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Today, we are discussing common collector amplifiers. Can anyone explain what the main purpose of a common collector configuration is?
Isn't it mainly to provide high input impedance and low output impedance?
That's correct! It effectively acts as a buffer. High input impedance minimizes loading effect on the previous stage. We can remember this as 'HIL'βHigh Input, Low output!
What about its applications?
Itβs primarily used in impedance matching. Can someone suggest a situation where that might be crucial?
In audio applications, where we need to connect microphones with high impedance to amplifiers?
Exactly! Now, letβs summarize key points: Common collector amplifiers serve to match impedances and reduce signal loss.
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Letβs dive into calculating the small signal parameters like transconductance (gm) and output resistance (ro). Who remembers the formula for transconductance?
I think itβs gm = Ic/Vt, where Ic is the collector current?
Exactly! If Ic is 0.5 mA and Vt is 26 mV, what would gm be?
That would be about 19.23 mS!
Correct! And how does ro relate to this?
Itβs related to the Early voltage, right? ro = Early Voltage/Ic.
Spot on! Letβs summarize: transconductance and output resistance are crucial parameters influencing amplifier performance!
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Now that we understand small signal parameters, letβs evaluate the upper cutoff frequency. Who can tell me how we calculate it?
Is it related to the output impedance and capacitance, like f_upper = 1/(2ΟRoCL)?
Correct! If we have a load capacitance of 100 pF and output resistance of around 50 β¦, can you calculate the upper cutoff frequency?
Using the formula, it would be approximately 318 KHz.
Well done! Remember, higher capacitance could lead to reduced cutoff frequency; weβll call this the βCapacitance Cautionβ!
Thatβs a great way to remember it!
Great discussion today. Summarizing: Upper cutoff frequency ties directly with output impedance and load capacitance.
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Next, letβs consider how varying the source resistance impacts our circuit. Why would this matter?
It can affect the bias point and subsequently the voltage gain.
Exactly! If we assume a source resistance of 100kβ¦, would the gain still be close to 1?
Yes, but the voltage drop across it might change the base voltage.
Right! This is why we ensure our source resistance is minimized. Let's call the principle: βLess Resistance, More Precisionβ!
Iβll remember that!
To recap: Source resistance influences gain via bias voltage; minimizing resistance improves stability.
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In this section, students learn about the upper cutoff frequency in common collector and common drain amplifiers through numerical examples. It covers the significance of small signal parameters and how they impact overall performance metrics such as voltage gain, input and output impedance, and the operating point of the circuits.
This section focuses on the reevaluation of the upper cutoff frequency in common collector and common drain amplifiers. The discussion begins with the operating parameters of a typical common collector amplifier, where various significant aspects are analyzed, including:
Key numerical examples illustrate the calculation of the operating point, where concepts like voltage gain, input and output impedance play a significant role. The section emphasizes how small variations in the source resistance can affect performance without drastically changing small signal parameters, thereby maintaining a high upper cutoff frequency. Overall, the interplay of parameters like load capacitance and circuit resistances are explored thoroughly to equip students with a keen understanding of amplifier behavior under varying conditions.
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So, we can say that the upper cutoff frequency now, so this is done. Now the upper cutoff frequency if I say that f upper cutoff frequency, it is . So that is, let me use different color should see ( ) R C .
The upper cutoff frequency (f_u) is the frequency beyond which the output voltage of the amplifier starts to significantly drop off. It's important to determine this frequency for understanding how the amplifier behaves at higher frequencies.
Think of the upper cutoff frequency as a sliding door. Once you push it too hard, it doesn't slide open anymore; instead, it starts to close. Similarly, at frequencies beyond the cutoff, the amplifier cannot amplify signals effectively.
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So, we do have . So, that is 1010 alright, and so this is 10β10. So, that comes to be 1012, 1010 divided by approximately or say to be more precise 104 Γ Ο. So, that is .
The actual formula for the upper cutoff frequency is f_u = /(R_C imes C_L), where R_C is the output resistance and C_L is the load capacitance. Here, numerical estimations are done to simplify the calculation, leading to an approximate cutoff value.
Imagine trying to fill a balloon with water (analogous to signal current). Once the water pressure exceeds its capacity (upper cutoff), the balloon starts leaking, similar to how the amplifier fails to process signals effectively past the cutoff frequency.
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So, roughly we can see that approximately if I say that this part it is 3 and then this is almost 100. So, that is 10, 10 to the power it is now, this is we do have another 100. So, this is 108. So, we do have 100 divided by no.
The calculations yield an approximate upper cutoff frequency of around 30 MHz. This means that the amplifier can effectively amplify signals but starts to lose its ability to do so as the frequency approaches 30 MHz.
The 30 MHz cutoff frequency can be likened to a loudspeaker. It can handle up to a certain high pitch (30 MHz), beyond which the sound distorts or fades, much like the amplifier's performance at higher frequencies.
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So, let us see in the next circuit that if we consider source resistance R which is say may be having some practical value. Then you can see what will be the corresponding impact.
The load capacitance (C_L) has a significant effect on the overall behavior of the amplifier, particularly in defining the upper cutoff frequency. This section suggests analyzing circuits under practical conditions, which can affect the frequencies at which they operate effectively.
Imagine trying to drive a car with heavy cargo. The car can move faster (signal amplification) until a certain limit (cutoff frequency). As you add more cargo (increase load capacitance), the car slows down and may struggle to reach higher speeds, much like how high load capacitance slows the amplifier's response.
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So, in the next slide, it is basically the same circuit except, here we are considering the R different from different from 100 k.
When introducing a different source resistance (R_S), the effects regarding the cutoff frequency and output impedance become crucial. This change can demonstrate how sensitive the amplifier is to such variations in circuit design.
Consider a singer's performance where the microphone (representing the amplifier) picks up sound differently based on distance (source resistance). The further away the singer stands (higher source resistance), the less effective the microphone is at capturing sound, illustrating how variations in source resistance can diminish performance.
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Key Concepts
Common Collector Configuration: High input impedance and low output impedance for signal buffering.
Transconductance: Key parameter affecting voltage gain and defined as Ic/Vt.
Upper Cutoff Frequency: Determined by output resistance and load capacitance, crucial for frequency response.
See how the concepts apply in real-world scenarios to understand their practical implications.
Example of a common collector amplifier circuit providing voltage gain close to 1.
Calculating transconductance and its effect on the amplifier's performance.
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High input, low output, thatβs the way, Common collector amplifiers save the day!
Imagine a busy librarian (common collector) who manages the quiet section (high input) and directs traffic to borrowing books (low output) without losing any readers!
For Upper Cutoff Frequency, remember: 'U Can Find Rollover' - Upper Cutoff = 1/(2ΟRoCL)
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Review the Definitions for terms.
Term: Common Collector Amplifier
Definition:
An amplifier configuration characterized by high input impedance and low output impedance, commonly used for signal buffering.
Term: Transconductance (gm)
Definition:
A measure of the control of the output current by the input voltage in an amplifier; defined as the collector current divided by thermal voltage.
Term: Output Resistance (ro)
Definition:
The resistance seen by the load at the output terminal of the amplifier, influencing gain and performance.
Term: Upper Cutoff Frequency
Definition:
The frequency at which the output signal power falls below half of its maximum value; determined by load capacitance and output resistance.