Calculating the effective impedance of a current source

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Discussion Overview

The discussion revolves around calculating the effective impedance of a current source in a common emitter transistor circuit, particularly when using a constant current source as the emitter load. Participants explore various aspects of circuit design, gain calculations, and the implications of using different transistor configurations, including Darlington pairs.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant seeks to calculate the effective resistance of a current source using a Zener diode and questions how this affects the gain of the circuit.
  • Another participant shares a previous experience with a constant current source and suggests modifications for improved temperature compensation.
  • Several participants request the original poster to provide their circuit for better context and clarity in the discussion.
  • There is mention of the gain of a common emitter amplifier with an unbypassed emitter resistor, which is approximated as (RL/RE) under certain conditions.
  • Concerns are raised about the effective impedance of the collector in a specific circuit configuration and its impact on the input impedance of the main transistor.
  • A participant expresses frustration with online tutorials that provide incomplete information about the impedance of active loads and questions how to reconcile this with gain calculations.
  • Another participant discusses the theoretical infinite impedance of a current source versus the practical output admittance of a transistor, suggesting typical values and their implications for gain.

Areas of Agreement / Disagreement

Participants express varying viewpoints on the effective impedance of current sources and the implications for gain calculations. There is no consensus on the exact values or methods for determining these parameters, indicating ongoing debate and exploration of the topic.

Contextual Notes

Participants highlight limitations in existing tutorials and the complexity of calculating effective impedance, which may depend on specific circuit configurations and assumptions about component behavior.

bitrex
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I'd like to calculate the gain of a common emitter transistor circuit I'm looking at that has a a constant current source as the emitter load. Now I know the gain is going to be -gm(Re||RL) but how do I calculate what the effective resistance of the current source is? The current source I'm using is one that uses a Zener diode to keep a constant voltage across base to emitter junction, and thus a constant current through the collector of and the emitter to collector of the input transistor.

A tangentially related question is, if I were using a Darlington pair as the device connected to the constant current source instead of a transistor, how would I go about calculating the transconductance of the Darlington? Thanks for any assistance!
 
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Here is a constant current source I have used in the past, For this circuit, when changing the pullup resistor R3 from 1 ohm to 50 ohms, the collector current changed from 176.569 mA to 176.566 milliamps in simulation. R1 can be changed to change the output current. For improved temperature compensation of the Q2 base-emitter junction, put a diode in series with R1.
 

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Could you post your actual circuit please?

The gain of a common emitter amplifier with an unbypassed emitter resistor approximates (RL/RE) provided the RE is large compared with the R of the base emitter junction.

This is a very handy way of getting a predictable gain.
 
vk6kro said:
Could you post your actual circuit please?
The gain of a common emitter amplifier with an unbypassed emitter resistor approximates (RL/RE) provided the RE is large compared with the R of the base emitter junction.
This is a very handy way of getting a predictable gain.
I was suggesting in my post that you use the Q1-Q2-R1 circuit in my post and thumbnail as your emitter-to-ground connection instead of just an emitter resistor for a very stable constant current sink. The reason this connection is so stable is that the Q2 collector-to-emitter voltage is about 2 diode drops, so the Q2 gain is pretty good. Using a zener from emitter to base would give you no current adjustability and very poor thermal stability.
-
 
Hi Bob,

My request was to the original poster to post his circuit.


Yours is fairly standard although a bipolar transistor which was fully conducting would be quite a shunt across the input impedance of the main transistor.
One advantage of the unbypassed emitter resistor is that you get an increase in input impedance. It is approximately (Hfe times RE) which is quite a useful lift in impedance for a bipolar transistor.
 
vk6kro said:
Yours is fairly standard although a bipolar transistor which was fully conducting would be quite a shunt across the input impedance of the main transistor.
One advantage of the unbypassed emitter resistor is that you get an increase in input impedance. It is approximately (Hfe times RE) which is quite a useful lift in impedance for a bipolar transistor.
I was trying to point out that the effective impedance of the collector of Q1 in my circuit is very high and has a good frequency (flat) response, and if used as the emitter load in your circuit would give you a very high RE (emitter resistance). Just substitute your circuit for R3, and select R! to adjust the Q1 collector current.
 
Sorry for the delay in my reply. The tutorial online at: http://www.ecircuitcenter.com/Circuits_Audio_Amp/Active_Load_Gain_Stage/Active_Load_Gain_Stage.htm says about the impedance of the active load "And rumor has it - its quite high." Well, how high is it? That's what I hate about some of these tutorials, they'll lead you 90% of the way there and leave you hanging. If I knew the impedance of the active load I could figure out the gain of the stage - is the impedance looking into the emitter of the active load just 1/gm? If that's the case though and the emitter resistance of the transistor the active load is loading is also 1/gm then finding the gain through Rl/Re will give me unity! How's that supposed to give the big gain that current source loads are supposed to provide? Figuring this out has been gnawing at me for days now - any pointers as to where I'm going wrong would help so much!
 
Thanks for the circuit. Makes it much clearer.

A current source has infinite impedance theoretically.
However a real transistor has output admittance which is like a resistor in parallel with the output.
This is typically 10 k but can be as low as 1 K. So, this would be your load from the current source Q4, and it appears in parallel with the output admittance of the gain transistor Q3.

So, worst case, you might really have a load of 500 ohms. More likely it would be about 5000 ohms. This limits your final gain.

The driver circuit apparently includes another current source but details of this are not shown. The input of Q3 will be quite low impedance (maybe 1000 ohms) and the voltage output of the driver would be the current source output times this resistance.
So,
V at input of Q3 = gm * v(1-2) * R (input of Q3).

.
 
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