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Today, we're going to discuss the common collector stage. Can anyone tell me what the primary function of a CC stage is?
Isn't it to provide a high input impedance?
Exactly! The CC stage, often called an emitter follower, indeed provides high input impedance. This feature is crucial so that it can couple effectively with the next stage.
How does it help with biasing the next stage?
Great question! The emitter current of the CC stage can provide biasing for the base of the CE stage. This mutual support simplifies the biasing arrangements.
So, does that mean we can omit some components in the circuit design?
Exactly! By utilizing this configuration, we can simplify the biasing because the stages support each other.
In summary, the CC stage aids in biasing and reduces complexity in CE amplifiers.
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Let's dive deeper into biasing. How does the base terminal of the CE amplifier get its bias from the CC stage?
Is it based on the emitter current from the CC transistor?
Yes, the emitter current from the CC transistor directly affects the base of the CE transistor, thus establishing the bias directly.
Can you explain why this configuration is efficient?
Certainly! It ensures that the necessary DC voltage at the base of the CE stage is maintained, while also improving gain characteristics.
In summary, biasing between CC and CE stages simplifies design and enhances performance.
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Now, let's look at the input resistance. What do you think happens when we connect a CC stage before a CE stage?
I think the input resistance increases, right?
Absolutely! The CC stage enhances the input resistance, making the overall amplifier more effective for high source resistance applications.
What about input capacitance? How does that change?
Excellent point! The addition of a CC stage helps reduce the input capacitance by providing an effective AC ground, which is beneficial in many amplifier applications.
To summarize, utilizing a CC stage increases input resistance and lowers input capacitance, improving circuit performance.
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Let's compare this configuration with the Darlington pair. What are the main similarities and differences?
Both use multiple transistors, right?
Correct! However, the Darlington pair connects transistors in a different way, affecting characteristics such as input capacitance.
So, the Darlington pair has higher input capacitance compared to CC-CE?
Yes, exactly! Due to the Miller effect, the input capacitance increases significantly in the Darlington configuration.
In summary, while both configurations serve similar purposes, their input characteristics differ significantly.
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Let's wrap up by discussing some application areas for the CC followed by CE amplifier configuration. Where do you think itβs commonly used?
In audio amplifiers?
Absolutely! This configuration is popular in audio applications where high fidelity and impedance matching is crucial.
What about in RF applications?
Great point! CC-CE amplifiers are also effective in radio frequency applications, benefiting from their high input resistance.
To summarize, CC-CE configurations find applications in audio amplifiers and RF circuits, leveraging their performance benefits.
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The section explores how a common collector amplifier can effectively bias a common emitter amplifier, explaining the mutual benefits between the two stages, including the enhancement of input resistance and a decrease in input capacitance. Additionally, it covers numerical examples illustrating these concepts.
In this section, we explore how a common collector (CC) stage is configured to couple with a common emitter (CE) amplifier. The CC stage, due to its high input impedance and ability to sink current, aids in the biasing of the CE amplifier. The working assumptions include mutual biasing where the emitter current from the CC stage helps in biasing the base of the CE stage, simplifying biasing arrangements. A numerical example illustrates the significance of biasing with calculated current values that are requisite for operation. Moreover, we delve into the advantages of this configuration, such as increased input resistance and reduced input capacitance, making it beneficial for applications requiring high source resistance.
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So, now, we do have another example, where we do have the CC followed by CE amplifier. And what we have here it is, the CC stage it is directly getting coupled to CE stage. And you can see here the in the CC stage, basically this part is the CC stage and normally we do have a current sink here for proper biasing; but here we assume that whatever the emitter current we do have out of Q1 that is entirely getting consumed to the base or base terminal of Q2.
This chunk introduces the concept of using a Common Collector (CC) amplifier followed by a Common Emitter (CE) amplifier. In this configuration, the CC stage is directly connected to the CE stage. Typically, a current sink is used for good biasing in circuits. However, in this setup, it's assumed that the current from the emitter of Q1 (the CC stage) flows completely into the base of Q2 (the CE stage), meaning that the extra biasing circuit isn't necessary.
Think of the CC amplifier as a helpful friend who supplies energy (current) directly to another friend (the CE amplifier) who needs it to perform a task. Instead of both needing to have their own power sources to function successfully, they support each other so that only one power source is needed effectively.
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Now again here we assume that DC voltage of Q2, it is sufficient to feed the signal at the base of Q1; or you may say that, whatever the emitter current we do have out of Q1 that is good enough to make a bias of the Q2. So, in summary what will I like to say that, Q2 is biased by the base terminal of Q1. So, it is biased at its emitter by the base terminal of Q2. On the other hand Q2 is biased at its base terminal by emitter current of Q1.
In this part, itβs explained how the biasing works between the two stages. Q2's base is supplied with enough DC voltage from Q1's emitter current to operate correctly. Thus, Q1 helps to set the biasing for Q2 through its base terminal. This mutual biasing simplifies the circuit design, as the two transistors assist each other in maintaining their operating points.
Imagine a team of two people working together; one person's input (Q1's emitter current) supports and guides the other's task (Q2's operation). They rely on each otherβs strengths to get the job done, resembling a close teamwork setup.
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Now, here for comparison with our previous circuits, we are setting the value of this R1 such that the current flowing through this Q2 we are expecting that it will be say 1 mA. So, if the I_C of transistor-2 it is 1 mA and then we like to retain the same DC voltage at its emitter, we are maintaining R = 1.2 k and then now the required current here; since its Ξ² it is 100, so the required current here it is close to 10 Β΅A. If I say that this 10 Β΅A base current of transistor Q2 equals the emitter current of Q1.
This section discusses the current flow and the resistance needed in the circuit configuration. It calculates that in order to have a collector current (Ic) of 1 mA through Q2, certain resistances are required to maintain correct voltage levels. It further analyzes the base current required for Q2, which is determined using the beta (Ξ²) value of the transistor, establishing that the base current is significantly smaller. Hence, a very high resistance is necessary to support this current in the circuit.
Think of this as managing a line of dominoes. The first domino (emitter current) needs to be strong enough to tip the next one (base current of Q2) over. If the support (resistance) for that first domino isn't high enough, the chain reaction can't happen smoothly. You need to ensure they are aligned properly to maintain stability.
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So, if I am having these two resistances are known, and then we can find what will be the input resistance of this circuit. The input resistance here is R, it is the parallel connection of R1 and whatever the resistance we do have. And what we have, the resistance here it is r_Ο1 coming in series with (1 + Ξ²)r_Ο2.
This chunk focuses on calculating the input resistance of the CC-CE amplifier configuration. It shows how to determine the overall input resistance as a combination of resistances from both stages, illustrating how to compute a more comprehensive resistance value that is essential for understanding circuit performance in actual applications.
Consider the input resistance like a water pipeline. The input resistance affects how easily water can flow through. If you have a pipe (resistance) that is too narrow or if there are too many intersections (parallel connections), it can impede water (signal) movement. The ideal scenario is to ensure every section of the pipeline facilitates a smooth flow.
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So, C of the circuit it is we do have C of transistor-1. So, we do have C of transistor-1 in Β΅ and this node it is AC ground. On the other hand, this C_Ο breezing the input base terminal and emitter terminal of Q1, its gain is very close to 1, so we may say that the effect of this C_Ο is negligible.
In this section, the impact of capacitance is analyzed. The capacitance of the first transistor is assessed, indicating how it interacts with the system; because the gain of this transistor is almost unity, its capacitance effect is considered minimal, thus not significantly affecting the overall performance of the circuit.
Imagine capacitance as a sponge soaking up water (signal). If the sponge is too small, it wonβt affect how much water flows through (the signal). Since Q1βs gain is close to one, the sponge doesn't hold enough water to matter much, so we can ignore it and focus on bigger issues in the circuit.
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I compare to CC-CE amplifier, there is another configuration something called Darlington pair and we will see that what the difference basic difference is. In fact, their configuration-wise they are very close; but there is a small difference, in the next slide we will be discussing about that.
This last chunk outlines how this CC-CE amplifier configuration can be compared to a Darlington pair configuration. Although both setups are similar, there are distinctions in how they operate, particularly regarding their gains and input resistances. This sets the stage for understanding why one might be preferred over the other depending on the application's requirements.
Visualize a sprinter (Darlington) who has another sprinter (CC-CE) in front of them. Both have great speed (gain) but the sprinter in the Darlington has a minor advantage in agility (input resistance) which may allow them to swiftly navigate corners (circuit complexity) during a race (active operation) making them slightly more efficient in certain situations.
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Key Concepts
Common Collector (CC) Stage: High input impedance and mutual biasing capabilities.
Common Emitter (CE) Stage: Voltage amplification with a lower input impedance.
Biasing: The arrangement to maintain correct operating conditions of transistors.
Input Resistance: Increased input resistance through CC stage enhances amplifier performance.
Input Capacitance: CC stage helps reduce overall input capacitance in CE designs.
See how the concepts apply in real-world scenarios to understand their practical implications.
Example of CC stage providing bias for CE amplifier: CC stageβs emitter current is used to bias the base of the CE stage, simplifying the biasing arrangement.
Numerical calculation showing input resistance enhancements achieved by CC stage before CE stage in an amplifier circuit.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
In CC, the input is free, it's high you see; it feeds CE and helps it be!
Imagine a carpenter (CC) who provides tools (current) to a builder (CE), simplifying the building process (biasing).
Remember 'CC for Current and Coupling' which helps in biasing the CE stage.
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Review the Definitions for terms.
Term: Common Collector (CC) Amplifier
Definition:
An amplifier configuration that allows the output to be taken from the emitter terminal, providing a high input impedance.
Term: Common Emitter (CE) Amplifier
Definition:
An amplifier whose output is taken from the collector terminal, commonly used for voltage amplification.
Term: Biasing
Definition:
The process of setting a transistor's operating point by applying a DC voltage.
Term: Miller Effect
Definition:
A phenomenon where the input capacitance of an amplifier increases due to feedback in certain configurations.
Term: Emitter Current
Definition:
The current flowing through the emitter terminal of a transistor.
Term: Input Resistance
Definition:
The resistance seen by the input source in an amplifier circuit.
Term: Input Capacitance
Definition:
The capacitance associated with the input of an amplifier which can affect high-frequency performance.