Difference between revisions of "Lab 13 RS"

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'''2.) Construct the circuit below according to the type of transistor you have. '''
 
'''2.) Construct the circuit below according to the type of transistor you have. '''
  
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'''6.) Overlay points from the transistor's data sheet on the graph in part 5.).(10 pnts)'''
 
'''6.) Overlay points from the transistor's data sheet on the graph in part 5.).(10 pnts)'''
  

Revision as of 18:49, 15 March 2011

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DC Bipolar Transistor Curves

Data sheet for transistors.

Media:2N3904.pdf Media:2N3906.pdf

2N3904 PinOuts.png2N3906 PinOuts.png


Using 2N3904 is more srtaight forward in this lab.

Transistor circuit

1.) Identify the type (n-p-n or p-n-p) of transistor you are using and fill in the following specifications.


I am going to use n-p-n transistor 2N3904. Below are some specifications from data shits for this type of transistor:

Value Description
[math]V_{(BR)CEO} = 40\ V[/math] Collector-Base breakdown voltage
[math]V_{(BR)EBO} = 6\ V[/math] Emitter-Base Breakdown Voltage
[math]V_{(BR)CEO} = 40\ V[/math] Maximum Collector-Emitter Voltage
[math]V_{(BR)CBO} = 60\ V[/math] Maximum Collector-Emitter Voltage
[math]I_C = 200\ mA[/math] Maximum Collector Current - Continuous
[math]P = 625\ mW[/math] Transistor Power rating([math]P_{Max}[/math])
[math]h_{FE}\ min \ [/math] [math]h_{FE}\ max \ [/math] [math]I_C[/math], [math]V_{CE}[/math]
40 300 [math]I_C=0.1\ mA[/math], [math]V_{CE}=1.0\ V[/math]
70 300 [math]I_C=1\ mA[/math], [math]V_{CE}=1.0\ V[/math]
100 300 [math]I_C=10\ mA[/math], [math]V_{CE}=1.0\ V[/math]
60 300 [math]I_C=50\ mA[/math], [math]V_{CE}=1.0\ V[/math]
30 300 [math]I_C=100\ mA[/math], [math]V_{CE}=1.0\ V[/math]








2.) Construct the circuit below according to the type of transistor you have.

TF EIM Lab13a Circuit.pngTF EIM Lab13 Circuit.png


Let [math]R_E = 100 \Omega[/math].

[math]V_{CC} \lt 5 Volts[/math] variable power supply

[math]V_{BE}= 1\ V[/math].

Find the resistors you need to have

[math]I_B = 2 \mu A[/math] , [math]5 \mu A[/math] , and [math]10 \mu A[/math]

By measurements I was able to find that [math]V_{BE}= 0.6\ V[/math]. So I am going to use this value. Also let picks up [math]V_{BB}= 1.6\ V[/math]. So my current [math]I_B = \frac{V_{BB} - V_{BE}}{R_B} = \frac{(1.6 - 0.6)\ V}{R_B} = \frac{1.0\ V}{R_B}[/math].

Now to get [math]I_B = 2\ \mu A[/math] I need to use [math]R_B = \frac{1.0\ V}{2\ \mu A} = 500\ k\Omega[/math]
    To get [math]I_B = 5\ \mu A[/math] I need to use [math]R_B = \frac{1.0\ V}{5\ \mu A} = 200\ k\Omega[/math]
    To get [math]I_B = 10\ \mu A[/math] I need to use [math]R_B = \frac{1.0\ V}{10\ \mu A} = 100\ k\Omega[/math]



3.) Measure the emitter current [math]I_E[/math] for several values of [math]V_{CE}[/math] by changing [math]V_{CC}[/math] such that the base current [math]I_B = 2 \mu[/math] A is constant. [math]I_B \approx \frac{V_{BB}-V_{BE}}{R_B}[/math]


I used:

[math]R_1 = (199.5 \pm 1.0)\ k\Omega [/math]
[math]R_1 = (198.7 \pm 1.0)\ k\Omega [/math]
[math]R_1 = (100.0 \pm 1.0)\ k\Omega [/math]
[math]R_B = (R_1 + R_2 + R_3) = (498.2 \pm 1.7)\ k\Omega [/math]

and

[math]R_E = (100.0 \pm 1.0)\ \Omega [/math]


Below is the table with my measurements:

Table 2uA 01.png


And below is my currents and power calculation:

Here:

[math]I_{E} = \frac{V_E}{R_E}[/math]
[math]I_{B} = \frac{V_{BB}-V_B}{R_B}[/math]
[math]P_{max} = I_C \cdot V_{EC} = (I_E - I_B) \cdot V_{EC} [/math] 

Table 2uA 02.png


4a.) Repeat the previous measurements for [math]I_B \approx 5\ \mu A[/math]. Remember to keep [math]I_CV_{CE} \lt P_{max}[/math] so the transistor doesn't burn out


I used:

[math]R_B = (199.5 \pm 1.0)\ k\Omega [/math]

and

[math]R_E = (100.0 \pm 1.0)\ \Omega [/math]


Below is the table with my measurements:

Table 5uA 01.png


And below is my currents and power calculation:

Here:

[math]I_{E} = \frac{V_E}{R_E}[/math]
[math]I_{B} = \frac{V_{BB}-V_B}{R_B}[/math]
[math]P_{max} = I_C \cdot V_{EC} = (I_E - I_B) \cdot V_{EC} [/math] 

Table 5uA 02.png


4a.) Repeat the previous measurements for [math]I_B \approx\ 10 \mu A[/math]. Remember to keep [math]I_CV_{CE} \lt P_{max}[/math] so the transistor doesn't burn out


I used:

[math]R_B = (100.0 \pm 1.0)\ k\Omega [/math]

and

[math]R_E = (100.0 \pm 1.0)\ \Omega [/math]


Below is the table with my measurements:

Table 10uA 01.png


And below is my currents and power calculation:

Here:

[math]I_{E} = \frac{V_E}{R_E}[/math]
[math]I_{B} = \frac{V_{BB}-V_B}{R_B}[/math]
[math]P_{max} = I_C \cdot V_{EC} = (I_E - I_B) \cdot V_{EC} [/math] 

Table 10uA 02.png



5.) Graph [math]I_C[/math] -vs- [math]V_{CE}[/math] for each value of [math]I_B[/math] and [math]V_{CC}[/math] above. (40 pnts)

Bellow is my plot for the case of [math]I_B = 2 \mu A[/math]

Plot 2uA.png


Bellow is my plot for the case of [math]I_B = 5 \mu A[/math]

Plot 5uA.png


Bellow is my plot for the case of [math]I_B = 10 \mu A[/math]

Plot 10uA.png








6.) Overlay points from the transistor's data sheet on the graph in part 5.).(10 pnts)

I can not really do it because there are not good points to compare from data sheet. I can take for example this data from data sheet:

Table sheet 01.png

And from the table above I can only extract the range of [math]I_B[/math] like

1) [math]I_C = 0.1\ mA,\ V_{CE} = 1.0\ V \rightarrow I_B = \frac{I_C}{/beta} = \frac{0.1}{40..300} = (2.5 - 0.33)\ \mu A[/math]
2) [math]I_C = 1.0\ mA,\ V_{CE} = 1.0\ V \rightarrow I_B = \frac{I_C}{/beta} = \frac{0.1}{70..300} = (14.2 - 3.3)\ \mu A[/math]

And my measurements looks like:

1) [math]I_B = 2\ \mu A,\ I_C = 0.3\ mA,\ V_{CE} = 1.0\ V \rightarrow \beta = \frac{I_C}{I_B} = \frac{0.3\ mA}{2\ uA} = 150[/math]
2) [math]I_B = 5\ \mu A,\ I_C = 0.72\ mA,\ V_{CE} = 1.0\ V \rightarrow \beta = \frac{I_C}{I_B} = \frac{0.72\ mA}{5\ uA} = 144[/math]
3) [math]I_B = 10\ \mu A,\ I_C = 1.40\ mA,\ V_{CE} = 1.0\ V \rightarrow \beta = \frac{I_C}{I_B} = \frac{1.40\ mA}{10\ uA} = 140[/math]

First point to note that [math]I_C[/math] from my measurements and from data sheet are different so I can not really overplay them and compare. Second, I have specific values of [math]I_B[/math], otherwise from data sheet I have the range of [math]I_B[/math]. And third, I can't really plot this range of [math]I_B[/math] from data sheet on my plots just because my plot doesn't have the [math]I_B[/math] axis.


All I can do here is to say that my measured [math]\beta[/math] is inside the range of data sheet [math]\beta[/math].

Questions

1) Compare your measured value of [math]h_{FE}[/math] or [math]\beta[/math] for the transistor to the spec sheet? (10 pnts)


I will calculate my [math]\beta[/math] from my measurements above in active region like:

1)[math]I_B = 2\ \mu A[/math]:  [math]\beta = \frac{I_C}{I_B} = \frac{(0.298 \pm 0.010) mA}{(1.967 \pm 0.108) uA} = (151 \pm 9) [/math] 
2)[math]I_B = 5\ \mu A[/math]:  [math]\beta = \frac{I_C}{I_B} = \frac{(0.725 \pm 0.021) mA}{(4.862 \pm 0.121) uA} = (149 \pm 6) [/math] 
3)[math]I_B = 10\ \mu A[/math]:  [math]\beta = \frac{I_C}{I_B} = \frac{(1.391 \pm 0.052) mA}{(9.200 \pm 0.372) uA} = (151 \pm 8) [/math] 


And above values of [math]\beta[/math] are in agreement with range of [math]\beta[/math] from the spec sheet which is from 30 to 300. But I can not say nothing more because 1) my [math]I_C[/math] current doesn't correspond to published in data sheet. 2) My [math]\beta[/math] calculation is for specific value of [math]I_B[/math] current. But in the data sheet the range of [math]\beta[/math] is reported for specific values of [math]I_C[/math] and [math]V_{CE}[/math].


2) What is [math]\alpha[/math] for the transistor? [math]\alpha = \frac {I_{C}}{I_{E}}[/math] (10 pnts)

3) The base must always be more positive (negative) than the emitter for a npn (pnp) transistor to conduct I_C.(10 pnts)

4) For a transistor to conduct I_{C} the base-emitter junction must be forward biased.(10 pnts)

5) For a transistor to conduct I_{C} the collector-base junction must be reversed biased.(10 pnts)

Extra credit

Measure the Base-Emitter breakdown voltage. (10 pnts)


I expect to see a graph [math](I_{B} -vs- V_{BE} )[/math] and a linear fit which is similar to the forward biased diode curves. Compare your result to what is reported in the data sheet.


I used:

[math]R_B = (199.5 \pm 1.0)\ k\Omega [/math]
[math]R_E = (100.0 \pm 1.0)\ \Omega [/math]
[math]V_{CC} = (840 \pm 20)\ mV [/math]


Below is the table with my measurements and current calculations:

Here:

[math]I_{B} = \frac{V_{BB}-V_B}{R_B}[/math]

Table extra.png


And bellow is my plot for the Base-Emitter breakdown voltage

Plot extra fitted.png

The fitting line is [math]I_B[\mu A] = (111.7 \pm 10.61) + (0.1809 \pm 0.01634)[mV] [/math]. The intersection this line with x-axis gives the forward turn on voltage:

[math]V_{BE} = \frac{p_0}{p_1} = \frac{111.7 \pm 10.61}{0.1809 \pm 0.01634} = (617.46 \pm 80.93)[mV][/math]

Actually what we are measuring here is better to call the forward turn on voltage for base-emitter junction (Base-Emitter breakdown voltage is for reverse current measurement). From the data sheet this point (called the base-emitter saturation voltage) is 0.65 V and this point is inside my predicted values [math](617.46 \pm 80.93)[mV][/math]


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