What is the role of biasing in a Class A BJT amplifier?

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Discussion Overview

The discussion centers on the role and implications of biasing in Class A BJT amplifiers, exploring its purpose in establishing operating regions, the effects on output signals, and design considerations for achieving specific transfer functions. Participants examine both theoretical and practical aspects of biasing in amplifier circuits.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant seeks clarification on the purpose of biasing in a BJT Class A amplifier, noting its role in placing the circuit in a specific operating region.
  • Another participant illustrates the effect of biasing using a sine wave input, arguing that proper biasing allows for undistorted amplification of the signal.
  • A question is raised about the method for selecting bias current to design for a specific transfer function, with a suggestion that it may require a small signal model.
  • It is noted that the gain of an amplifier is typically determined by the transistor's characteristics and load resistance, rather than the bias current itself.
  • Participants discuss the use of current sources for biasing, with one noting that while resistors are more common in discrete circuits, current sources are often preferred in integrated circuits for their advantages in size and functionality.
  • There is a mention that certain circuits may serve more as substitute loads rather than biasing components, indicating a need for proper biasing arrangements.

Areas of Agreement / Disagreement

Participants express varying views on the methods and implications of biasing, with no consensus reached on the best practices or specific techniques for biasing in Class A amplifiers.

Contextual Notes

The discussion includes assumptions about the characteristics of transistors and load resistances, as well as the implications of biasing on signal distortion and amplifier performance. Some participants reference specific circuit configurations without resolving the effectiveness of these approaches.

Who May Find This Useful

Readers interested in amplifier design, BJT operation, and biasing techniques in electronic circuits may find this discussion relevant.

b-rett
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Can someone clarify the overall purpose and implications of biasing a BJT Class A amplifier? I just can't get my head wrapped around the entire purpose.

As far as I know, biasing the circuit will place it in a certain operating region, but I don't know the limits/implications of doing this.

Example from book: "Consider the operation of the emitter follower circuit for sine-wave input. Neglecting V_CEsat we see that if the bias current I is properly selected, the output voltage can swing from -V_CC to +V_CC with the quiescent value being zero."

What constitues a "properly selected" bias current I and why does this gave way to the output being able to swing between -V_CC and +V_CC?
 
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Have a look at this circuit and graph:
http://dl.dropbox.com/u/4222062/Voltage%20amplifier.PNG

You can see that if the input voltage is gradually increased, the output stays the same (12 V) for a while then starts to drop until the output is zero.

Quite a small change in voltage (0.6 V to 1.1 V) caused the change in output from 12 volts to zero. So, it works as an amplifier.

But what if you had a sinewave you wanted to amplify?
Sinewaves swing positive and negative.
If you just used a sinewave at the input, you would get output variation only for the small input range of +0.6 volts to +1.1 volts. All the negative part of the sinewave would be lost and a lot of the positive half. The output would be very distorted.

The best way to do this would be to set the zero point of the sinewave at about 0.85 volts and then vary the sinewave around this level. This is biasing.

Suppose you did this and varied the sinewave from 0.7 v to 1 v. You can see that the output would vary from about 10 volts to about 2 volts and it would be an undistorted sinewave but amplified to be bigger than the input.

This is all that biasing does. It tries to make sure that the output will be an undistorted version of the input.
 
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makes sense now.

i see biasing often done with current sources usually at the emitter of the npn. is there a way to easily choose this bias current to design for a specific transfer function with respect to changing input voltage, or does it require a small signal model and calculating the overall gain and manipulating impedance for pole/zero?
 
i see biasing often done with current sources usually at the emitter of the npn. is there a way to easily choose this bias current to design for a specific transfer function with respect to changing input voltage, or does it require a small signal model and calculating the overall gain and manipulating impedance for pole/zero?

The gain of an amplifier is not normally set by the bias current. It is a function of the characteristics of the transistor (which you have little control over) and the load resistance.

The bias current is usually dictated by these factors.

For example, if the load resistor has already been chosen, the bias current is selected to give a collector to emitter voltage of about half of the supply voltage. This way, the output voltage can swing equally in each direction.

i see biasing often done with current sources usually at the emitter of the npn.
I don't think I have seen this. Could you give an example?
 
ex this amplifier which is biased by I from Q2.
 

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Yes, I have seen that circuit, but it is very rarely used.

Usually a resistor works OK.
 
vk6kro said:
Yes, I have seen that circuit, but it is very rarely used.

Usually a resistor works OK.

That's certainly true for discrete circuits, where resistors are usually cheaper than transistors, and possibly more reliable.

By contrast, current source biasing is more commonly used within Integrated Circuits. This is partly because moderate to large value integrated resistors are relatively bulky compared to transistors. It is also possible to obtain a number of related bias currents by a technique called current mirroring, which can allow useful features like adjustable speed/power trade-offs.
 
This circuit is really more of a substitute load than a biasing component.

You still have to arrange biasing to Q1's base.
 

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