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Good morning, class! Today we will look into differential amplifiers. Can anyone explain why we need to consider common mode voltage in these circuits?
Isnβt it because we want to ensure the transistors operate properly under varying input conditions?
Exactly! Common mode voltage affects how we operate the transistors. We need to make sure both are biased properly, typically above 0.6V for BJT operation. Let's remember this as 'Minimum Bias Voltage (MBV)'.
How do we find out what common mode voltage range is suitable?
That's great! We'll explore calculations that reveal upper and lower limits of common mode voltage later.
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Now, letβs calculate the current through a resistor in the circuit. If you apply a 0.8V DC voltage across a 1 kβ¦ resistor, what current do you expect?
Oh! Using Ohm's law, I = V/R, we can find it!
So that would be 0.2 mA?
Correct! That current sets our voltage drops further down the circuit. Remember, this value is 'Critical Current (CC)'.
Could this affect output voltage?
Absolutely! That brings us to output voltage calculations when considering both differential and common mode gains.
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What happens to output voltage when our input conditions change?
If the differential signal increases, the output should increase proportionally based on the gain!
Exactly! Thatβs why we compute differential mode gain, highlighted as 'Differential Gain (DGA)'. In our previous calculations, we found this gain to be 200 in one scenario.
And the common mode gain is lower, right? It affects how clean our output signal is?
Yes! We've seen how common mode components can distort our output. Balancing both gains is vital.
Can we adjust our design to improve the gain?
We certainly can! We will discuss modifications in upcoming sessions.
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It covers the concept of common mode voltage in differential amplifiers, explaining how to calculate suitable ranges while considering the operating points and gain effects. Several numerical examples elucidate the implications of these calculations on circuit design, ensuring both theoretical and practical understanding.
In this section, we delve into the workings of differential amplifiers, focusing on the impact of common mode voltage and associated numerical examples. The discussion begins with basic assumptions on DC voltage values required for operating the transistors in the active region. The students learn to calculate the suitable range of common mode voltages and the implications of varying these voltages on the device's performance, particularly within the context of a BJT-based differential amplifier. Multiple scenarios illustrate the changes in current, voltage drop, and overall gain. The complexities of distinguishing between differential and common mode gains are highlighted, alongside detailed calculations that demonstrate the operational limits imposed by the choice of voltage levels.
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So, we are talking about the Differential Amplifier and we assume that we do have meaningful value of this DC voltage. So, our next exercise is to find what may be the range, suitable range of this common mode voltage.
So, here we are having some value of V which is just 0.8 V. In fact we need this INC voltage to be at least 0.6 V because to make Q and Q ON, we need the V voltage sufficiently high.
In this part, we focus on the differential amplifier and its common mode voltage range. To operate correctly, the input voltage, denoted as V_INC, must be adequate to turn on the transistors Q1 and Q2. The minimum voltage required for proper operation is 0.6 V. The text mentions that the value we are using is 0.8 V to ensure it's high enough for this purpose.
Think of a differential amplifier like a light switch. To turn on a light (representing the amplifier's operation), the switch (input voltage) needs to be pressed down sufficiently (minimum voltage). If you only apply a little force (less than 0.6 V), the light remains off. But if you apply enough pressure (0.8 V or more), the light turns on.
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So, here just we are taking 0.8 V so that the drop across this resistance it is only 0.2 V. So, if the voltage here it is only 0.2 V and R it is 1 k⦠and the DC voltage here it is 0.8 V which is given here. So, the current flow here it is 0.2 mA.
This segment explains the process of calculating the current flowing through a resistor when a voltage is applied. Given a resistor (1 kβ¦) and a voltage drop (0.2 V), the flow of current can be calculated using Ohm's Law (I = V/R). With a 0.2 V drop, the current would be 0.2 mA. This understanding forms a foundation for how differential voltage amplifiers operate.
Imagine a water pipe; the voltage drop is like the pressure of water in the pipe. If you have a small pressure (0.2 V), a small amount of water (current) flows through the pipe (resistor). If the pipe is wider (lower resistance), more water could flow, but here we are constrained by how narrow the pipe is (1 kβ¦).
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So, if it is 0.5 V here the minimum value of the output voltage then we do have a very good swing of 11 V, close to 11 V. So, βve side swing is not a problem but the +ve side swing it is very small 0.52 V so, that is the first problem.
This portion discusses the output voltage swing from the amplifier. The output can swing positively up to 0.52 V and negatively to 0.5 V, creating a swing range of nearly 11 V. However, the positive swing is very limited compared to the negative swing, which could lead to performance issues.
Think of a swing in a playground. If the swing can only go up slightly in one direction (positive side swing), but can go far down (negative side swing), it might not be fun or can cause issues in use. A well-balanced swing should have equal movement in both directions for optimal performance.
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So, the differential mode gain A_d = g_m R_C = . So, that is equal to only 20. So, the gain you may recall the previous case when the current here it was 1 mA, the gain it was 200, now it comes to 20.
Here, the differential mode gain (A_d) is calculated, indicating how much the amplifier can amplify the input signal. With lower current (0.1 mA compared to 1 mA previously), the gain decreases from 200 to just 20, which indicates that the output signal (v_o) will now only be 0.4 V instead of 4 V, significantly reducing amplification.
Consider a microphone amplifier. When you speak softly (lower current), the amplifier captures only a whisper (gain of 20), whereas if you shout (higher current), the amplifier captures your voice clearly and loudly (gain of 200). Lower input levels lead to poorer amplification in the signals picked up by the device.
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So, the common mode gain A_C = β . And the g_m = β§. So, the numerator it becomes 20 which we already have calculated, and here we do have ( ). So, I do have the common mode gain, it is not having much change, in fact it is only β 2.3 instead of β 2.6.
This part covers the calculation of common mode gain (A_C) which measures how much the amplifier outputs a signal that is common to both inputs. In this case, the change in common mode gain is minimal, remaining around -2.3, indicating that the amplifier's ability to reject noise or unwanted signals has not significantly altered.
Think of tuning a radio to pick up music while ignoring static (common noise). A good radio (amplifier) has better performance if it can reject unwanted signals. A stable common mode gain suggests the radio can effectively filter out noise and focus on the music, regardless of changing volumes.
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So, indicating that this voltage probably it is quite low and it is alarmingly low and the gain here it is very small particularly the value of g_m is small and that is coming from the device it is almost in the, I should say towards the cutoff.
This section emphasizes the importance of maintaining a proper operating point for the amplifier to function effectively. A low voltage can cause the transistor to approach the cutoff region, where it fails to operate optimally, resulting in reduced gain and distorted signals.
Imagine a car engine that runs best at a specific speed (operating point). If the car runs too slow (low voltage), it may stall or lose power, struggling to reach the desired speed, just like how an amplifier can falter in performance if not maintained at its ideal conditions.
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So, this is the exercise we can try, what maybe the maximum value of this V keeping both Q and Q in active region of operation.
This section presents an exercise to determine the maximum value of the input voltage (V_INC) while ensuring that both transistors are in their active operating region, which is essential for linear amplification without distortion. The goal is to find the balance where increasing input voltage won't push the transistors into saturation or cutoff.
Consider trying to fill a cup with water; you can only pour in so much before it overflows. Finding that maximum amount of water without spilling on the table (maximum voltage without saturating the transistor) is crucial to ensure nothing goes to waste and performs as expected.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Common Mode Voltage: The average voltage in differential amplifier inputs that may affect signal integrity.
Differential Gain: The foundational measure of how much an amplifier amplifies the difference between its inputs.
See how the concepts apply in real-world scenarios to understand their practical implications.
Example of calculating the current flow through a resistor using Ohm's law in a BJT differential amplifier.
Example detailing how to find the output voltage when subjected to common mode gains.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
In amp design, donβt forget, common mode knows its debt.
Imagine two brothers, one represents V1 and the other V2, when they fight, their output is distorted, just like the amplifier!
DCs help Affirm: V biases are a must for normal amplify.
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Review the Definitions for terms.
Term: Common Mode Voltage
Definition:
The average voltage present in both inputs of a differential amplifier.
Term: Differential Gain
Definition:
The ratio of output voltage to differential input voltage in a differential amplifier.
Term: Transconductance (g)
Definition:
A measure of the gain of a device in converting voltage into current.