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Welcome back, everyone! Today, letβs dive into the common source amplifier. What is its main function in circuits?
Isn't it used to amplify voltage signals?
Absolutely! Now, do you remember the significance of parameters like transconductance and threshold voltage?
Transconductance is how effectively the input voltage controls the output current, right?
Exactly! We denote it as `g_m`. And itβs essential to know that the threshold voltage, denoted as `V_th`, is the minimum gate-source voltage needed to create a conducting path.
Why is it important for our calculations?
Without it, we can't determine when the device operates in saturation. Let's remember: 'Threshold is the key to flow!'
Thatβs a good mnemonic!
Thanks! Letβs move on to how these parameters influence our voltage gain.
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Now that we know the parameters, how do we calculate the voltage gain?
Is it just the transconductance multiplied by resistance?
Yes! And in our example, if `g_m` is 2mA/V and the output resistance is 3kβ¦, can anyone calculate the voltage gain?
I think itβs 6!
Exactly! Thatβs a critical takeaway: 'Gain is gain from `g_m` to `R`! Now, letβs discuss the implications of this gain with respect to frequency response.
How does gain relate to bandwidth?
Great question! Letβs calculate upper cut-off frequency next.
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To find the upper cutoff frequency, we need load capacitance along with our output resistance. Anyone remember the formula?
Is it `f_U = 1/(2ΟRC)`?
Yes! With a load capacitance of 100 pF and our earlier resistance, what do we get?
It seems like 530 kHz if I multiplied?
Exactly! So that tells us very important information about bandwidth and gain.
Does that mean our amplifier can respond to signals only up to that frequency?
Right! Understanding how gain and frequency relate in amplifiers is crucial. Now, letβs see how adding a common drain stage changes this.
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We are now ready to discuss how integrating a common drain stage can enhance our overall design. Can anyone remind me what the main benefit is?
It helps extend the bandwidth while keeping the gain stable!
Correct! The overall gain remains around 6. By adding the common drain stage, we can shift our upper cutoff frequency to around 4.24 MHz. This is a tenfold increase!
So, just adding another stage improves performance significantly?
Yes, and it shows the practical benefits of cascading in amplifier design. This realization is essential for modern electronics.
Thatβs really insightful!
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In this section, we delve into the workings of a common drain (CD) stage using a numerical example derived from a common source (CS) amplifier. Key parameters such as voltage gain, output resistance, and upper cutoff frequency are calculated, illustrating the advantages of combining stages to extend bandwidth in amplifier circuits.
In this section, we explore the Common Drain Stage
, also known as the Source Follower, focusing on its role in amplifier circuits. We start with a numerical example based on a common source amplifier scenario, examining the device parameters such as transconductance and threshold voltage. By analyzing the voltage gain, output resistance, and frequency response, we see how the CD stage can improve bandwidth.
The example involves key calculations:
- Voltage Gain Calculation: From the common source configuration, we observe a voltage gain of 6. This is obtained through the product of transconductance (g_m
) and the load resistance.
- Upper Cut-off Frequency: Next, we evaluate the upper cutoff frequency determined by the load capacitance and resistance, yielding values that highlight how cascading stages increases frequency response.
- Performance Enhancement: Finally, the integration of the CD stage allowed for an improvement in the overall bandwidth, showcasing the effectiveness of cascading in multi-transistor amplifiers. The overall gain remains similar to standalone configurations while the bandwidth significantly extends.
This section emphasizes the practical advantages and calculations associated with the common drain stage, preparing students for real-world applications in electronic circuit design.
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So, in the next slide we do have that example here. So, all the informationβs are we are keeping it same we do have additional common drain stage coming out of the transistor M2 and the its bias circuit R and R it is given here it is 1.5 kβ¦. Note that its biasing it is done directly from the DC voltage available at the drain of transistor-1.
In this section, we are discussing how a common drain stage is set up. This configuration includes a transistor, M2, which is the second transistor in the circuit. We start by noting that the additional components involved here are a bias circuit with potentially resistors mapped as R4 and R3, which is given as 1.5kβ¦. This means that the biasing, or how we establish a stable operating point for our transistor, is done using the direct current (DC) voltage available from the previous transistor, which is M1. This is crucial because it allows M2 to operate consistently based on the conditions set by M1.
Think of the biasing process like setting the temperature of a heater based on outdoor conditions. Just as the data from outside decides how warm to make the inside of a home, the voltage from transistor M1 helps determine how M2 will behave in the circuit.
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The DC voltage coming here if you see the current flow of here it is 2 mA and R it is 3 k. So, drop across this 3 k it is 6 V. So, we can say that we do have a DC voltage of 6 V coming to the gate of transistor-2.
Here, we are calculating the source voltage and gate voltage in the common drain configuration. The current in the circuit is specified as 2 mA. There is a resistor R3 of 3 k⦠connected, and hence, we calculate the voltage drop across it by using Ohm's law (V = IR). With the known current, we find the voltage drop, which results in a DC voltage of 6 V at the gate of transistor-2.
It's akin to how water pressure is measured in a pipe. The water flow (the current) and the resistance in the pipe (the 3 k⦠resistor) gives the pressure drop along the pipe, which is analogous to the voltage drop we calculate here.
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How do you find the corresponding current here I_DS? So, there is a method first of all this I_DS flowing through this R creating a drop which is defining the source voltage here and then at the gate we do have 6 V.
To determine the drain-source current (I_DS) in this stage, we notice how this current flows through the resistor R4, creating a voltage drop that sets the source voltage. Since we know both the gate voltage (6 V) and how current flows in relation to this setup, we can apply similar principles from earlier calculations to establish the current level through transistor-2.
Imagine a scenario of filling a tank with water. The inlet (gate) provides water pressure (voltage) to fill up to a certain level. The current flowing through the drain can be likened to the amount of water flowing out once the tank reaches this specific level.
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Now, since this equation it is coming primarily in terms of V_GS - V_th let me consider this is x. So, we can say that this is x = 5 - R4(1.5 k)(1m).
In this chunk, we are manipulating the equation to solve for the gate-source voltage (V_GS) concerning the threshold voltage (V_th). We designate the equation variables and solve for x, which in this case simplifies down to a quadratic equation. Ultimately, our solution reveals two potential values for x, but only one solution is practical, leading us to deduce that V_GS = V_th + 2V.
Think of balancing your bank account. You subtract (threshold voltage) from your total balance (V_GS) to see how much you can actually spend. Here, we are effectively determining how much voltage we can utilize after accounting for the threshold voltage needed to operate the transistor.
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So, the g of this transistor it is Γ (V_GS - V_th). So, here also we got g = 2 mA/V and then the output resistance and of course, since we do not have the equivalent whatever r we are having in BJT.
In this segment, we calculate the transconductance (g) and output resistance of the transistor in the common drain stage. The transconductance is derived from the earlier voltage findings, which gives us a value of 2 mA/V. Since the structure of MOS transistors differs from BJTs, this output resistance can be considered much simpler, allowing us to assume the output gain is nearly one.
Consider a tuning fork or a spring: the sensitivity to changes (transconductance) will define how well it resonates (amplifies). In this analogy, the output resistance allows us to understand how 'quiet' or stable the output signal will be when affected by these changes.
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Now, if I call it is fβ² it is having 2 candidates to define the upper cut off frequency; one is R_O2 and the corresponding load capacitance we do have C_L.
Here we explore the upper cutoff frequencies resulting from our circuit's design. In any electronic circuit, the cutoff frequency is critical to determining how capable the circuit is at amplifying various frequencies. We consider two potential contributors to the cutoff frequency: the load capacitance and the resistance from the circuit. By comparing calculations and ensuring we capture the lower limit, we can efficiently optimize bandwidth.
This is similar to how a sound system has different frequencies it can play. For example, a subwoofer handles low frequencies while tweeters handle high ones. Just as the system needs both types of speakers to produce a full range of sound, we take into account multiple sources of cutoff frequency to ensure our circuit can operate over a broad spectrum of signals.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Voltage gain is essential for determining how much an amplifier can amplify a signal.
Common drain stages can enhance bandwidth while keeping the gain stable.
Understanding transconductance is critical to evaluating amplifier performance.
Upper cutoff frequency determines the effective operational range of an amplifier.
See how the concepts apply in real-world scenarios to understand their practical implications.
A common source amplifier with a voltage gain of 6 representing the ratio of output to input voltages.
Cascading a common drain stage with a common source stage to achieve a bandwidth increase from 530 kHz to 4.24 MHz.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
Gain is gain from g_m
to R
, cascading amplifiers will take you far.
Imagine an amplifier trying to shout louder. It meets a common drain stage, its voice gentle yet firm, spreading out the sound while keeping its strength. Together, they reach new frequencies, amplifying without losing clarity.
G.R.E.A.T for remembering: Gain, Resistance, Enhance, Amplify, Threshold.
Review key concepts with flashcards.
Review the Definitions for terms.
Term: Common Drain Stage
Definition:
Also known as a source follower, it is an amplifier configuration used primarily for voltage buffering.
Term: Voltage Gain
Definition:
The ratio of output voltage to input voltage in an amplifier.
Term: Upper Cutoff Frequency
Definition:
The frequency at which the gain falls off by 3 dB from its maximum value.
Term: Transconductance (g_m)
Definition:
The ratio of the change in drain current to the change in gate-source voltage.