varies based on how heavy the load is (capacitance) and how many speed bumps (nodes) it encounters along the way. A lighter load or fewer bumps means a quicker response time.

Analyzing Frequency Response

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So, our first task is to find the frequency response from this point to this point, namely maybe in Laplace domain we can see, and then we can find what is the corresponding transfer function we are getting.

Detailed Explanation

The analysis begins with determining the frequency response, which indicates how the circuit behaves at different frequencies. Utilizing the Laplace domain allows for easier manipulation of the differential equations that represent the circuit. The objective is to derive the transfer function, a mathematical representation that describes the output signal in relation to the input signal, vital for predicting circuit performance.

Examples & Analogies

Imagine tuning a radio to different frequencies to find your favorite station. Each frequency you tune is similar to the analysis of the circuit's response. The transfer function acts like the clarity of the signal at each frequency; it tells you how well the circuit (radio) can amplify and transmit the signal (music) you want.

Transfer Function Development

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Now, if you see here to get the frequency response of this circuit namely in Laplace domain, we can get the transfer function by considering this impedance which is R β«½ and then R in series with + R β«½.

Detailed Explanation

This step involves deriving the transfer function by evaluating the impedance of the circuit. By calculating the total impedance from resistances in series and parallel, we can identify how the circuit responds to a sinusoidal input. This step is crucial for analyzing stability and gain at various frequencies.

Examples & Analogies

Think of a water park slide (impedance). When you add more slide sections (resistances), the overall speed (response) changes. Calculating total slide length (impedance) at different angles (input frequencies) determines how quickly someone can reach the bottom of the slide (circuit output).

Definitions & Key Concepts

Learn essential terms and foundational ideas that form the basis of the topic.

Key Concepts

  • Generalized Model: The complete representation of CE/CS amplifiers, including resistance and capacitance impacts.

  • Frequency Response: How amplifiers react over different frequencies, especially in identifying gain behavior at pole and zero locations.

Examples & Real-Life Applications

See how the concepts apply in real-world scenarios to understand their practical implications.

Examples

  • An example of a BJT amplifier's frequency response showcasing gain reduction at higher frequencies.

  • A case study on a MOSFET amplifier analyzing the impact of capacitance on overall circuit performance.

Memory Aids

Use mnemonics, acronyms, or visual cues to help remember key information more easily.

🎡 Rhymes Time

  • In frequency response, poles are key, where gain drops low but feels like free.

πŸ“– Fascinating Stories

  • Imagine a race where the signal must pass through a series of hurdles (capacitors) that only allow the right ones to pass - just like how coupling capacitors allow AC but block DC signals on their way through.

🧠 Other Memory Gems

  • P.A.C.E. - Poles And Capacitance Effects summarize how these parameters affect amplifier response.

🎯 Super Acronyms

G.A.I.N. - Gain, Amplifiers, Input Network can help remember what we look for in our designs.

Flash Cards

Review key concepts with flashcards.

Glossary of Terms

Review the Definitions for terms.

  • Term: CE Amplifier

    Definition:

    Common Emitter Amplifier, a type of amplifier configuration that provides high voltage gain.

  • Term: CS Amplifier

    Definition:

    Common Source Amplifier, primarily used in MOSFET devices, known for its similar high voltage gain characteristics.

  • Term: Frequency Response

    Definition:

    The output spectrum of an amplifier in response to an input signal across given frequencies.

  • Term: Poles and Zeros

    Definition:

    Poles are the frequencies at which the gain of the system approaches zero, whereas zeros are frequencies where gain becomes infinite.