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Today we'll be discussing differential amplifiers. Can anyone tell me what a differential amplifier does?
Is it used to amplify the difference between two voltages?
Exactly, a differential amplifier amplifies the difference between two input signals. It rejects common-mode signals, which is crucial for improving signal quality. Remember 'Differential = Different' to help you remember this key concept.
So, what's special about the components used in these amplifiers?
Good question! We typically use matched transistors for consistent performance. Who can share why that's important?
Because matched transistors ensure better gain stability, right?
Correct! It minimizes variations due to component differences. Let's move on to building our own BJT differential amplifier.
In summary, differential amplifiers amplify the difference between inputs while rejecting common signals, improving signal integrity.
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Now that we've built our amplifier, let's measure the differential gain. Who remembers how we can do that?
We apply a small differential input signal and measure the output, right?
Exactly! Using an oscilloscope, we can connect to the input and output to determine the gain. Remember the formula: A_d = V_out / V_in. If we have a 100 mV input and a 4.5 V output, what’s our gain?
That would be 45, right?
Exactly! Using the formula, you can see how the gain is derived. Don’t forget to observe the phase shift too. Can anyone tell me what we expect?
A phase shift of 180 degrees due to the inverting nature of the amplifier?
Well done! Summarizing today's session: we learned how to measure differential gain and the significance of phase relationships in amplifiers.
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Moving on, who can explain what common-mode gain tells us about our amplifier?
It shows how well the amplifier rejects common signals, right?
Correct! Ideally, we want A_cm to be as close to zero as possible. So, what do we include in our calculations for CMRR?
We need the ratios of A_d to A_cm.
Exactly! How about the significance of a high CMRR?
It indicates better noise rejection in our signals!
Exactly right! In summary, A_cm informs us about noise rejection capability of our amplifier, and CMRR quantifies that performance.
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Let’s transition to operational amplifiers. Who can explain what makes Op-Amps so widely used in electronics?
They have very high gain and input resistance!
Great point! Op-Amps typically consist of three stages: the differential input stage, intermediate gain stages, and the output stage. Can anyone elaborate on these?
The input stage is where the differential amplification happens, right?
Absolutely! It provides high input impedance. What about intermediate stages?
They add extra gain and help with voltage level shifting!
Exactly! And finally, what is the output stage designed to achieve?
To provide sufficient current to the load without distortion?
Correct! In conclusion, we discussed the structure of Op-Amps, emphasizing their staging for optimal function.
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Now it’s time to put our knowledge to the test! We’ll set up both inverting and non-inverting amplifiers. Who remembers the gain formula for the inverting configuration?
A_v is -R_f/R_in.
Right! And what about for the non-inverting amplifier?
It's 1 + R_1/R_2.
Perfect! As you assemble these configurations, pay attention to the output and how they compare. What should you expect for the phase in the inverting configuration?
A 180-degree phase shift!
Exactly! In summary, we reinforced our grasp on Op-Amps by building two different configurations and exploring their outputs.
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The procedure details systematic steps for designing, constructing, and testing both BJT differential amplifiers and basic operational amplifier configurations, including the measurement of differential and common-mode gains, CMRR, and bandwidth characteristics.
This section provides a comprehensive guide to performing Experiment No. 7 on the differential amplifier and basic operational amplifier gain stages. It lays out aims and objectives, emphasizing the analysis of both AC and DC characteristics of BJT differential amplifiers, focusing on key performance metrics such as differential gain (A_d), common-mode gain (A_cm), and the Common Mode Rejection Ratio (CMRR).
The procedure is segmented into four main parts: characterizing the BJT differential amplifier, determining the Input Common Mode Range (ICMR), characterizing basic gain stages of operational amplifiers—including inverting and non-inverting configurations—and discussing the internal stages of an Op-Amp.
In Part A, detailed steps are provided for constructing the BJT differential amplifier using a constant current source or resistor approximation, followed by measurements for differential and common-mode gains, leading to an understanding of CMRR. Part B focuses on measuring the ICMR, examining how the differential amplifier handles various input voltage ranges. Parts C and D involve the practical implementation of operational amplifiers and discussions about their internal structures, emphasizing the significance of operational amplifiers in various applications. This systematic approach reinforces theoretical knowledge through practical application, making it essential for students to grasp the functioning of these fundamental components in electronics.
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In this part, we focus on designing a BJT differential amplifier, which is a key component in many circuits. The first step is to set up a dual power supply that provides both positive and negative voltages. Next, we need to create a constant current source which can be done using either a large resistor connected to the negative supply (an approximation) or a dedicated BJT current source for better precision. Choosing suitable values for the collector resistors is essential for maintaining the transistors in their operational regions. After this, it's critical to match the transistors to ensure they perform identically, which can be done by measuring their beta values. Finally, we must calculate expected amplifier gains and record these values to compare later.
Think of the differential amplifier like a team of runners in a relay race, where each runner (transistor) needs to perform consistently for the team to succeed. The dual power supply is like the energy source for each runner, giving them the power they need. A strong teammate (the current source) allows the runners to work effectively together. Matching transistors is like having runners who can keep pace with each other, ensuring the team works most efficiently.
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In this stage, once we have prepped our components and calculations, it's time to physically build the BJT differential amplifier on a breadboard. This is where precision is crucial; if components are connected incorrectly, the circuit might not function as intended. Following the schematic from Figure 7.1 closely will help ensure that all connections are correct and the appropriate values for resistors and transistors are placed accordingly.
Building the circuit is like constructing a model with building blocks. Each component is a block, and if one is in the wrong spot or is the wrong type, the whole structure may not stand or work properly. Just as in model construction, following the plan closely ensures a successful and sturdy build.
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After the circuit is assembled, the next step is to power it up and measure the DC voltages at various points. This is crucial to ensure that the transistors are operating in their 'active region,' which is necessary for the differential amplifier to function correctly. We also check that the DC current source is providing the correct amount of current. By measuring the voltage across one of the collector resistors, we can calculate the collector current, which gives us valuable information about how the amplifier is behaving.
Think of this measurement as checking the fuel levels in a car before a trip. Just as a driver needs to ensure the fuel tank is full and the engine is running properly, we need to check that the amplifier is set up correctly and ready to operate as intended by verifying its voltage levels.
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In this measurement step, we are primarily focused on assessing how effectively the differential amplifier amplifies a small input signal. A sinusoidal input is applied to one transistor while the other is grounded. The oscilloscope will help visualize both the input signal and the output signal, allowing us to determine the differential gain (A_d). By comparing the output to the input signal, we can see how much the amplifier has increased the signal's strength. We should also pay attention to any phase shifts that occur between the input and output.
Measuring the differential gain is like observing how a microphone picks up sound and amplifies it for a speaker. The microphone takes in a soft voice (the input signal) and converts it into a much louder sound through the speaker (the output signal). Just as we’d want to know how well the microphone amplifies our voice, we measure how well the differential amplifier increases the strength of its input signal.
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This step is focused on estimating how the differential amplifier responds to common-mode signals, which is important for understanding its ability to reject noise. When the same signal is sent to both transistors, we check the output to see how much of that common signal gets amplified. The expectation is that the output should be very small if the amplifier is functioning correctly, indicating good common-mode rejection.
Expect this measurement to be like listening to a crowded room where someone tries to communicate with you. If multiple people are speaking at once (common-mode signals) but you only want to hear your friend (the differential signal), it’s crucial to discern that individual voice through the noise. Ideally, the amplification of the shared noise (A_cm) should be low, allowing your friend’s voice (A_d) to come through clearly.
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In this calculation step, we take the values of differential gain and common-mode gain we measured previously and calculate the Common Mode Rejection Ratio (CMRR). This is a critical parameter because it tells us how well the amplifier can reject unwanted signals that are common to both inputs compared to the signals we want to amplify. A higher CMRR indicates better performance. We also convert this ratio into decibels (dB) for easier interpretation.
Calculating the CMRR is similar to evaluating the performance of a filter in a sound system. If a filter effectively lets through the music (desired signal) but blocks out background noise (common-mode signals), it will have a high CMRR, making listening more enjoyable. A good CMRR in our differential amplifier means we can focus on the desired inputs while minimizing interference from noise.
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For this part, we want to determine how the differential amplifier behaves under varying common-mode voltage inputs. We connect the bases of both transistors and apply a DC voltage while also superimposing a small AC signal. The idea is to find the limits of the common-mode input voltage range where the amplifier can still operate linearly, meaning its output is not distorted or clipped. This gives insights into how the amplifier will behave in practical applications.
This stage can be compared to an artist testing the limits of their paintbrush on canvas. Just as the artist needs to know how much pressure to apply before the paint runs or loses its shape, we need to identify how much common-mode voltage we can apply before the amplifier starts to distort the output. Discovering these limits helps understand the practical application of the amplifier in real-world scenarios.
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Here, we actively test the differential amplifier by adjusting the common-mode voltage to see when the output signal remains clean and when it begins to distort. We identify the limits by gradually increasing the DC input voltage and observing changes in the output displayed on the oscilloscope. The lowest point where distortion begins indicates the lower limit of the Input Common Mode Range (ICMR), while the highest point before clipping indicates the upper limit.
This procedure is similar to tuning a radio. You can turn the dial and hear the music clearly until you reach a point where the signal distorts or cuts out entirely. The goal in both cases is to find the sweet spot where you receive the best sound quality—here, that relates to the ICMR limits of our amplifier circuit.
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In this part, we start setting up the operational amplifier for testing. Connecting it to the correct power supply is crucial as it ensures the Op-Amp has the necessary voltage levels to operate. The connections to pins are made following the manufacturer’s datasheet for the LM741 to guarantee proper functioning.
This stage is akin to plugging in electronic devices at home. Just like a lamp requires the right voltage to light up, the operational amplifier needs a proper power supply to function effectively. Paying close attention to power connections ensures that the device will operate as expected.
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Now, we proceed to build the inverting amplifier configuration. The design process involves selecting appropriate resistor values based on the desired voltage gain—the ratio of the feedback resistor to the input resistor. After constructing the circuit, we apply a small input signal and measure both the input and output to determine the actual gain and observe the phase relationship, which should indicate a 180-degree phase shift, typical for inverting amplifiers.
Designing the inverting amplifier can be compared to adjusting the settings on a camera lens. If you want a particular focus effect (gain), you adjust the lens (resistor values) to ensure it captures the scene well (amplifies the input). Taking pictures and reviewing them is like measuring output signals and validating the design.
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○ Bandwidth Measurement: Perform a frequency sweep (similar to Experiment 3, Part C). Keep V_in constant. Vary the frequency from mid-band (e.g., 1 kHz) upwards until the gain drops by 3 dB from the mid-band gain. This is your upper cutoff frequency (f_H). Since Op-Amp circuits typically have low-frequency gain maintained by coupling capacitors, f_L is usually very low. Calculate the bandwidth BW=f_H−f_L≈f_H. Record in Table 7.4.
In this step, we measure how the gain of the inverting amplifier changes as we adjust the frequency of the input signal. By identifying the frequency at which the gain decreases by 3 dB from its mid-band value, we can determine the upper cutoff frequency. This frequency is significant as it defines the operational limits of the amplifier in real applications. We can calculate the bandwidth based on this information.
Determining bandwidth is akin to checking the range of a walkie-talkie. Just as you can communicate effectively only within a certain distance, an amplifier effectively amplifies signals within a specific frequency range. Beyond that range, the clarity of the signal deteriorates—as evident in our measurements with increased frequencies.
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In the next step, we build the non-inverting amplifier circuit. The selection of resistor values is based on the desired gain, which, unlike the inverting amplifier, will not introduce a phase shift. We will apply an input signal, measure the input and the output, and ensure we calculate the gain accurately, while also confirming that the observed phase relationship reflects the expected outcome.
Constructing a non-inverting amplifier can be likened to directing a conversation where you encourage the other person’s ideas without interruptions. Here, the goal is to boost your voice (amplify the signal) without altering the essence of what is being said (maintaining the same phase). The purpose is to amplify without distortion, ensuring the message is retained.
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○ Bandwidth Measurement: Perform a frequency sweep similar to the inverting amplifier to find f_H. Calculate BW. Record in Table 7.4.
Just like we did with the inverting amplifier, we perform a frequency sweep with the non-inverting amplifier circuit. By determining the upper cutoff frequency at which the gain decreases significantly, we establish the operational bandwidth of this amplifier configuration.
This measurement mirrors tuning a radio to find the clearest signal. You adjust the frequency until you notice clarity starts to fade, indicating you're reaching the edges of its effective range. Similarly, in our measurement, we seek to identify the limits of the non-inverting amplifier's ability to amplify signals.
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In this discussion part, students are encouraged to reflect on what they have learned about the internal architecture of operational amplifiers. The Op-Amp’s three main stages play distinct yet crucial roles: the differential input stage amplifies signals while operating with high impedance, the intermediate stages add gain, and the output stage supports low output impedance for driving loads efficiently. Discerning these functions helps students understand how Op-Amps are designed to optimize performance in various applications.
This analysis can be compared to understanding the hierarchy in a well-functioning company. The executive team (differential input stage) sets the strategic goals while maintaining a broad oversight (high input impedance), the middle management (intermediate stages) implements plans to ensure smooth operations (generate high gain), and the frontline staff (output stage) delivers on those strategies with efficiency (low output resistance). Each layer works in unison to ensure the success of the organization.
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Key Concepts
Differential Amplifier: Amplifies the difference between input signals.
Common-Mode Gain: Measures how an amplifier responds to the same signal on both inputs.
CMRR: Critical for assessing the performance of amplifiers in noisy environments.
Operational Amplifier: Versatile building blocks in analog circuits, fundamentally designed to amplify electrical signals.
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Example of calculating A_d: If we apply 100 mV yielded an output of 4.5 V, then A_d = 4.5 V / 0.1 V = 45.
Example of CMRR: If A_d is measured as 100 and A_cm as 0.1, then CMRR = 1000, indicating excellent common-mode rejection.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
To amplify the difference, that is the aim, the differential amplifier is its name!
Imagine a speaker at an event. The speaker is the differential amplifier, booming with the voice difference between 2 microphones while ignoring crowd noise, representing common-mode signals.
D for Differential means Difference; C for Common-mode means Common signals.
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Review the Definitions for terms.
Term: Differential Amplifier
Definition:
An amplifier that amplifies the difference between two input signals and rejects their common components.
Term: CommonMode Gain (A_cm)
Definition:
The gain of an amplifier when the same input signal is applied to both inputs.
Term: Differential Gain (A_d)
Definition:
The gain of the differential amplifier when differential input is applied, calculated as the output voltage divided by the differential input voltage.
Term: Common Mode Rejection Ratio (CMRR)
Definition:
A measure of an amplifier's ability to reject common-mode signals relative to the differential signals it amplifies.
Term: Input Common Mode Range (ICMR)
Definition:
The range of common-mode voltage inputs over which the differential amplifier operates linearly.
Term: Operational Amplifier (OpAmp)
Definition:
A high-gain voltage amplifier with differential inputs, characterized by high input impedance and low output impedance.
Term: Transconductance (g_m)
Definition:
A parameter that indicates the change in output current per change in input voltage; crucial for calculating differential gain.
Term: GainBandwidth Product (GBW)
Definition:
A constant that represents the product of an amplifier’s gain and bandwidth.