Part B: Ac Mid-band Analysis (gain And Impedances) (6.2) - SINGLE-STAGE BJT AMPLIFIER CHARACTERIZATION
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Part B: AC Mid-Band Analysis (Gain and Impedances)

Part B: AC Mid-Band Analysis (Gain and Impedances)

Practice

Interactive Audio Lesson

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Introduction to Mid-Band Voltage Gain

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Teacher
Teacher Instructor

Today, we're delving into mid-band voltage gain for our BJT amplifier. Who can explain what voltage gain is?

Student 1
Student 1

Isn't it the ratio of output voltage to input voltage?

Teacher
Teacher Instructor

Exactly! It tells us how much we can amplify our signal. It's expressed as A_v = V_out/V_in. Can anyone tell me how we might express it in decibels?

Student 2
Student 2

I think it's A_v(dB) = 20 log_10(|A_v|)?

Teacher
Teacher Instructor

Perfect! This logarithmic scale makes it easier to work with large ranges of gain. Now, can someone summarize the significance of mid-band voltage gain in amplifiers?

Student 3
Student 3

It helps us understand how well the amplifier will perform within a specific frequency range.

Teacher
Teacher Instructor

Great summary! Remember, maintaining a stable A_v in the mid-band is crucial for good performance.

Measuring Input and Output Resistance

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Teacher
Teacher Instructor

Next, let's discuss input and output resistance. Why do you think measuring these resistances is critical?

Student 4
Student 4

Because it affects how the amplifier interacts with other circuit components, right?

Teacher
Teacher Instructor

Exactly! R_in determines the loading effect on the previous stage, while R_out affects the next stage. Who remembers how we measure R_in?

Student 1
Student 1

We use a variable resistor in series to drop the voltage and find the input resistance?

Teacher
Teacher Instructor

Right! And what about R_out? How can we measure that?

Student 2
Student 2

By measuring the output voltage drop across a known load resistance?

Teacher
Teacher Instructor

Exactly, great job! Understanding these resistances allows us to predict circuit behavior.

Frequency Response and Bandwidth

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Teacher
Teacher Instructor

Now, let’s talk about frequency response. What happens to gain at low and high frequencies?

Student 3
Student 3

It tends to roll off due to capacitive effects, right?

Teacher
Teacher Instructor

Correct! At low frequencies, coupling capacitors block signal passage, while at high frequencies, internal capacitances can short circuit the input signal. How do we identify the bandwidth?

Student 4
Student 4

By finding the -3 dB cutoff frequencies!

Teacher
Teacher Instructor

Exactly! The -3 dB point indicates where the gain drops significantly. Who can summarize how bandwidth relates to an amplifier's performance?

Student 1
Student 1

A wider bandwidth means that the amplifier can handle a larger range of frequencies without a significant drop in gain.

Teacher
Teacher Instructor

Excellent summary! Bandwidth is crucial for the functionality of amplifiers in various applications.

Role of Coupling and Bypass Capacitors

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Teacher
Teacher Instructor

Let's explore the role of coupling and bypass capacitors in our amplifier. How do they affect the frequency response?

Student 2
Student 2

Coupling capacitors block DC and allow AC signals, which can determine cutoff frequencies.

Teacher
Teacher Instructor

Correct! And what about bypass capacitors?

Student 3
Student 3

They help stabilize the gain by providing a low-resistance path for AC signals to ground.

Teacher
Teacher Instructor

Exactly! What happens to gain if we remove the bypass capacitor?

Student 4
Student 4

The gain would decrease because AC signals can't bypass the emitter resistor effectively.

Teacher
Teacher Instructor

Great insights! Remember that the type and value of capacitors can significantly impact amplifier performance.

Recap and Application of Concepts

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Teacher
Teacher Instructor

Let's recap what we learned about the mid-band analysis of our BJT amplifier. What are the main components we focused on?

Student 1
Student 1

Mid-band voltage gain, input resistance, output resistance, and frequency response.

Teacher
Teacher Instructor

Exactly! Can anyone explain why understanding these parameters is crucial for circuit design?

Student 2
Student 2

Because they determine how well the amplifier will integrate with other components and perform the desired function.

Teacher
Teacher Instructor

Right! How can you apply these concepts in real-world design?

Student 3
Student 3

By selecting the right components and ensuring compatibility between stages.

Teacher
Teacher Instructor

Well said! Remember, solidifying these concepts will aid in more advanced electronic design.

Introduction & Overview

Read summaries of the section's main ideas at different levels of detail.

Quick Overview

This section focuses on the analysis of gain and impedances in a common-emitter BJT amplifier during mid-band operation.

Standard

In this section, students learn about experimental techniques to determine mid-band voltage gain, input and output resistance of a common-emitter BJT amplifier. It emphasizes theoretical calculations and practical measurements at mid-band frequencies, offering insights into the impact of frequency response on amplifier performance.

Detailed

In this section, we explore the AC mid-band analysis of a common-emitter Bipolar Junction Transistor (BJT) amplifier, focusing on gain and impedances. The core objectives include measuring mid-band voltage gain (A_v), input resistance (R_in), and output resistance (R_out). Students will engage in hands-on experimentation, utilizing techniques for determining these parameters, and deepen their understanding of how the amplifier performs with small AC signals. Theoretical calculations are combined with practical measurements to enhance comprehension of gain representation in decibels and the significance of frequency response, particularly the bandwidth defined by cutoff frequencies (f_L and f_H). Observational exercises reinforce the impact of capacitors on frequency response, culminating in a comprehensive understanding of AC analysis in electronic circuits.

Audio Book

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Complete Circuit Assembly

Chapter 1 of 5

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Chapter Content

With the DC power supply OFF, integrate the AC input coupling capacitor (C_C1), the output coupling capacitor (C_C2), the emitter bypass capacitor (C_E), and the load resistor (R_L, e.g., 10 kΞ© or 15 kΞ©) into your breadboard circuit as shown in Figure 3.1. Ensure all capacitor polarities are correct.

Detailed Explanation

Before starting the AC analysis, ensure you have assembled the entire circuit, including the necessary capacitors and load resistor. The AC coupling capacitors (C_C1 and C_C2) allow AC signals to pass while blocking DC, which protects the transistor from unwanted shifts in its operating point. The bypass capacitor (C_E) significantly affects gain at mid-band frequencies, helping provide a stable AC signal. Make sure to double-check all polarities as incorrect connections may damage the components or lead to incorrect measurements.

Examples & Analogies

Think of capacitors in your circuit as gates that control what kind of signals can pass through. Imagine a party where some guests can only enter if they meet certain criteria - for instance, they need to have an RSVP (like AC signals) while others (DC signals) are not allowed in at all. If the gates (capacitors) are not set correctly, then the wrong guests (signals) could disrupt the event (circuit operation).

Theoretical Mid-Band Parameter Calculation

Chapter 2 of 5

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Chapter Content

Based on your measured I_E (from Part A.3), calculate the experimental r_eβ€² using r_eβ€²=V_T/I_E (where V_Tapprox26textmV). Using this r_eβ€² and your assumed beta_ac (e.g., 150), calculate the theoretical mid-band voltage gain (A_v), input resistance (R_in), and output resistance (R_out) using the formulas provided in Section 4.3.

Detailed Explanation

First, calculate the emitter dynamic resistance (r_eβ€²) using the thermal voltage (V_T, approximately 26 mV) divided by the measured emitter current (I_E). After obtaining r_eβ€², you can proceed to calculate the theoretical mid-band voltage gain (A_v) using the formula that incorporates the collector resistor (R_C) and load resistance (R_L). You also need to determine the input resistance (R_in) using the values for base biasing resistors and the dynamic resistance. Finally, ensure that the output resistance (R_out) is recorded, which is often taken to be equal to R_C in these analyses.

Examples & Analogies

Think of calculating these parameters like adjusting the settings on a musical equalizer. The A_v is like finding the right balance of sound at mid frequencies; R_in determines how well your amplifier can pick up signals without being overloaded, and R_out affects how well it can drive a speaker. Each value impacts the overall sound quality, similar to how these resistances impact the performance of your amplifier.

Mid-Band Voltage Gain (A_v) Measurement

Chapter 3 of 5

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Chapter Content

Power on the DC supply (V_CC). Connect the AC Function Generator to the input of the amplifier (before C_C1, or between C_C1 and the base) and set it to produce a sinusoidal waveform with a small peak-to-peak amplitude (e.g., 20-50 mV p-p). Set the frequency to a mid-band value (e.g., 5 kHz or 10 kHz). Choose a frequency where the gain is relatively stable (not affected by coupling/bypass caps or parasitic caps). Connect Channel 1 of the Oscilloscope to the actual amplifier input (i.e., at the base of the BJT, after C_C1) to measure V_in(pβˆ’p). Connect Channel 2 of the Oscilloscope to the output of the amplifier (across the load resistor R_L) to measure V_out(pβˆ’p). Ensure both oscilloscope channels are set to AC coupling for accurate AC signal measurement. Adjust the Volts/Div and Time/Div settings for clear waveform visualization. Measure the peak-to-peak input voltage (V_in(pβˆ’p)) and the peak-to-peak output voltage (V_out(pβˆ’p)). Calculate the experimental mid-band voltage gain: A_v=fracV_out(pβˆ’p)V_in(pβˆ’p). Observe and note the phase relationship between the input and output waveforms (a 180-degree phase shift is expected for CE). Record the measured A_v in Observation Table 7.3. Convert it to dB: A_v(dB)=20log_10(∣A_v∣).

Detailed Explanation

By powering the circuit and applying the AC input signal, we can measure both the input and output voltages using an oscilloscope. The measurement process involves setting the function generator to a specific amplitude and frequency, then connecting to the input and output points of the amplifier. The experimental gain (A_v) is found by taking the output voltage and dividing it by the input voltage, showing how much the amplifier has boosted the signal. Be attentive to the phase relationship; in a common-emitter setup, the output should ideally show a phase inversion of 180 degrees compared to the input.

Examples & Analogies

Picture a person yelling (input voltage) into a microphone (the amplifier). The microphone captures the sound and sends it to a speaker (the output). The speaker plays the sound at a louder volume (the amplified output). Just like you’d want to check that the sound is not only louder but also sounds correct and clear, in the circuit, we confirm that the voltage is not only boosted but also in the correct phase.

Input Resistance (R_in) Measurement (Source Resistance Method)

Chapter 4 of 5

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Chapter Content

Ensure the Function Generator is connected to the amplifier input through C_C1. Connect a known variable resistor (or a decade resistance box) R_S in series with the function generator output and the amplifier input (i.e., between the Function Generator and C_C1). Initially set R_S=0Ξ©. Apply a mid-band AC input signal with a convenient amplitude. Measure the input voltage at the base of the BJT (V_in) using the oscilloscope when R_S=0. Record this as V_in(0). Now, increase the value of R_S until the input voltage at the base (V_in) drops to exactly half of V_in(0). At this point, the value of the series resistor R_S is equal to the input resistance of the amplifier: R_in=R_S. Alternatively, measure V_in (at base) with R_S=0 (V_in0) and then with R_S=R_Sβ€² (a known value) (V_inβ€²). Then calculate R_in=R_Sβ€²left(fracV_in0V_inβ€²βˆ’1right). Record the measured R_in in Observation Table 7.3. Compare it to your theoretical calculation.

Detailed Explanation

To find the input resistance, we apply a known resistor in series with the input signal. By adjusting this resistor until the input voltage at the amplifier's base is halved compared to no additional resistor, we can directly measure the input resistance. This method leverages the relationship between voltage drop across the resistors and allows for an accurate determination of the input impedance of the amplifier.

Examples & Analogies

Imagine trying to push an object across a surface – if you apply a force (like voltage) without any resistance (like R_S), it moves easily. But if you introduce a heavier object (the resistor), you notice that less of the initial force translates into movement (voltage drop). In the same way, the input resistance contrasts the ability of the amplifier to receive signals based on how much 'push' the input voltage can provide against the effective 'weight' of the connected circuitry.

Output Resistance (R_out) Measurement (Load Resistance Method)

Chapter 5 of 5

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Chapter Content

Remove any external load resistor R_L connected to the amplifier output (if present, measure V_out right after C_C2). This is your open-circuit output voltage (V_out(OC)). Now, connect a known variable load resistor (R_Lβ€², e.g., a potentiometer or decade box) at the output (across the output terminals, after C_C2 and parallel to the internal output resistance). Apply a mid-band input signal. Adjust R_Lβ€² until the output voltage (V_out) drops to half of the previously measured V_out(OC). At this point, the value of R_Lβ€² is equal to the output resistance of the amplifier: R_out=R_Lβ€². Record the measured R_out in Observation Table 7.3. Compare it to your theoretical calculation.

Detailed Explanation

To measure the output resistance, we first take the open-circuit output voltage (no load connected) before adding a known load resistor. By adjusting the value of the load resistor until the output voltage drops to half of its original value, we can establish the output resistance. This drop in output voltage gives us insight into how the amplifier behaves under load, which is critical for understanding its performance in practical applications.

Examples & Analogies

Think about a water hose connected to a nozzle (the amplifier output). If the nozzle is blocked (open circuit), water flows freely (V_out(OC)). However, when you attach a nozzle that restricts water flow (load connected), the spray becomes weaker (V_out decreases). The amount of water flow reduction tells you how strong the nozzle was and, consequently, how much the system can cope with the constraints of load.

Key Concepts

  • Voltage Gain: Ratio between output and input voltages.

  • Input Resistance: Resistance seen by the input AC signal.

  • Output Resistance: Resistance seen at the amplifier's output.

  • Cutoff Frequencies: Frequencies at which the amplifier's gain drops significantly.

  • Frequency Response: How amplifier gain varies with frequency.

Examples & Applications

Example 1: If an amplifier has an input signal of 0.1V and an output signal of 1V, the voltage gain (A_v) is 10.

Example 2: A BJT amplifier with a R_in of 10kΞ© and R_out of 2kΞ© will affect how it interfaces in a larger circuit.

Memory Aids

Interactive tools to help you remember key concepts

🎡

Rhymes

Gain is the name of the game; V_out over V_in is how we claim.

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Stories

Imagine an amplifier as a superhero, taking a tiny signal and making it huge, soaring from input to output, dodging low and high frequency traps.

🧠

Memory Tools

Gain and Impedance: G.I. - Gain = Output/Input; I = Input Res + Output Res.

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Acronyms

BAND - Bandwidth Analysis Needs Determining.

Flash Cards

Glossary

Voltage Gain (A_v)

The ratio of output voltage (V_out) to input voltage (V_in), indicating how much an amplifier increases the voltage of a signal.

MidBand

The frequency range over which an amplifier performs with stable gain without significant attenuation.

Input Resistance (R_in)

The resistance seen by the AC signal source looking into the input terminals of the amplifier.

Output Resistance (R_out)

The resistance seen by the load looking back into the output terminals of the amplifier.

Cutoff Frequencies

The frequencies at which the gain of the amplifier drops to a certain level (usually -3 dB) from the peak value.

Reference links

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