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Today, we will discuss how we can cascade Common Emitter amplifiers. Who can tell me why we might want to do this?
To increase the overall gain of the amplifier circuit!
Good! Indeed, cascading allows us to combine the gains. However, there's a catch. Can anyone guess what might happen to the gain when we cascade these amplifiers?
Maybe it will drop off because of loading?
Exactly. That's due to the attenuation factor introduced by the loading effect. Remember, βLoading leads to lessβ β itβs a great way to recall the essence!
What happens to the frequency response when we cascade?
Great question! The frequency response can also shift. The upper cutoff frequency can drop due to how these components interact. Letβs keep this in mind as we move forward!
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Let's dive deeper into how attenuation occurs. When we have two cascaded amplifiers, their gains should multiply, right?
Yes, but if the resistances are significant, will that not change things?
Absolutely! If the output resistance of the first stage is comparable to the input resistance of the second, it creates a voltage divider effect. Hence the term βattenuation factorβ reflects how much gain we actually lose due to loading.
Can we calculate that attenuation?
Yes! It can often be visually represented as R_out / (R_out + R_in). Keep this factor in mind β youβll encounter it frequently in design!
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Now, let's consider how cascading affects the frequency response. Who can explain what happens to the upper cutoff frequency?
It decreases, depending on the new effective capacitance, right?
Correct! The effective capacitance might include Miller effects. Itβs crucial to analyze this to maintain signal integrity through the cascading stages!
So we need to manage that capacitance to keep the response stable?
Exactly! βControl capacitance to sustain responseβ is another good mnemonic to remember!
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We have identified the problems β what's our solution? How do we prevent loading effects when cascading amplifiers?
By using buffers between the stages?
Exactly! Buffers should have high input resistance and low output capacitance. This minimizes loading, preserving both gain and frequency response.
So we can restore the expected performance of our system!
Right! Remember, buffers act like βwalls of protectionβ against loading β keep that image in mind!
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Cascading Common Emitter and Common Source amplifiers can lead to unexpected drops in gain and cutoff frequency due to loading effects. By analyzing these effects, we identify the need for buffers to mitigate attenuation and maintain frequency response. Key concepts include attenuation factors and their impact on overall amplifier performance.
In this section, we explore the limitations associated with cascading Common Emitter (CE) and Common Source (CS) amplifiers. These configurations are known for their amplify characteristics; however, when cascaded, they exhibit notable performance constraints. The main focus is on the attenuation caused by loading effects, which can significantly impact both gain and upper cutoff frequency.
Understanding these concepts is crucial for designing effective multiphase amplifier circuits in analog electronic systems.
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So, how we do that output of the first CE amplifier will be connecting to the input of the second CE amplifier. But of course, with the use of C we can isolate the DC operating point of the first stage and the second stage. And of course, the capacitor C it is supposed to be allowing the signal going from the output of the first stage to the input of the second stage.
Now, while we will be connecting this circuit we may be expecting that suppose we do have a gain of this stage; it is say A and then gain of this stage it is say A, we may be expecting that the overall gain say A = A Γ A.
This chunk explains that when two Common Emitter (CE) amplifiers are connected in series (cascaded), the output of the first amplifier is connected to the input of the second amplifier through a DC blocking capacitor, which prevents DC voltage levels from affecting each other. We expect to achieve a high overall gain by multiplying the individual gains of each amplifier. For instance, if the first stage has a gain of A1 and the second stage has a gain of A2, the overall gain should be A = A1 Γ A2.
Think of this like a relay race where each runner (amplifier stage) has a specific speed (gain). If the first runner has a speed of 5 meters per second (A1) and the second runner has a speed of 3 meters per second (A2), you would expect the total speed of the race to be 15 meters per second (A = 5 Γ 3). However, if something slows them down (like loading effects), they won't achieve that expected speed.
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So, the observation we may see two important things; that the gain low free or mid frequency gain it may be different from the product of mid frequency gain of the two individual stages, and also the upper cutoff frequency may be different. For instance, if we combine these two stages through this cascading, we may be expecting that the overall frequency response it may be having very high gain, and then the lower cutoff frequency is defined by whichever the lower cutoff frequency of the two stages is higher.
When we connect two amplifiers, we often find that the actual mid-frequency gain is lower than what was expected from simply multiplying the individual gains. This is partly due to loading effects, which occur when the input impedance of the next stage interacts with the output impedance of the previous stage. Similarly, the frequencies (cutoff frequencies) where the amplifier effectively operates can be shifted. The lower cutoff frequency is determined by the highest of the two individual stage's lower cutoff frequencies.
Imagine two teams working on a project together, where one teamβs progress affects the other's ability to work efficiently. If they both have deadlines for their parts of the project but one team performs slower due to interruptions, the overall project completion time (gain) will be longer than expected. Just like this, the 'cutoff frequency' shifts based on the slower team's impact on the overall timeline.
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So, we can say that whatever the voltage it is we are getting here of course, that is considered as v and the second stage it is amplifying that. So, the voltage coming at the primary output we can say, it is say v = A Γ v and then this v; this v, it is A Γ v multiplied by the attenuation factor.
The chunk discusses how the output voltage from the first amplifier is reduced (attenuated) due to loading effects before it is sent to the second amplifier. The voltage at the output of the entire cascaded amplifier setup is not just the product of the two gains but also includes an attenuation factor. This attenuation is influenced by the relationship between the input and output resistances of the stages.
Think about filling a glass with water where the faucet provides a steady flow (gain), but the size of the glass is very small (loading). If the glass is too small, even if the faucet is wide open, not all the water can be collected. The glass size can be thought of as the loading effect, leading to less water than anticipated at the end. Here, the actual amount of water in the glass represents the output voltage after accounting for the attenuation factor.
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So, we can say that whatever the input capacitance it is coming primarily from this C and C. So, that we can write say this is C of the second stage; and then this C it is C almost yeah C Γ the (1 + the second stage gain A); and. Since, we do have a very good gain of the second stage that makes the C this C it is very significant.
The upper cutoff frequency in cascaded amplifiers can also change because of added capacitance. When amplifiers are cascaded, the capacitance seen by the input increases due to the first amplifier's output capacitance interacting with the second amplifier's input capacitance. This can lower the upper cutoff frequency, meaning that the cascaded amplifier may not handle high frequencies effectively.
Imagine a bottleneck created in a water supply system. If there are pipes of different diameters connected in series, the narrowest section limits how much water can flow through at higher pressures (frequencies). Likewise, when amplifiers are cascaded, the interaction of their capacitances reduces the range of high frequencies that can be amplified effectively.
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If we put a buffer; so if we put a buffer say or say some intermediate circuit having some important feature we will be discussing that such that, the input resistance of this stage; call R_buff, if it is quite high then whatever the attenuation it will be getting introduced by R and R. If that is approximately 1 then we can say that the cascading effect here it is very small.
The necessity of incorporating a buffer amplifier into the circuit setup is highlighted in this chunk. A buffer amplifier helps to isolate the stages and can prevent unwanted loading effects that might cause attenuation of the signal. If the buffer's input resistance is high enough compared to the loading resistances, it helps maintain the overall gain of the cascaded circuit.
Consider a middleman in a transaction who can also help ensure that both parties get their fair deal without influencing each other's contributions. In audio systems, a buffer amplifier acts like that middleman, ensuring the signalβs integrity is maintained while also accommodating the needs of each amplifier stage without causing a 'loss' in signal.
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Key Concepts
Cascading Amplifiers: Combining multiple amplifier stages to achieve desired gain.
Attenuation Factor: The reduction in gain due to loading from interactions between amplifier stages.
Buffer Circuits: Components designed to isolate signals and minimize loading effects.
See how the concepts apply in real-world scenarios to understand their practical implications.
Consider a CE amplifier with a gain of 10 connected to another with a gain of 5. Expected gain would be 50. However, due to loading, the actual gain could be significantly lower.
A buffer stage with high input resistance isolates the preceding stage from affecting the following stage, thus preserving the expected frequency response.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
When amplifiers combine to amplify, loading can make signals shy.
Imagine a river (amplifier gain) flowing into two ponds (cascaded stages). If the ponds (inputs) are too deep (high resistance), water flow (signal) decreases. A strong dam (buffer) helps sustain the water flow!
A for Amplifier, B for Buffer, G for Gain, L for Loading.
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Review the Definitions for terms.
Term: Common Emitter Amplifier
Definition:
A type of amplifier where the emitter terminal is common to both input and output; known for high gain.
Term: Cascading
Definition:
Connecting two or more amplifiers in series to increase overall gain.
Term: Attenuation Factor
Definition:
A ratio that reflects the reduction in voltage gain caused by loading effects in cascaded stages.
Term: Buffer
Definition:
A circuit component used to isolate and manage the load between two stages of an amplifier.
Term: Upper Cutoff Frequency
Definition:
The frequency above which the amplifier gain begins to roll off, significantly affecting circuit performance.