92.1.7 - Current Amplifier and its Input Resistance
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Understanding Feedback Systems
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Let's start our discussion on current amplifiers. What do you think happens when we apply feedback to an amplifier?
I believe it stabilizes the gain.
Correct! Feedback can indeed stabilize and improve performance. We primarily have four configurations of negative feedback systems. Can anyone name one?
Voltage-series feedback!
Great! Voltage-series feedback is where the input port is shunted and the feedback connection is in series. Remember the acronym V - S - F for Voltage-Series Feedback.
What is the significance of feedback on input resistance?
Excellent question! Feedback tends to increase the input resistance, which is crucial for maintaining signal integrity.
How do we express this change mathematically?
We can express the changed input resistance as R_in_f = R_in (1 + βA). Here β is the feedback factor, and A is the amplifier’s gain. Let's remember 'R = RA' to recall this equation.
Ideal vs. Practical Feedback
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In ideal conditions, what can you tell me about input and output resistances?
The input resistance is infinite, and the output resistance is zero, right?
Exactly! However, in practical systems, we often have finite input and output resistances. Why might this matter?
It could affect the voltage gain and signal quality.
Spot on! As we introduce load resistances, they can influence the overall gain. It's important to account for these changes in design.
How do we do that mathematically?
We modify our equations to account for practical resistances, shifting from ideal to real-world applications. This could change our input resistance formula.
Impact of Load Resistance
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Let's consider how load resistance affects our feedback system. Specifically, how does that change the effective gain?
It reduces the gain because some current will flow through the load instead.
Exactly! This reduction leads to a new effective gain, which we can express as A' = A * (1 - RL/R). Remember 'A' for Gain in our formulas.
And for input resistance, how does it change?
In this case, we have R_in_f = R_in(1 + βA'). The gain is modified by the load, which in turn alters our feedback calculations.
Transconductance Amplifiers
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Now moving on to transconductance amplifiers, what key characteristic distinguishes them?
They convert voltage inputs to current outputs!
Correct! And in these systems, feedback can still amplify our input resistance through similar principles we've discussed.
So, how would we express this amplification?
We would still refer to the desensitization factor, modifying our equations to R_in_f = R_in(1 + βG), where G is the transconductance. Keep in mind the difference between voltage and current terms!
Introduction & Overview
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Quick Overview
Standard
The section provides a comprehensive analysis of feedback systems' influence on input and output resistance of amplifiers. It covers both ideal and practical scenarios, emphasizing the relationship between feedback factors and input resistance.
Detailed
Current Amplifier and its Input Resistance
In this section, we delve into the effects of negative feedback on the input and output resistance of current amplifiers. The discussion begins with a foundational understanding of feedback systems, noting four basic configurations. The focus then shifts to defining input resistance in both ideal conditions—where the input resistance is infinite, and output resistance is zero—and realistic scenarios where these factors are finite.
To illustrate, we consider the feedback loop where an input signal is applied to the amplifier and explore how this affects voltage and current within the system. Various equations describe how input resistance changes with feedback, highlighting the significance of the desensitization factor, which amplifies input resistance based on the feedback gain. The section also explores scenarios involving finite loads and finite input resistance, examining how they impact the output voltage and the effective gain.
Practical applications are discussed, including the transconductance amplifier where the current signal relationship is established and linked to input resistance. As the narrative progresses, we analyze the impact of loading effects and derive expressions for input resistance based on varying configurations, ultimately emphasizing the critical role of feedback in optimizing amplifier performance.
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Feedback System Overview
Chapter 1 of 5
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Chapter Content
So, dear students, welcome back after the break ... we have to consider load of the circuit it is ∞.
Detailed Explanation
This chunk sets the stage for discussing the feedback system's impact on input and output resistance. It introduces the feedback network configurations: shunt-series (voltage series feedback), and emphasizes the importance of considering ideal situations (infinite input resistance and zero output resistance) when starting the analysis.
Examples & Analogies
Think of a feedback system like a thermostat in your home. It has an ideal scenario of being perfectly sensitive to temperature changes (infinite effectiveness), which allows for the best control over your heating or cooling. If conditions were not ideal, like a broken sensor, the performance would worsen (finite effectiveness).
Calculating Input Resistance
Chapter 2 of 5
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Chapter Content
Now, to get this derivation of this input resistance ... and using this relationship we can see that this is R (1 + βA).
Detailed Explanation
This section describes how to derive the input resistance of the feedback system. By stimulating the input with a signal and observing the resulting current, we can establish a relationship between voltage and current. The formula for the changed input resistance takes into account the forward amplifier's input resistance and gain.
Examples & Analogies
Consider a car's fuel efficiency when the tires are inflated to the optimal level (ideal conditions). If you then load extra passengers and cargo, the car's efficiency decreases but remains proportional to how much extra weight you add. The relationship between the weight and efficiency mirrors the calculation of the input resistance and feedback effects.
Practical Load Effects on Input Resistance
Chapter 3 of 5
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So, if we put say R here and then the voltage here v ... we can say that this new expression of the input resistance where A′ it is defined here.
Detailed Explanation
In a practical scenario, we introduce a finite load resistance that affects the voltage available at the port. This effect alters the input resistance and requires using a load-affected gain (A′) in calculations. It shows how real-world conditions necessitate adjustments to theoretical models.
Examples & Analogies
Imagine you're trying to pour juice into a glass. If you add ice cubes, the juice splashes and spills due to the added volume from the ice (load). Similarly, when the load increases in a circuit, it affects the input resistance, necessitating adjustment to account for the changes.
Feedback Network with Finite Resistance
Chapter 4 of 5
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Chapter Content
On the other hand, if I say that i current is flowing and it is entering to the circuit ... but we are keeping in the feedback network ports are I should say ideal namely the input resistance here it is 0.
Detailed Explanation
This chunk extends the concept to situations where the ideal characteristics of the feedback network are changed by introducing finite resistances. It describes how the output resistance impacts how the feedback system behaves, stressing that both input and feedback network characteristics must be practical.
Examples & Analogies
Think of trying to fill a balloon with air. If the balloon has no holes (ideal), it fills quickly. If there are small holes (finite resistance), it takes longer to fill and some air escapes. This highlights how imperfections can affect the efficiency of the feedback system.
Desensitization Factor in the Feedback System
Chapter 5 of 5
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Chapter Content
What we have seen that the series connection ... it is independent of this port situation.
Detailed Explanation
This section discusses the concept of the desensitization factor which describes how the series connection in a feedback system can lead to increased input resistance. It emphasizes that these properties hold regardless of the specific configuration at the input port.
Examples & Analogies
Imagine a rubber band that, when stretched (series connection), becomes harder to stretch even further. Similarly, the input resistance in a feedback system increases due to the desensitization factor when feedback is applied.
Key Concepts
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Feedback Systems: Configurations that alter amplifier characteristics.
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Input Resistance: Affects signal integrity and overall amplifier gain.
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Output Resistance: Influences how the amplifier interacts with loads.
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Desensitization Factor: Amplifies input resistance through feedback mechanisms.
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Transconductance: Converts voltage to current in amplifiers.
Examples & Applications
If an ideal feedback configuration is employed, the input resistance becomes infinite, ensuring that signals can flow without loss.
In practical applications, if a load resistance of 100 ohms is connected, the input resistance could modify based on its interaction with the amplifier's intrinsic resistances.
Memory Aids
Interactive tools to help you remember key concepts
Rhymes
Gain is in the desensitization, helps resistance in amplification!
Stories
Imagine a gardener (feedback) watering plant (amplifier) to ensure it grows tall (increases stability).
Memory Tools
Remember V - S - F for Voltage-Series Feedback to recall configuration types.
Acronyms
R = RA
Recall the relationship of input resistance in feedback amplifiers.
Flash Cards
Glossary
- Input Resistance
The resistance seen by a signal source at the input of an amplifier.
- Output Resistance
The resistance seen by the load connected to the output of an amplifier.
- Desensitization Factor
The factor that amplifies input resistance due to feedback in the input circuit.
- Transconductance Amplifier
An amplifier that converts voltage signals to proportional output currents.
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