Lab 14 RS

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The Common Emitter Amplifier

Circuit

1.)Construct the common emitter amplifier circuit below according to your type of emitter.

2.)Calculate all the R and C values to use in the circuit such that

a. Try [math]R_B \approx 220 \Omega[/math] and [math]I_C \approx 100 \mu A[/math]

b. [math]I_C \gt 0.5[/math] mA DC with no input signal

c. [math]V_{CE} \approx V_{CC}/2 \gt 2[/math] V

d. [math]V_{CC} \lt V_{CE}(max)[/math] to prevent burnout

e. [math]V_{BE} \approx 0.6 V[/math]

f. [math]I_D \approx 10 I_B \lt 1[/math] mA

Let's [math]V_{CC} = 20\ V[/math], [math]R_E = 200 \Omega[/math] and [math]R_C = 1.8\ k\Omega[/math]. The load line equation becomes:

[math]I_C = \frac{V_{CC}}{R_E+R_C} + \frac{V_{EC}}{R_E+R_C} = \frac{20\ V}{2\ k\Omega} + \frac{V_{CE}}{2\ k\Omega} = (10 + 0.5 \cdot V_{CE})\ mA[/math]

This load line pretty high and give me the wide range of amplification the input signal.

3.)Draw a load line using the [math]I_{C}[/math] -vs- [math]I_{EC}[/math] from the previous lab 13. Record the value of [math]h_{FE}[/math] or [math]\beta[/math].

On the plot above I overlay me output lines from the previous lab report #13 and me load line I am going to use to construct amplifier. My [math]\beta \approx 150[/math] based on my previous lab report #13

4.)Set a DC operating point [math]I^{\prime}_C[/math] so it will amplify the input pulse given to you. Some of you will have sinusoidal pulses others will have positive or negative only pulses.

I will set up my operating point in the middle of the load line: [math]I_C = 5\ mA[/math], [math]V_EC = 10\ mA[/math]. So I will have the wide range of amplification the input signal [math]I_B = \pm 5\ mA[/math]

Let's calculate all bias voltage to set up this operating point.

[math]V_{EC} = I_E \cdot R_E = 5\ mA \cdot 0.2\ k\Omega = 1\ V[/math]
[math]V_{BE} = 0.6\ V[/math]
[math]V_{B} = V_{CE} + V_B = (1.0 + 0.6)\ V = 1.6\ V[/math]

So to get this operating point I need to set up [math]V_{B} = 1.6\ V[/math]. I can do it using voltage divider [math]R_1/R_2[/math]. To get operating point independent of the transistor base current we want [math]I_{R1} \gg \I_B[/math]

[math]I_B = \frac{I_C}{\beta} = \frac{5\ mA}{200} = 25\ uA[/math]. Here are have used [math]\beta = 200[/math] instead of [math]\beta = 150[/math] as in my previous lab because it's my actual values of [math]\beta[/math] here. I have measured this [math]\beta[/math] using millivoltmeter.

5.)Measure all DC voltages in the circuit and compare with the predicted values.(10 pnts)

6.)Measure the voltage gain [math]A_v[/math] as a function of frequency and compare to the theoretical value.(10 pnts)

7.)Measure [math]R_{in}[/math] and [math]R_{out}[/math] at about 1 kHz and compare to the theoretical value.(10 pnts)

How do you do this? Add resistor in front of [math]C_1[/math] which you vary to determine [math]R_{in}[/math] and then do a similar thing for [math]R_{out}[/math] except the variable reistor goes from [math]C_2[/math] to ground.

8.)Measure [math]A_v[/math] and [math]R_{in}[/math] as a function of frequency with [math]C_E[/math] removed.(10 pnts)

Questions

1. Why does a flat load line produce a high voltage gain and a steep load line a high current gain? (10 pnts)
2. What would be a good operating point an an [math]npn[/math] common emitter amplifier used to amplify negative pulses?(10 pnts)
3. What will the values of [math]V_C[/math], [math]V_E[/math] , and [math]I_C[/math] be if the transistor burns out resulting in infinite resistance. Check with measurement.(10 pnts)
4. What will the values of [math]V_C[/math], [math]V_E[/math] , and [math]I_C[/math] be if the transistor burns out resulting in near ZERO resistance (ie short). Check with measurement.(10 pnts)
5. Predict the change in the value of [math]R_{in}[/math] if [math]I_D[/math] is increased from 10 [math]I_B[/math] to 50 [math]I_B[/math](10 pnts)
6. Sketch the AC equivalent circuit of the common emitter amplifier.(10 pnts)

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