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Today, we'll discuss the common emitter amplifier. Can anyone share what they know about its basic characteristics?
I think it's used in amplification circuits and often has a phase inversion?
Exactly! The CE amplifier indeed provides a significant voltage gain and exhibits a 180-degree phase shift between input and output. Let's remember this with the mnemonic 'Phase Shift: CE's Gift!'
What is the input and output configuration like?
Good question! In the CE configuration, the input is applied to the base, and the output is taken from the collector.
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Now, let's transform our CE amplifier into its AC equivalent. What happens to the DC sources?
They are replaced by shorts and opens?
Perfect! This helps us analyze small AC signals effectively. Can anyone tell me what happens to the capacitors in low frequency?
They are viewed as shorts too, right?
Exactly! This simplification allows AC signals to pass through. Remember the acronym 'CAPS' - Capacitors Are Pass-through Shorts at low frequencies!
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Let's derive the key performance parameters like voltage gain. What does the formula for voltage gain look like?
It's A_v = -g_m(R_C || r_o)! But why do we use a negative sign?
Great observation! The negative sign indicates the phase inversion. Let’s memorize 'GAINS' - Gain Always Inverts the Negative Signal!
Can we calculate the input resistance too?
Yes! The input resistance is R_B || r_pi. It's essential to understand how these components affect impedance.
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Let's apply what we've learned. Given R_C = 4.7 kΩ and g_m = 40 mS, how would we find the voltage gain?
We'd calculate A_v = -g_m * R_C?
Correct! And if we assume r_o is large enough to ignore, we’d simply multiply to find the gain. Always remember to put the sign to show inversion!
What about the input resistance?
It would be calculated by R_B || r_pi. All these components together determine the overall performance of the amplifier.
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In this section, we explore the common emitter (CE) BJT amplifier configuration, which is known for its high voltage gain, input, and output resistance characteristics. We analyze the AC equivalent circuit, derive key parameters such as voltage gain, input resistance, and output resistance, and illustrate with numerical examples.
The common emitter (CE) configuration is a fundamental and widely used amplifier circuit in electronics, primarily involving a Bipolar Junction Transistor (BJT). This section outlines the key characteristics and performance metrics associated with CE amplifiers. Key Characteristics include:
To analyze the CE amplifier's performance, we utilize the AC equivalent circuit where:
- DC sources are replaced by their AC equivalents (shorts for DC voltage sources and opens for DC current sources).
- Transistors are substituted with their small-signal models (such as the π-model).
\[ A_v = -g_m (R_C || r_o) \]
The negative sign indicates phase inversion, and the gain is highly dependent on load conditions.
\[ R_{in} = R_B || r_{ ext{pi}} \]
\[ R_{out} = R_C || r_o \]
A numerical example provided estimates voltage gain, input resistance, and output resistance for a CE amplifier using typical values for BJT parameters. Calculations demonstrate the influence of these components on the overall performance of the amplifier.
This section is instrumental for understanding how to effectively implement and analyze common emitter amplifiers in electronic circuit design.
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Configuration Characteristics:
The Common Emitter (CE) configuration of a BJT amplifier is defined by how the input and output voltages are connected. The input signal is applied to the transistor's base, while the output is taken from the collector. The emitter terminal is often grounded for AC signals, sometimes with the help of a large bypass capacitor that allows AC signals to pass while blocking DC. A notable feature of the CE amplifier is its inverting property; the output voltage is 180 degrees out of phase with the input voltage. This configuration is well-known for its capability to deliver high voltage gains, making it a popular choice in amplification needs. While it has a moderate input resistance and output resistance, it provides a significant advantage in amplifying small signals.
Imagine a microphone connected to a speaker through a common emitter amplifier. The sound waves (input) produced by the microphone are amplified, but the amplified sound comes out of the speaker in reverse phase (inverting). You can think of it as a speaker ‘echoing back’ your voice, but it may sound flipped in tone. This makes the CE amplifier useful in audio applications, where transforming low sounds into louder ones is necessary.
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AC Equivalent Circuit (Simplified, assuming r_o is infinite and no R_E or bypassed):
Input side: v_in connected to base, R_B (parallel combination of bias resistors) connected to base, r_pi between base and emitter (ground). Output side: Collector connected to R_C (load resistor) and g_mv_be current source. Emitter is AC ground.
In analyzing a CE amplifier, we can create an AC equivalent circuit to simplify our calculations. Here, we assume that the output resistance, r_o, is infinite, which means we can ignore it for the purposes of this model. In the AC equivalent, the input signal (v_in) is applied to the base of the transistor. The resistors used for biasing are connected parallel to each other, acting together as R_B, and we also have r_pi, which represents the input resistance between the base and emitter. On the output side, the collector is connected to a load resistor (R_C), which helps determine how much voltage can be delivered to the load. This simplification allows us to analyze how the amplifier affects the input signal, leading to a clearer understanding of its performance.
Think of the AC equivalent circuit like a team of players working together to achieve a goal. In our case, v_in is like a player who makes a play on the field (input). R_B, made up of parallel biasing resistors, are like teammates who support our main player. r_pi is the connection that channels the play effectively towards R_C, which represents the goal of scoring (output). This setup helps visualize how teamwork (every element) helps to successfully amplify a signal.
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Derivations using π-model, assuming bypassed R_E if present, and r_o typically much larger than R_C:
When deriving the key parameters of the CE amplifier, we start with the voltage gain (A_v), which is determined by how the input voltage at the base (v_in) translates to the output voltage (v_out). Because the transistor amplifies current, the gain also depends on the current flowing through a dependent current source, which is controlled by g_m, a measure of transconductance. The output voltage across the load resistor R_C is given by the product of the gain and the current through R_C. It's important to note that the negative sign in the voltage gain indicates that the output signal is inverted relative to the input, which is a characteristic of the CE amplifier.
Consider a water hose connected to a garden spray nozzle. The water pressure going into the hose (input voltage) is transformed through the nozzle's design (the amplifier) into a strong, directed spray of water (output voltage). If you apply a small amount of water pressure, you will get a stronger spray of water out the nozzle (high gain), but notice that the spray shoots out in the opposite direction to where the pressure is applied—this reflects the inverting nature of the CE amplifier.
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The input resistance (R_in) and output resistance (R_out) play crucial roles in how the CE amplifier interacts with other components in the circuit. To calculate R_in, we look into the base and consider the input resistance, r_pi, which is affected by any biasing resistors connected to the base. This combination works together to determine how much current can flow into the circuit before impacting the signal. For R_out, when we analyze the output, we set the input to zero to evaluate the resistance looking into the collector terminal. The output resistance includes the load resistor R_C and is affected by the output resistance of the transistor, r_o, which, for simpler calculations, is thought of as infinite. Understanding both resistances is key to designing effective amplifier circuits.
Imagine plugging your electronic device (input) into a power outlet. The outlet's resistance represents the input tendency of the device to consume power (R_in), while the power supply itself works harder (output resistance, R_out) to maintain voltage. The better the outlet can supply current without dropping voltage (i.e., low resistance), the more efficiently the device runs. Similarly, an amplifier's resistances shape how well it can receive signals and deliver them to the next stage.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Common Emitter (CE) Configuration: A configuration where the common emitter transistor provides significant voltage amplification.
Input/Output Characteristics: The input is at the base, output is at the collector, and the signal is inverted.
Small-Signal Analysis: Simplifies complex transistor behavior for AC signal analysis.
Voltage Gain Calculation: Describes how to calculate the voltage gain using specific parameters.
Input/Output Resistances: Essential for understanding how the amplifier interacts with other stages.
See how the concepts apply in real-world scenarios to understand their practical implications.
Consider a CE amplifier with R_C = 4.7 kΩ and g_m = 40 mS. This setup can yield a voltage gain of approximately -188.
If the input resistance looking into the base is R_B = 50 kΩ and r_pi = 2.5 kΩ, the overall resistance would be calculated as R_{in} = 50 kΩ || 2.5 kΩ.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
In the common emitter, signals are gay, phase is inverted, loud and sway.
Imagine a puppet show where every command given from the front is echoed back upside down; that’s how CE amplifiers work, inverting the signal while amplifying it!
Use 'CRISP' to remember Common Emitter: Common, Resistance, Invert, Signal, Performance.
Review key concepts with flashcards.
Review the Definitions for terms.
Term: Voltage Gain (A_v)
Definition:
The ratio of the output AC voltage to the input AC voltage in an amplifier.
Term: Input Resistance (R_in)
Definition:
The equivalent resistance seen by the input signal source when looking into the amplifier's input terminals.
Term: Output Resistance (R_out)
Definition:
The equivalent resistance seen by the load looking back into the amplifier's output terminals.
Term: SmallSignal Model
Definition:
A linearized representation of a non-linear device at small AC signal variations around a DC operating point.
Term: Phase Inversion
Definition:
A phenomenon where the output signal is 180 degrees out of phase with the input signal.
Term: BJT
Definition:
Bipolar Junction Transistor, a type of transistor that relies on the movement of charge carriers.