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Today we will start by understanding differential amplifiers, which are crucial in many analog applications. Can anyone tell me what a differential amplifier does?
It amplifies the difference between two input signals!
Exactly! We denote the difference as V_id. Now, what happens to signals that are common to both inputs?
Those common signals get rejected, right?
Correct! This capability is measured by the Common Mode Rejection Ratio, or CMRR. Can anyone explain the significance of a high CMRR?
A high CMRR means better noise rejection, which is really important in clean signal processing!
Well done! Remember, CMRR is calculated as the ratio of the magnitudes of A_d to A_cm. Next, let’s summarize: A differential amplifier outputs a signal that is the amplified difference between two inputs, effectively filtering out common signals.
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Now, let's discuss how we calculate the differential gain, A_d. Can someone recall the formula?
Isn't it A_d = V_out / V_id?
That's right! And when we use a BJT differential amplifier, A_d can also be expressed in terms of transconductance. Who can tell me the expression for g_m?
g_m is I_CQ divided by V_T, where V_T is approximately 26mV at room temperature.
Excellent! So our equation for differential gain A_d becomes A_d = -g_m R_C / 2, using the collector resistor R_C. Remember, the negative sign indicates a phase inversion. Now, let's calculate a sample value together. Assume R_C = 4.7k Ohm and I_CQ = 0.5 mA.
So A_d becomes -((0.5 mA)*(4.7 k Ohm))/2, which is about -45.19!
Perfect! That’s how we derive the gain for our amplifiers. Great teamwork!
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Let’s shift gears to operational amplifiers. Who can explain what differentiates inverting and non-inverting configurations?
In the inverting configuration, the input goes into the negative terminal, and we get a phase shift of 180 degrees, right?
That’s correct! And what about the gain formula for the inverting amplifier?
It’s A_v = -R_f / R_in!
Excellent! Now, how does the non-inverting amplifier differ?
For the non-inverting setup, we directly apply the input to the non-inverting terminal. The gain is A_v = 1 + R_1/R_2.
Exactly! This gives you a higher input impedance. To summarize: inverting amplifiers invert the phase while non-inverting amplifiers maintain it. Let’s keep these configurations in mind as we move to practical exercises.
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The section details the operation and performance metrics of BJT differential amplifiers and operational amplifiers (Op-Amps). It covers key concepts such as differential gain, common-mode gain, and the common-mode rejection ratio (CMRR), alongside practical measurements and calculations for various amplifier configurations.
This section explains essential elements of operational amplifier (Op-Amp) basic gain stages, particularly emphasizing differential amplifiers. The primary objective is to analyze both DC and AC performance characteristics of bipolar junction transistor (BJT) differential amplifiers, focusing on crucial metrics like differential gain, common-mode gain, and the common-mode rejection ratio (CMRR).
Through these topics, learners gain insights into the nuances of amplifier design and function, which is critical for further studies in electronics and circuit design.
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The inverting amplifier is set up by connecting an input signal through a resistor to its inverting input terminal, while the non-inverting terminal is kept at ground. The output also feeds back into the inverting input through another resistor, creating a feedback loop. The formula for voltage gain shows how the output voltage relates to the input voltage. The gain is negative, indicating that the output phase is inverted compared to the input.
Think of the inverting amplifier like a seesaw. If a child pushes down on one side (the input), the other side (the output) goes up. This represents how the input and output are inversely related. If the input increases, the output decreases and vice versa.
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To calculate the voltage gain of the inverting amplifier, plug the resistor values into the gain formula. For example, with R_in set to 1kΩ and R_f to 10kΩ, it results in a voltage gain of -10. This means that if you input a signal, the output voltage will be 10 times higher but inverted.
Imagine a water pipe where the input water pressure (voltage) increases. If the pipe narrows down (like increasing R_f), the water shoots out much stronger on the other side, but if the pressure reverses (the negative sign), it signifies that the direction of flow is opposite to what's expected.
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In this configuration, the input signal goes to the non-inverting terminal of the Op-Amp. The feedback through resistors R_1 and R_2 influences the gain positively. The voltage gain equation shows how the gain is directly proportional to the resistors' values. The non-inverting amplifier provides a high input impedance, meaning it doesn’t significantly load the signal source.
Consider this amplifier like a group of friends discussing a topic. If one person shares a story (the input), the group collectively responds more positively, emphasizing it further (the output). The way they react is amplified and understood better, similar to how the amplifier boosts the input signal.
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To find the voltage gain for this non-inverting amplifier, simply substitute the resistor values into the gain formula. For R_1 of 9kΩ and R_2 of 1kΩ, it results in a gain of 10, meaning whatever input voltage you provide, the output will be 10 times that value.
Think of an amplifier at a concert. If you have a singer (the input) and the microphone system (the amplifier) boosts their voice so that it reaches the whole audience (the output), effectively increasing everyone’s experience. The gain indicates how much stronger their voice is projected.
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The bandwidth of an Op-Amp is crucial because it tells us how well the amplifier can operate at different frequencies. As you increase the gain, the bandwidth generally decreases. The gain-bandwidth product is a constant that helps relate these two factors, meaning they are inversely related. So, if we wish to achieve high gain at a particular frequency, our bandwidth must be limited.
Imagine a relay race where runners start at different points. The more runners you have (high gain), the shorter the distance each runner needs to cover (limited bandwidth). If you have fewer runners, they cover more distance effectively, just like the amplifier can perform well over a broader range of frequencies if not asking too much gain.
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Key Concepts
Differential Gain (A_d): The ratio of the output voltage to the differential input voltage.
Common-Mode Gain (A_cm): The ratio of the output voltage to the common-mode input voltage.
Common Mode Rejection Ratio (CMRR): A statistical measure of performance indicating how well the differential amplifier rejects common-mode inputs.
Operational Amplifier (Op-Amp): A versatile component used to perform various analog functions, with different configurations providing unique gain characteristics.
See how the concepts apply in real-world scenarios to understand their practical implications.
Calculating the differential gain of a BJT differential amplifier with specific resistor and current values.
Comparing inverting and non-inverting amplifier configurations through gain calculations to understand the relationship between resistor values and gain.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
In circuits of two, the difference is true; Amplifying the gap between me and you!
Can You Recall Ratio? (CMRR - where 'C' is for common, 'Y' for you, and 'R's for rejection ratio).
Imagine two friends, one saying it's sunny while the other says it's raining. The differential amplifier hears them both but focuses only on the difference – are they arguing over what's real?
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Review the Definitions for terms.
Term: Differential Amplifier
Definition:
An amplifier that amplifies the difference between two input signals while rejecting any signals that are common to both inputs.
Term: Common Mode Rejection Ratio (CMRR)
Definition:
A measure of how well a differential amplifier can reject common-mode signals as compared to its ability to amplify differential signals.
Term: Transconductance (g_m)
Definition:
The ratio of the output current to the input voltage in a transistor, representing how effectively the transistor can control the output current.
Term: Operational Amplifier (OpAmp)
Definition:
A high-gain voltage amplifier with a differential input and usually a single-ended output.
Term: Inverting Amplifier
Definition:
An amplifier configuration where the input signal is applied to the inverting input, resulting in a phase-inverted output.
Term: NonInverting Amplifier
Definition:
An amplifier configuration where the input signal is applied to the non-inverting input, producing an output in phase with the input.