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Today we are discussing current mirrorsβcan anyone tell me what a current mirror is?
Isn't it a circuit that copies a current from one branch to another?
Precisely! We use them in amplifiers to ensure different transistors maintain the same current. Remember, 'mirroring' means duplicating! What do you think happens if thereβs a mismatch in transistor parameters?
I guess it could cause incorrect biasing and affect the output voltage?
Exactly. If transistors are not well-matched, output characteristics will vary, leading to performance issues. Always look for compatible specifications in your circuit designs.
Got it! What values do we usually figure out first?
We start with collector current. For example, if the collector current is 2 mA, how do we find the bias resistance?
We can use the beta value and current to calculate it, right?
Correct! Remember, balancing both base and collector currents is crucial! Let's proceed to the next example.
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Next, let's discuss the output resistance. Can anyone recall the formula we use for calculating the output resistance of our amplifier?
Is it something like R_out = r1 + r4 when transistors are matched?
Close! The output resistance depends on the small signal parameters of the transistors, like r_o1 and r_o4. Given our example, do we know what these values are?
Yes, they are both 50 kβ¦, leading to an output resistance of 25 kβ¦.
Exactly! And understanding this resistance is vital for determining the amplifier's performance. Why is a higher output resistance preferable?
It improves voltage gain and signal integrity?
Right again! Higher output resistance equates to better gain characteristics, which is our goal in amplifier design.
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Now, let's move on to voltage gain. How do we calculate the voltage gain of our circuit?
It's gain = gm * R_out, isn't it?
Exactly! The transconductance multiplied by output res limits gives us the voltage gain. What value do we get in our example?
I remember us finding it around 1923 or close to 2000.
Good memory! High voltage gain means the circuit can amplify signals significantly, which is our primary objective. Can anyone think of a practical application of such high gain?
In audio equipment or perhaps in sensor amplification?
Correct! We encounter these in many real-world applications, emphasizing the importance of proper gain calculations.
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Finally, letβs calculate the DC output voltage. Can anyone remind me how we approach this calculation?
We look at the voltage drop across the base-emitter junctions and bias current?
Exactly! The output voltage can be derived from V_cc minus the V_be drops. If we think in terms of 12V supply minus 0.6V, you get 11.4V.
And if current mismatch occurs, how does that affect our output?
Good question! Mismatches can lead to unexpected drops. If we discover that one transistor operates at slightly different beta, we may find our output voltage differing from expected values.
So, finer details matter a lot in practical scenarios?
Absolutely! Always double-check your parametersβand consider how transistor characteristics may shift with temperature. These nuances define our circuit's reliability.
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This section covers specific numerical examples related to common emitter amplifiers utilizing current mirrors for biasing. It discusses how to establish the appropriate current levels through the transistors involved, the calculations required for determining output voltage, resistance, and voltage gains, while underlining the importance of transistor matching and early voltage effects.
This section delves into the application of current mirrors within common emitter amplifiers, particularly focusing on biasing mechanisms, output resistance, voltage gain calculations, and the role of transistor matching. We consider transistor-Q, which serves as an active load, thus necessitating a proper configuration of bias resistances for transistorsβespecially the collector and base currents that need to match. A precise analysis begins with specified values such as B2 (beta), early voltage, and given current levels (e.g., 2 mA for collector current).
The discussions transition towards real-world implications, illustrating how discrepancies in transistor values can lead to significant output variations, thereby posing practical considerations for differential amplifiers and other applications where precision is essential.
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Dear students, welcome back after the break. So, we are going through different numerical examples and now we are going to talk about one common emitter amplifier which is using current mirror and particularly to bias the active load say Q. We are using current mirror and transistor-1; it is the amplifying device then we are assuming that Q and Q are identical and also we are assuming that whatever this Q and Q are also identical.
In this section, the instructor introduces the topic of common emitter amplifiers utilizing a current mirror. The common emitter amplifier is a foundational circuit in analog electronics used for amplifying signals. The lecturer emphasizes the assumption that certain transistors, labeled Q1 to Q4, are identical, which simplifies calculations and conceptualization. Assuming that components behave in identical ways allows engineers to predict how the circuit will perform under different conditions.
Think of the common emitter amplifier as a team of identical workers in a factory, where each worker (transistor) can produce the same output effectively. By assuming they are identical, you maximize efficiency in understanding how the overall productivity (amplification) of the team (circuit) will function.
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So, to get the I current of transistor-1 and collector current or transistor-4 equal. We want the current flow through transistor-2 should be equal to current flow through transistor-1. And since, Q and Q are identical having the same Ξ² value of 100. So, then the value of this resistance bias resistance, based biased resistance R should be identical to this transistor the resistor R.
This chunk delves into the specifics of biasing the transistors for optimal performance. The goal is to ensure that the collector currents of transistors 1 and 4 are equal, requiring careful balancing of the currents through transistors 1 and 2. Since transistors Q1 and Q2 are identical, they share the same current gain (Ξ²). This matching allows for precise control of the output, as the performance of the circuit hinges on these equal currents.
Imagine a seesaw where two kids of the same weight are sitting. For the seesaw to be balanced (equal current), they have to sit symmetrically. If one child swings up (increased current), the other must emulate the same to keep balance, just like the transistors must have equal current to achieve a stable configuration in the circuit.
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So, that the base current here and base current here, DC base current they should be equal. So, also we do have othered information namely all the devices are having early voltage 100 V and with this information let us try to find what will be the value of this resistance to get the collector current I = 2 mA.
The instructor outlines the process of calculating the bias resistances necessary to achieve a desired collector current of 2 mA. This involves using the known parameters, such as the Early voltage of the transistors, to derive the values of the resistors (R1 and R2) in the circuit. Having the base currents equal is critical for maintaining consistency in the amplification process, ensuring that each transistor operates correctly in the circuit.
Itβs comparable to adjusting the knobs of two home heaters to achieve the same temperature in a room. If one heater (transistor) has more power (current), you must adjust the other heater's settings (resistance) accordingly to maintain the desired room temperature (collector current).
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Now, with this information let us try to find the small signal output resistance and voltage gain of the amplifier. So, we are assuming both the devices are in active region.
In this section, the focus shifts to determining the output resistance and voltage gain of the amplifier. The instructor assumes both transistors are in their active region, a state conducive for amplification. The small signal parameters like output resistance (Ro) are critical for understanding how the amplifier will behave with varying input signals.
Consider this like tuning a radio to find the best signal (voltage gain). You adjust the knobs (output resistance) until you get clear sound (optimal amplification). If the settings are just right, youβll hear the amplified sound without distortion, mimicking perfect voltage gain in these electronic circuits.
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The current flow here it is to be more precise it is 2 mAΓ( ) = 2 mAΓ( ). So, whatever the current. Now if you see this current is getting mirrored here ignoring the base current loss here, because for transistor-3 and transistor-4, we have considered their Ξ²βs are very high.
This segment concentrates on calculating the final DC output voltage based on the mirrored current. The instructor notes that with base current losses negligible due to high beta values for transistors 3 and 4, it allows for a more straightforward calculation of the output voltage. This practical approach enables easier design and analysis of the circuit's behavior.
Imagine scaling up a successful recipe (current) to serve a large crowd. As long as each ingredient is adjusted proportionately (mirrored), the final dish (DC output voltage) will maintain its quality. Neglecting insignificant adjustments ensures you have the best taste in bulk without losing flavor intensity.
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Now where this current it will be coming from. So, of course, we do have in the small signal equivalent circuit we do have r which is connected to the supply.
In this section, the narrative shifts to non-ideal behaviors of the circuits. The instructor explains how certain current imbalances can lead to voltage changes and deviations from predicted values. This aspect illustrates the importance of accounting for small variations in current and the eventual impacts on output voltage.
Think of it like a stream fed by several tributaries (currents). If one tributary dries up (current loss), it can noticeably alter the flow of the main stream (voltage). Small changes can lead to significant impacts downstream, highlighting the need for careful management in electronic circuit designs.
Learn essential terms and foundational ideas that form the basis of the topic.
Key Concepts
Current Mirror: A circuit configuration that maintains a constant current across matched transistors.
Common Emitter Amplifier: An amplifier configuration with output taken from the collector.
Transconductance: Measure of output current per input voltage in an amplifier setup.
See how the concepts apply in real-world scenarios to understand their practical implications.
If we set the collector current of a transistor at 2 mA and use a beta of 100, we can calculate the necessary bias resistor efficiently.
To achieve a voltage gain of around 2000, we consider both output resistance and the transconductance value, factoring in the current flowing through our transistors.
Use mnemonics, acronyms, or visual cues to help remember key information more easily.
In the circuit where current flows, / Mirrors help it stay in rows.
Picture a bridge that carries the same amount of water across two sides of a river. This represents current mirrors, which ensure consistent flow in different paths.
Remember the acronym 'CAVE' for Current Mirrors: Current, Active load, Voltage gain, Early voltage.
Review key concepts with flashcards.
Review the Definitions for terms.
Term: Current Mirror
Definition:
A circuit configuration that copies current from one branch to another, maintaining a constant current across matched transistors.
Term: Common Emitter Amplifier
Definition:
A basic amplifier configuration where the output is taken from the collector, using a common emitter junction for input.
Term: Transconductance (gm)
Definition:
The ratio of the output current to the input voltage in an amplifier, determining the voltage to current conversion effectiveness.
Term: Early Voltage
Definition:
The measure of how much the effective base-emitter voltage must increase to maintain a consistent collector current for a transistor as the collector voltage changes.