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Today, we're going to explore how to measure the voltage gain of our BJT amplifier. Can anyone tell me what voltage gain represents in terms of an amplifier's performance?
I think it’s how much the amplifier increases the voltage of the signal.
Exactly! We measure voltage gain (A_v) as the ratio of output voltage to input voltage. Typically, we can express it in decibels too. Does anyone recall the formula for converting this ratio into decibels?
Is it 20 times the log of the output voltage over the input voltage?
That's right, Student_2! So, when we set our function generator to send a small AC signal into the BJT, we will measure the V_in and V_out using an oscilloscope. What do you think we should expect to observe in our measurements?
A phase inversion because of the common-emitter configuration!
Exactly! Great observation, Student_3. Let's keep that in mind as we go through our measurements today.
To sum up, we'll measure V_in and V_out, calculate the voltage gain using the formula for decibels, and it’s important to note the phase behavior. Understanding these concepts is key to analyzing amplifier performance.
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We discussed voltage gain, but how do we determine the input and output resistances of our BJT? What do you think they represent in our circuit?
Input resistance is how much the amplifier resists the incoming signal, right? And output resistance is about how much load it can handle?
That's correct, Student_4. The input resistance affects how the amplifier interacts with the preceding stage, while output resistance impacts its ability to drive the following stage. So, how do we measure these resistances practically?
For input resistance, we could use the source resistance method and adjust until we achieve half the input voltage.
Exactly! You apply a known resistance in series with the input and observe the drop until it halves the voltage. And what about output resistance?
We would remove the load, measure the open-circuit voltage, then connect different loads until the output voltage drops by half.
Perfect, Student_2. This hands-on approach enhances your understanding of how the amplifier interacts with other components in a circuit.
Remember, knowing these resistances is crucial for designing effective circuits and ensures we can predict how our amplifier will function in practical applications.
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Next, let’s turn our attention to frequency response. Why do you think it's important for us to understand the frequency response of our amplifier?
It tells us how the amplifier performs at different frequencies, not just the mid-band.
Absolutely! An amplifier doesn't amplify all frequencies equally. We observe roll-off at low and high frequencies due to coupling and bypass capacitors and internal transistors' capacitance. What are the two cutoff frequencies we often look for?
The lower cutoff frequency, f_L, and the upper cutoff frequency, f_H.
Precisely! And the bandwidth? How do we calculate that?
Bandwidth is f_H minus f_L, right?
Correct! Understanding bandwidth is crucial as it informs us how versatile our amplifier is with respect to different signal types or applications.
In summary, frequency response lets us evaluate the amplifier's performance across a range of frequencies, helping to design for specific needs.
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In this section, students learn to measure and analyze the mid-band performance of a common-emitter BJT amplifier. It covers the theoretical calculations for voltage gain, input resistance, and output resistance, as well as the practical measurement techniques and the interpretation of results.
In this section, we delve into the mid-band performance of a common-emitter Bipolar Junction Transistor (BJT) amplifier. Specifically, we outline key parameters: voltage gain (A_v), input resistance (R_in), and output resistance (R_out). These measurements are pivotal in evaluating an amplifier's capability to effectively transfer AC signals.
The section includes practical exercises and procedures for obtaining these measurements and emphasizes the importance of frequency response in amplifier performance assessment. All measurements culminate in a comprehensive understanding of the amplifier's operational effectiveness within its specified mid-band range.
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The AC emitter resistance (r_e′) represents the dynamic resistance of the forward-biased base-emitter junction. It's crucial for gain calculations. r_e′=V_T/I_E Where V_T is the thermal voltage (V_T≈26 mV at room temperature, 300K), and I_E is the quiescent (DC) emitter current.
In a BJT amplifier, the AC emitter resistance (r_e′) is calculated by determining the thermal voltage (about 26 mV) and dividing it by the emitter current (I_E). This small-signal resistance is vital as it influences the amplifier's voltage gain. The signal input causes small variations in current and voltage in the circuit, and understanding how the emitter resistance interacts with these fluctuations helps in designing efficient amplifiers.
Think of r_e′ as the responsiveness of a car suspension system. Just like how a good suspension dampens bumps and allows smooth riding, a well-calibrated emitter resistance helps the amplifier respond accurately to input signals without distortion.
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For a common-emitter amplifier with an emitter bypass capacitor (C_E effectively shorts R_E for AC), the mid-band voltage gain is: A_v=–R_C ∣∣R_L/r_e′ Where: R_C: Collector resistor. R_L: External AC load resistance connected at the output. If no external load is connected, R_L=infinity, so R_C ∣∣infinity=R_C. The negative sign indicates a 180-degree phase shift between the input and output voltage signals.
To determine the mid-band voltage gain (A_v) of a common-emitter amplifier, you use the formula A_v = - (R_C || R_L) / r_e′. In this formula, R_C is the collector resistor, and R_L is the resistance of any connected load. If there is no external load, the load resistance is infinite, and the gain simplifies to just R_C divided by r_e′. The negative sign shows that the output signal is inverted relative to the input, typical of a common-emitter configuration.
Imagine you're tuning a radio. The signal strength (or gain) you hear is influenced by both the radio station's broadcast strength (R_C) and your antenna's quality (R_L). Just as a weak signal would lead to poor sound, a larger r_e′ will reduce your amplifier's gain, making it less effective in amplifying audio.
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Input Resistance (R_in): This is the equivalent resistance seen by the AC signal source looking into the amplifier's input terminals. R_in=R_B ∣∣(beta_ac r_e′) Where: R_B=R_1 ∣∣R_2=R_1×R_2/(R_1+R_2) (the parallel combination of the base biasing resistors). beta_ac: The AC current gain of the transistor (also often denoted as h_fe). For most practical purposes, beta_ac≈beta_DC.
The input resistance (R_in) reflects how much resistance the input signal encounters as it enters the amplifier. It's calculated by combining the resistor values (R_1 and R_2) in a parallel configuration, then combining this with the product of the transistor's current gain (beta_ac) and the AC emitter resistance (r_e′). This measurement is crucial because a higher input resistance leads to less loading on the previous signal source, thus helping maintain signal integrity.
Think of R_in as a toll booth on a highway. If the toll is high (high resistance), fewer cars (signals) will enter, while a lower toll facilitates easier access, allowing more traffic. In an audio amplifier, having a low input resistance would discourage the microphone (source) from sending signals effectively.
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Output Resistance (R_out): This is the equivalent resistance seen by the load looking back into the amplifier's output terminals. R_out=R_C (assuming the transistor's intrinsic output resistance, r_o, is much larger than R_C, which is a common approximation for CE amplifiers).
The output resistance (R_out) indicates how much resistance the amplifier presents to a loaded output. In a common-emitter amplifier, it is primarily determined by the collector resistor (R_C). This means that the amplifier can drive various loads effectively, assuming R_C is substantially smaller than any intrinsic transistor output resistance. This property affects how well the amplifier can transfer power to its output load, which is critical in practical applications.
Imagine an electric kettle connected to a power outlet. The outlet imposes certain resistance based on how much current it can draw. If the kettle has a low output resistance, it draws sufficient power to heat the water quickly. In a similar fashion, a low output resistance in an amplifier allows it to drive the connected speakers or loads effectively.
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An amplifier does not amplify all frequencies equally. Its gain typically remains constant over a range of frequencies (the mid-band) and then decreases at very low and very high frequencies.
The frequency response of the amplifier describes how the gain varies across different frequencies. Within the mid-band, the amplifier performs optimally, providing a steady gain. However, as you move towards lower or higher frequencies, the gain starts to decrease, often leading to a graph that shows a flat area (mid-band) and declining edges (low and high frequencies). Understanding this aspect helps in applications where specific frequencies are critical, such as audio amplification.
Imagine a concert speaker system. It’s designed to handle a specific range of sounds (mid frequencies) effectively while muffling sounds that are very low (bass) or too high (treble). Just like an amplifier that performs well across a specific frequency range, a good speaker setup limits output to ensure clear sound quality.
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Cutoff Frequencies are the frequencies at which the amplifier's gain drops to 0.707 times (or 1/sqrt(2)) of its maximum mid-band gain. In decibels, this corresponds to a 3 dB drop from the mid-band gain. Bandwidth (BW): The range of frequencies over which the amplifier's gain is at least 3 dB below its mid-band maximum. BW=f_H−f_L.
Cutoff frequencies define the limits of effective amplification for a given amplifier. The lower cutoff frequency (f_L) is where the gain begins to decrease and the upper cutoff frequency (f_H) shows where it ends. The bandwidth is calculated by subtracting the lower cutoff from the upper cutoff frequency, providing a measurement of how broad a range of signals the amplifier can handle without significant loss of power. This information is key for engineers when selecting components for various signal processing applications.
Consider a water pipe that can only allow a certain flow rate of water through it. If the flow is either too fast or too slow (representing low and high frequencies), the water level varies significantly. In amplification terms, bandwidth indicates how well the amplifier can maintain a stable gain over a range of frequencies, similar to how a pipe maintains steady water flow within certain limits.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Voltage Gain: The measure of how much an amplifier increases the voltage level of its input signal.
Input Resistance: An important parameter that affects how the amplifier interacts with previous circuit stages.
Output Resistance: Reflects the capacity of the amplifier to drive external loads.
See how the concepts apply in real-world scenarios to understand their practical implications.
Example of calculating voltage gain: If V_out is 4V and V_in is 0.1V, then A_v = V_out / V_in = 40 or 32 dB.
If the input resistance measured when using a known resistor is found to be 2kΩ, this indicates the amplifier will work effectively with sources having a higher impedance.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
To gain more voltage, rely on the fate, A_v will tell you, it's never too late.
Imagine an amplifier as a bus. Input resistance is the entrance fee, while output resistance is how much weight it can carry. The bus travels a bandwidth route, not making stops at just any station but only at special cutoff points.
Remember 'GIP' for Gain, Input resistance, and Performance which covers major amplifier assessments.
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Review the Definitions for terms.
Term: AC Voltage Gain (A_v)
Definition:
The ratio of the output voltage to the input voltage in an amplifier, often expressed in decibels.
Term: Input Resistance (R_in)
Definition:
The resistance seen by the AC signal source at the input terminals of the amplifier.
Term: Output Resistance (R_out)
Definition:
The resistance seen by the load connected to the output terminals of the amplifier.
Term: Frequency Response
Definition:
The characteristic of an amplifier that defines how its gain changes with varying frequencies.
Term: Cutoff Frequencies
Definition:
The frequency points where the amplifier's gain drops to 0.707 times its maximum value.