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Today, we'll discuss cascode amplifiers. These amplifiers improve voltage gain and bandwidth compared to traditional common emitter amplifiers. Can anyone tell me why we use cascode amplifiers?
Is it because they provide better frequency response?
Exactly! They help minimize the Miller effect, which in turn aids in achieving higher cutoff frequencies.
What about their construction? Are they much different than CE amplifiers?
Great question! Cascode amplifiers involve stacking two transistor stages, optimizing performance at both low and high frequencies.
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Now let's work through a numerical example. We will consider transistor parameters such as Early voltage and transistor beta. Can anyone remind me what Early voltage signifies?
It indicates the output impedance or the effect of base-width modulation!
Correct! We assume our Early voltage is 100V. Given two BJTs in the circuit, we can calculate the operating point.
How do we find the collector current I ?
Excellent inquiry! Start with the supply voltage minus the V_BE drop divided by the respective resistor.
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We have calculated the small-signal parameters. Now let's find the voltage gain. Who remembers the formula to express voltage gain?
Is it v_o over v_in?
Close! It’s indeed the output voltage divided by the input voltage. Let’s plug in our calculated values.
So, we are calculating the gain from the base to output, right?
Exactly! And this voltage gain will show how effectively our amplifier converts input voltage into output voltage.
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Let's compare the performance. What key differences do you think exist between a cascode amplifier and a common emitter amplifier?
I think the bandwidth is different due to input capacitance...
That's right! Cascode amplifiers usually exhibit a higher bandwidth than a simple CE amplifier due to reduced input capacitance effects.
Does that maintain performance with high frequencies?
Precisely! Cascode amplifiers excel in preserving signal integrity across the desired frequency range.
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In this section, the voltage gain of cascode amplifiers using BJTs and MOSFETs is analyzed with detailed numerical examples. The significance of different parameters such as voltage gain, input capacitance, and frequency response are evaluated, culminating in a comparative analysis with common emitter amplifiers.
This section focuses on the voltage gain analysis of cascode amplifiers, primarily using Bipolar Junction Transistors (BJTs) and, briefly, Metal-Oxide-Semiconductor Field-Effect Transistors (MOSFETs). The lecture highlights the advantages of cascode amplifiers over simple Common Emitter (CE) amplifiers, particularly in terms of voltage gain and bandwidth.
A significant part of this exploration includes numerical examples that provide specific values for various components, such as the Early voltage, transistor beta (β), coupling capacitors, and biasing resistances. The voltage gain computation is detailed step-by-step, using derived small-signal parameters to reach an overall voltage gain. The session discusses the impact of different resistance configurations and capacitances on input and output signals, noting how these configurations affect the circuit's operational bandwidth.
Furthermore, the advantages of cascode amplifiers in creating higher cutoff frequencies and reducing input capacitance effects in comparison to CE amplifiers are discussed. Ultimately, the voltage gain and frequency response of both amplifier configurations are laid out for comparison.
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So, what is the voltage gain? So, try to remember these values of the small signal parameters to get the voltage gain.
Voltage gain (A) is a measure of how much an amplifier boosts the input signal. It is defined as the ratio of the output voltage (v_out) to the input voltage (v_in) of the amplifier. In this context, you should recall the small signal parameters that were determined earlier to calculate the voltage gain.
Think of voltage gain like a microphone amplifying your voice. If you speak into the microphone at a soft volume (input), and the sound recorded by the microphone is loud (output), then the microphone has a high gain because it made your voice much louder.
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Now this is the gain from the base terminal or transistor-1 till the output point. Now if I consider this R = 1.3 k. Why did I take 1.33 k? Just for simplicity that, the input resistance here in this circuit calls R which is (r and r it is 1.3 k)
When calculating the overall gain of the circuit, the gain from the base terminal of transistor-1 to the output refers to how much the input at this point is amplified at the output. The choice of R = 1.3 kΩ simplifies calculations since it represents the combined effect of input resistances.
Imagine turning the volume knob on your stereo. If the input (your music source) has a certain loudness and you turn it up a small amount (gain), you'll observe a significant increase in loudness coming from the speakers. Here, the resistors play a similar role in determining how much 'turning up' happens.
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So, overall gain A defined as the primary output divided by primary input.
The overall gain A can be calculated by taking the output voltage and dividing it by the input voltage. This gives a clear picture of how much the amplifier enhances the signal. It often takes into consideration multiple factors, including the different resistances and gain contributions from various parts of the circuit.
Think of it as a performance. If a singer usually sings at a volume of 80 decibels (dB) and with an amplifier it reaches 100 dB, then the overall gain is 100/80 = 1.25, meaning the sound is 25% louder. Here, the calculations also factor in the overall effect of different elements in the circuit similar to how the musician's vocal quality or electronics contribute to the total sound.
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So, C_in, input capacitance of this entire circuit looking at the base of transistor-1 which, is equal to C and C. And then C of course, it is bridging the base and the collector terminal of transistor-1.
The input capacitance (C_in) affects how quickly the amplifier can respond to changes in the input signal. It is determined by the capacitances associated with the transistors and any external capacitors. When these capacitors are combined, they form an effective capacitance that influences the amplifier’s frequency response.
Think of the input capacitance like a sponge soaking up water. The larger the sponge (capacitance), the more water (signal) it can hold. This means that if the sponge is too filled, it takes longer for it to absorb additional water. Similarly, if the input capacitance is too high, the circuit may not respond quickly enough to changes in the input signal.
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The reason is that the gain of this cascode amplifier you may recall if I consider R and then the overall gain, it was.
The configuration of the cascode amplifier affects its performance benefits, including the voltage gain and bandwidth. By comparing it to a simple common emitter amplifier, certain configurations can provide better performance characteristics, despite seeming similar in gain values.
Imagine two types of teams playing basketball: a well-coordinated team (cascode amplifier) that can pass quickly and efficiently compared to a less coordinated one (common emitter amplifier). Even if both teams score the same number of points (gain), the well-coordinated team might perform better under pressure (bandwidth), due to their strategies.
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So, to summarize that, if I compare the common emitter amplifier and then cascode amplifier; we can say that, for both the circuits the gain it is very close to each other.
In conclusion, while both the common emitter and cascode amplifiers have similar gains, the cascode design offers advantages in terms of input capacitance and bandwidth. This makes it more suitable for high-frequency applications where quick response to changes in voltage is critical.
Think of the cascode amplifier like a sports car that accelerates smoothly (higher bandwidth), while a regular car (common emitter) might not respond as fast when you hit the gas pedal. Even if both might reach a similar top speed (gain), the way they get there and handle roads can differ drastically.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Voltage Gain: The ratio of output voltage to input voltage, indicating amplifier effectiveness.
Cascode Amplifiers: Two-staged amplifiers that improve gain and reduce Miller effect.
BJT Parameters: Key elements like early voltage and beta, which influence amplifier performance.
Input Capacitance: Affects operational bandwidth and overall efficiency of amplifiers.
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In a cascode amplifier with an Early voltage of 100V and β values of 100 and 200, the voltage gain was calculated to be 107, illustrating the amplifier's efficiency.
When comparing a cascode amplifier to a common emitter amplifier, it was found that the input capacitance for the cascode configuration was 20pF, resulting in a higher cutoff frequency approximately 12 MHz, while the CE amplifier had 125pF leading to a lower cutoff frequency of 237kHz.
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For voltage gain so great, use cascode, it’s no debate! Higher bandwidth, it's the rate, helps your signal permeate.
Imagine a busy highway where cars move smoothly. The gradual incline in the middle section acts like a cascode amplifier, allowing traffic to flow without interruption, improving travel times — just like amplifiers enhance signal clarity.
CASCODE: C (Cascading), A (Amplifies), S (Signal), C (Clarity), O (Optimizes), D (Drain), E (Efficiency)
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Review the Definitions for terms.
Term: Voltage Gain
Definition:
A measure of how much an amplifier increases the voltage of a signal.
Term: Cascode Amplifier
Definition:
An amplifier configuration that stacks two transistor stages to improve gain and bandwidth.
Term: BJT (Bipolar Junction Transistor)
Definition:
A type of transistor that uses both electron and hole charge carriers.
Term: Early Voltage
Definition:
The voltage at which the current through a BJT becomes independent of the collector voltage.
Term: Bandwidth
Definition:
The range of frequencies over which an amplifier operates effectively.
Term: Input Capacitance
Definition:
The capacitance that an input signal sees when it enters an amplifier.