Hi everyone,
This is my first post on this forum.
I'm stuck on an exercise with a common emitter amplifier...
Is it possible to ask here a possible solution?
We will be happy to help you help yourself. Ask your question, tell us what you have done to work it out so far, and what troubles the exercise gives you.
I agree with David Bridgen, your writing is quite precise. If you had not mentioned that English was not your first language I am not sure that I could have figured it out from your post.
Ok...
I have attached a doc file with two images.
The first image is the amplifier in a common emitter configuration.
The second image should be the answer of the 1st and 2nd question.
The questions of this exercise are:
1 Using the output characteristics provided, construct the dc load line, (show all the calculations). State why it is possible to assume the load does not affect its performance.
2 Determine the output variations in VCE and IC for a signal input of 20sin(wt) uA.
Hence determine the current gain of the amplifier
3 Calculate the power dissipation and efficiency under these conditions.
4 Calculate the maximum efficiency of the amplifier.
5 Determine a value of bypass capacitor which could be used for amplifying ultrasonic signals between 50kHz and 100kHz.
1) Just following another exercise given during my classes I have tried to solve the first question as follow:
Step 1 KVL for output circuit
Vcc = Vrc + Vce + Vre
Vcc = Vre + Vrc + Vce
= Ic(Re+Rc) + Vce
Step 2 and 3
Set Ic = 0 => Vce = Vcc Vcc = 10V then plot the Vce point on the graph
1). You’ve plotted the dc load line. As to why the load doesn’t affect the performance, it is because the load’s impedance (100k) is far too high compared to the rc (500). What again is that by asuming the load is resistive, the presence of load is only affecting the ac gain by a very small fraction, and the gain remains linear, as the load is calculated parallel to the R3 as Rc.
2). I think you’ve done good for DC signals. For AC signals, it is mentioned in the next point.
3). Up to the power dissipation, I think it’s right, for DC state.
For ac signal, remember that C2 is there, and it’s making the Re becoming around only 2.5 ohms at room temperature, 10mA quiescent Ie.
The next calculations should be based on this AC Re to be valid. (Ic rms, hence Vce rms). Your above calculations is true, though, for DC signals.
4). The maximum efficiency I think is achieved when the signal is occupying the whole range of voltage swing that the transistor is capable of with this configuration.
5). The value for the capacitors should be found at an impedance that gives –3db cut-off at 50kHz. You know, the formula r=1/(ωc).