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Today, let's start by understanding what a differential amplifier is. A differential amplifier takes two input signals and amplifies the difference between them. Can anyone tell me which components we often use in these setups?
BJTs are often used in differential amplifiers, right?
Exactly! BJTs are commonly employed due to their excellent performance characteristics. Now, can someone explain why we need a tail current in such circuits?
The tail current is necessary to set a stable operating point for the transistors.
Correct! The tail current stabilizes the output and affects the amplifier's gain. Now, remember AC current can mirror DC signals via current mirrors, which we will explore next.
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Let's discuss current mirrors. They are crucial in providing a stable bias current. Who can describe how a current mirror is constructed?
A current mirror typically consists of two matched transistors. One is connected to the reference current, and the other mirrors that reference.
Perfect! This configuration ensures that we have consistent currents flowing through our amplifiers. Why do we prefer current mirrors over resistors for tail currents?
Using current mirrors allows for better linearity and improved gain margins.
Exactly! Remember, this design allows us to replace passive loads, maintaining high performance, which we'll analyze further next.
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Now that we understand current mirrors, let's compare active and passive loads. Can anyone explain the differences in performance?
Active loads generally offer higher gain compared to passive loads.
Correct! Active loads enhance gain but what about their limitation?
Active loads can increase common mode gain, but they also improve differential mode gain simultaneously.
Well said! Balancing these gains is vital for good amplifier design, and thatβs why we analyze them closely in our small signal models.
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Letβs calculate the differential mode gain using our setup. Who can define it for our circuit?
The differential mode gain can be expressed as the ratio of the output voltage to the differential input voltage.
Absolutely! The formula yields interesting results especially with current mirrors included. Which component significantly affects this gain?
The output resistance increases when using active loads, boosting the gain.
Great observation! Remember, analyzing small signal models helps us derive common and differential mode gains effectively.
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The section provides an in-depth examination of differential amplifiers constructed with BJTs, emphasizing the use of current mirrors as tail current sources. It discusses the importance of replacing passive loads with active loads, the implications for differential and common mode gain, and how these configurations can be utilized in circuit design.
In this section, we delve into the construction and analysis of a differential amplifier using Bipolar Junction Transistors (BJTs), particularly focusing on the usage of current mirrors to establish stable tail currents. The integration of active loads in place of passive resistors is explored, comparing the benefits of higher gain and enhanced performance metrics, such as common mode rejection ratios.
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So, we are talking about the differential amplifier particularly constructed by MOSFET. Now we are going to see the differential amplifier using BJT, where we will be deploying the current mirror, corresponding current mirror using BJT and will see the similar kind of situation there.
In this chunk, we are introduced to the concept of differential amplifiers. A differential amplifier is designed to amplify the difference between two input signals. Here, the discussion extends from MOSFET-based differential amplifiers to BJTs (Bipolar Junction Transistors). This sets the stage for exploring how current mirrors can be utilized in these configurations.
Think of a differential amplifier like a judge in a competition, who has to decide which participant performed better despite distractions. The judge listens to both participants, weighing their strengths or weaknesses against each other, much like how the differential amplifier compares and amplifies the difference between two signals.
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In fact, similar to the previous case, you can see that this is the current mirror circuit which is helping us to set the tail current here. Now in this case the reference current I_REF is coming from V_CC. And this reference current based on the reverse saturation current ratio of transistor-3 and transistor-4, we do get current here which is I_C3 = (Ξ²) Γ I_REF multiplied by two nonideality factors.
This chunk explains how the tail current in the differential amplifier circuit is established using a current mirror. The reference current, denoted as I_REF, is generated from the supply voltage V_CC. The relationship between transistors allows for the calculation of the tail current, noting the potential influence of nonideality factors such as base current gain (Ξ²) and other losses.
Imagine a water fountain, where the main water source is the reference current, and the fountain's spray (tail current) lives off this source. The design determines how effectively the fountain (the amplifier) uses the water to create mesmerizing patterns (the amplified signals), influenced by factors like pipe diameter and configurations (which represent nonideality factors).
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Now similar to the previous case, this part can also be replaced by active load and that load current of course, should be consistent with whatever the current we do have flowing through transistor-3.
In this segment, the emphasis is on the comparison between active and passive loads in differential amplifiers. Active loads are often more advantageous because they can provide higher gain and better performance than passive ones. The consistency of load current with the tail current is crucial for the amplifier's effective operation.
Consider a person lifting weights in a gym. If they use weights (passive load), they might tire out quickly. However, if the gym installs a pulley system that assists in lifting (active load), the lifter can manage heavier weights with ease. This analogy highlights the benefit of using an active mechanism in amplifiers to enhance performance.
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Again similar to the previous case here if you analyse we can find the common mode gain. And that can be well approximated by differential mode gain.
This section focuses on analyzing the small-signal equivalent circuit of the differential amplifier. It is crucial to understand how to derive the common mode gain from the small-signal analysis, as it provides insights into how well the amplifier can differentiate between signals of interest and noise or common signals.
Imagine a radio station trying to pick up a specific frequency while drowning out background static. The process of tuning the radio to isolate the desired frequency parallels how a differential amplifier uses small-signal analysis to enhance the quality of the output signal, removing unwanted noise.
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In comparison with this modified gain, if you recall the previous circuit; differential mode gain it was g_m Γ (R_D || r_o1). So, definitely this is having much higher gain.
Here, we discuss the differential mode gain, which is the gain when the amplifier processes differential signals. By comparing previous configurations, the text notes that using an active load significantly enhances this gain. This is important because a higher gain means the amplifier is more sensitive and effective in processing input signals.
Think of a microphone. A high-quality microphone (active load) amplifies soft sounds much more effectively than a basic one (passive load), allowing a subtle whisper to be heard clearly. In a similar way, increasing the differential mode gain enables the amplifier to detect and amplify smaller differences in input signals.
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Key Concepts
Current Mirror: A vital circuit element that stabilizes tail current in differential amplifiers.
Differential Mode Gain: The output signal's amplification relative to the difference in input signals.
Common Mode Rejection Ratio: A measure of an amplifier's ability to reject common mode signals while amplifying differential signals.
Active Load: Component design that enhances the voltage gain in amplifier circuits.
See how the concepts apply in real-world scenarios to understand their practical implications.
A differential amplifier using two BJTs to amplify the voltage difference between two inputs, utilizing a current mirror for stable tail bias.
Replacing a resistor in the circuit with a current mirror improves gain and stability for small signal variations.
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Current mirrors do reflect, stable currents they protect.
Imagine a team of synchronized swimmers, each one reflecting the movements of the leader. Like current mirrors, they keep their moves in perfect sync to form a cohesive performance.
A.B.C. (Active Beats Current) to remember that active loads outperform passive loads in amplifiers.
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Review the Definitions for terms.
Term: Current Mirror
Definition:
A circuit configuration that allows a current to be copied from one branch of a circuit to another, enabling consistent biasing.
Term: Differential Amplifier
Definition:
An amplifier that amplifies the difference between two input voltages while rejecting any common voltage.
Term: Active Load
Definition:
A load that consists of active components designed to increase the gain in amplifiers.
Term: Passive Load
Definition:
A load using passive components like resistors that do not provide power gain.
Term: Small Signal Model
Definition:
A simplified version of a circuit that linearizes non-linear components for analysis at small signal levels.