Calculating Midband Gain for NPN BJT: Are My Results Accurate?

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Discussion Overview

The discussion revolves around calculating the midband gain for a typical NPN BJT, specifically the 2N3904 model. Participants explore the implications of circuit design choices, such as the bypassing of the emitter resistor and the impact of source impedance on gain calculations. The conversation includes technical reasoning and verification of calculations related to gain and impedance measurements.

Discussion Character

  • Homework-related
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant calculates a midband gain of 0.748 and questions its accuracy.
  • Another participant notes that the emitter resistor (RE) is not bypassed and suggests that a high source impedance of 100kΩ could be causing significant gain loss.
  • A different participant asserts that RE is bypassed and challenges the expression of bypassing as CE = 0, indicating that this may misrepresent the circuit's behavior.
  • Concerns are raised about the circuit design, suggesting that bypassing the emitter resistor with a pure capacitor may lead to poor performance and that the gain will be limited by the transistor's beta at higher frequencies.
  • One participant expresses confusion over their calculations, noting discrepancies between their calculated gain and expected values, and questions whether their output voltage is attenuating.
  • Another participant emphasizes the importance of reviewing calculations and notes that heavy attenuation at the input could lead to an overall gain of less than 1.
  • A participant shares their peak-to-peak input and output voltages, indicating a desire to understand how to find -3dB points and measure input and output impedance correctly.
  • One participant suggests measuring voltage across the source resistor to calculate input impedance, recommending the use of a high-impedance probe to avoid affecting circuit conditions.

Areas of Agreement / Disagreement

Participants express differing views on the circuit's design and the implications of bypassing the emitter resistor. There is no consensus on the accuracy of the gain calculations, and multiple competing interpretations of the circuit behavior are present.

Contextual Notes

Participants mention potential limitations in their calculations and the need to clarify definitions and assumptions regarding circuit components and configurations. The discussion reflects uncertainty about the impact of source impedance and the correct methodology for measuring impedance.

Who May Find This Useful

This discussion may be useful for students and practitioners interested in transistor amplifier design, gain calculations, and impedance measurement techniques in electronic circuits.

r19ecua
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Homework Statement


I just have to calculate midband gain for a typical NPN BJT. The transistor model is a 2N3904
scan0391.jpg

scan0392.jpg


Have I calculated something wrong?? My gain is 0.748
 
Last edited:
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RE is not bypassed? So what is its value?

100kΩ is a very high source impedance! You are losing most of your gain there.
 
RE is bypassed, as all capacitors are shorted (internal are open). Source impedance is verified as 100k ohms
 
r19ecua said:
RE is bypassed, as all capacitors are shorted (internal are open).
Okay, but CE = 0 is not the way to express RE being fully bypassed!

Source impedance is verified as 100k ohms
So your have a large attenuator in front of your amplifier stage. Perhaps you should exclude RS from your calculations, so as to present a truer picture?
 
I can't change RS because that's the lab problem and I have no idea why I set all caps to zero, but I understand that CE = 0 is the incorrect way of expressing a short circuit. I calculated mid-band gain however, and my notes read a gain of about 34dB. Where as my calculations show a dB of 2.4 (after 20*log (0.748). So would it be safe to conclude that my output voltage is attenuating and that my value calculated in class is incorrect?
 
This circuit will not work right. You can't bypass the emitter resistor with a pure capacitor. The gain will climb with frequency until the transistor becomes beta-limited. A poor design.

Eliminate CE and you have a hi-pass circuit with the upper frequency rolloff determined by transistor specs only.
 
It would be worth going over your calculations, checking carefully. For example, that second last line which you equate to 0.748, does that line look right to you?

Whatever gain your transistor stage contributes, it will be largely undone by the heavy attenuation at the input, the attenuator RS and RB'. So I'm not surprised that overall you may appear to have a gain of less than -1.
 
Everyone, I understand what you are all trying to say. With this circuit, gain is less than 1, which means my input resistance is attenuating the output signal by a factor of 0.748. The circuit is not amplifying anything. This was a lab practice problem, I just wanted to know where my calculations were off.

Now, my peak to peak input is 12.6V and my output, (where it's steady BW) is 8.8V. So if everything up to this point is correct, in order to find my -3dB points on the oscilloscope is to multiply the 8.8V by 0.707V. Then, in order to find the frequencies that operate at 6.2V
(8.8 * 0.707V), I need to change the cursors to read a peak-to-peak voltage of 6.2V and start sweeping frequencies (turning knob on function generator).

Untitled-1.png


Based off of this picture, my calculations are slightly off, but the concept is correct. Please let me know if what I've said is totally wrong! If not, my last inquiry would be this:
How do you measure input and output impedance? Do I just place my DMM and measure the resistance? Am I suppose to break the circuit? I know how to calculate it (haven't yet), but by finding Z-thevenin, this value should net me Zin. I believe Zout is just the RL'... Please tell me if I"m incorrect
 
Last edited:
If you measure the voltage on both sides of Rs you can calculate your Zin, so measure the signal at the base using a probe of sufficiently high impedance so it doesn't affect the conditions.
 

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