Difference between revisions of "Lab 10 RS"

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  <math>C = 2.2\ uF</math>
 
  <math>C = 2.2\ uF</math>
 
  <math>\mbox{Zener}\ \mbox{Diode}\ 4.7\ V</math>
 
  <math>\mbox{Zener}\ \mbox{Diode}\ 4.7\ V</math>
 
and the following input parameters:
 
 
<math>\Delta t = 17\ ms</math>
 
<math>V_{in} = 12\ V</math>
 
  
  
Line 64: Line 59:
 
[[File:Tek00047.png | 800 px]]
 
[[File:Tek00047.png | 800 px]]
  
As we can see from the sketch above my output voltage has ripple about <math>\Delta V = 0.710\ V<math>, ripple time is the same as input time <math>\Delta t = 16.6\ ms</math>, and the output DC voltage is about <math>V_{out} = 0.6\ V</math>
 
  
 +
As we can see from the sketch above my output voltage has ripple about <math>\Delta V = 0.710\ V</math>, ripple time period is the same as input time <math>\Delta t = 16.6\ ms</math>, and the output DC voltage is about <math>V_{out} = 0.6\ V</math>
 +
 +
 +
 +
 +
<br><br><br><br><br><br><br><br><br><br>
 
=Full-Wave Rectifier Circuit=
 
=Full-Wave Rectifier Circuit=
 
[[File:TF_EIM_Lab10_FW_Rectifier.png| 500 px]]
 
[[File:TF_EIM_Lab10_FW_Rectifier.png| 500 px]]
Line 75: Line 75:
 
The output ripple in this case can be found by <math>\Delta V=\frac{I (\Delta t/2)}{C}</math>
 
The output ripple in this case can be found by <math>\Delta V=\frac{I (\Delta t/2)}{C}</math>
  
Because we are now using <math>(\Delta t/2)</math> instead of <math>(\Delta t)</math> than in previous case for half-wave rectifier theoretiacally we will be able to make <math>\Delta V</math> two times less then in previous case just by using exactly the same ellements and input parameters as before:
+
Because we are now using <math>(\Delta t/2)</math> instead of <math>(\Delta t)</math> than in previous case for half-wave rectifier theoretiacally we will be able to make <math>\Delta V</math> two times less then in previous case just by using exactly the same elements and input parameters as before. But here I realized by experiment that my Zener diode has low power limit and for this kind of circuit I need to use more powerful diode. Instead of 4.7 Zener Diode which has power limit 0.5 W I used rectifier diode 1N4001 which has power limit 50 W.
  
  
Line 86: Line 86:
 
  <math>R_{scope} = 1\ M\Omega</math>
 
  <math>R_{scope} = 1\ M\Omega</math>
 
  <math>C = 2.2\ uF</math>
 
  <math>C = 2.2\ uF</math>
  <math>2\ \mbox{Zener}\ \mbox{Diode}\ 4.7\ V</math>
+
  <math>2\ \mbox{1N4001}\ \mbox{Diode}\ 50\ W</math>
 +
 
 +
 
 +
Because now I need to replace <math>\Delta t</math> by <math>(\Delta t)/2</math> my output voltage now becomes two times less:
 +
 
 +
<math>\Delta V = \frac{0.9\ V}{2} = 0.45\ V</math>
 +
 
 +
Now my DC output voltage becomes about <math>V = 5.2\ V</math> and ripple you can not even see for that scale.
 +
 
 +
[[File:Tek00053.png | 750 px]]
 +
 
  
and the following input parameters:
+
To see ripple I used the AC mode of scope and they are plotted below. As we can see from this sketch my output voltage has ripple about <math>\Delta V = 68.4\ mV</math>, and the ripple time period now is two times less than input time period and is about <math>\Delta t = 8.4\ ms</math>.
  
<math>\Delta t = 17\ ms</math>
+
[[File:Tek00054.png | 750 px]]
<math>V_{in} = 12\ V</math>
 
  
  
Because now I need to replace <math>\Delta t</math> by <math>(\Delta t)/2</math> my output voltage now becomes two times less:
+
Now I have almost perfect output DC current with small ripple.
  
<math>\Delta V = \frac{0.9\ V}{2} = 0.45\ V</math>
 
  
  
 
[https://wiki.iac.isu.edu/index.php/Electronics_RS Go Back to All Lab Reports] [[Forest_Electronic_Instrumentation_and_Measurement]]
 
[https://wiki.iac.isu.edu/index.php/Electronics_RS Go Back to All Lab Reports] [[Forest_Electronic_Instrumentation_and_Measurement]]

Latest revision as of 20:03, 11 March 2011

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Lab 10 Unregulated power supply


Use a transformer for the experiment.

here is a description of the transformer.

File:TF EIM 241 transformer.pdf

File:IN5230-B-T DataSheet.pdf

Half-Wave Rectifier Circuit

1.)Consider building circuit below.

TF EIM Lab10 HW Rectifier.png

Determine the components needed in order to make the output ripple have a [math]\Delta V[/math] less than 1 Volt.

The output ripple can be found by [math]\Delta V=\frac{I\Delta t}{C}[/math]

Taking AC signal from outlet equals to [math]60\ Hz[/math] my input pulse width is [math]\Delta t = \frac{1}{60\ sec} = 17\ ms[/math] and using say [math]C = 2.2\ uF[/math] I need my current to be:

[math]I \le \frac{1\ V \cdot 2.2\ uF}{17\ ms} \le 0.129\ mA[/math]

Taking [math]R \ge 100\ k\Omega \Rightarrow I = \frac{12\ V}{100\ k\Omega} \le 0.12\ mA[/math]

that satisfy the condition above for current so my output ripple becomes less than 1 Volts.



List the components below and show your instructor the output observed on the scope and sketch it below.

I have used the following components:

[math]R = 96.9\ k\Omega[/math]
[math]R_L = 98.7\ k\Omega[/math]
[math]R_{scope} = 1\ M\Omega[/math]
[math]C = 2.2\ uF[/math]
[math]\mbox{Zener}\ \mbox{Diode}\ 4.7\ V[/math]


The current through the circuit can be found as [math]I = \frac{V_{in}}{R_{tot}}[/math]

where [math] R_{tot} = R + \left|\frac{R_L \cdot \frac{1}{j\omega C}}{R_L + \frac{1}{j\omega C}} \right| = R + \sqrt{ \left(\frac{R_L}{1 + j\omega CR_L}\right)\left(\frac{R_L}{1 + j\omega CR_L}\right)^* } = R + \sqrt{ \left(\frac{R_L^2}{1 + (\omega CR_L)^2}\right) } [/math]

[math] = 96.9\ k\Omega + \sqrt{\frac{(98.7\ k\Omega)^2 }{1 + (2\pi\ 60\ sec^{-1})^2(2.2\ uF)^2 (98.7\ k\Omega)^2} }= 96.9\ k\Omega + 1.2\ k\Omega =98.1\ k\Omega[/math].

And the current becomes [math]I = \frac{12\ V}{98.1\ k\Omega} = 0.122\ mA[/math]

So my output ripple becomes [math]\Delta V = \frac{0.122\ mA \cdot 17\ ms}{2.2\ uF} = 0.9 V[/math]


Tek00047.png


As we can see from the sketch above my output voltage has ripple about [math]\Delta V = 0.710\ V[/math], ripple time period is the same as input time [math]\Delta t = 16.6\ ms[/math], and the output DC voltage is about [math]V_{out} = 0.6\ V[/math]













Full-Wave Rectifier Circuit

TF EIM Lab10 FW Rectifier.png


Determine the components needed in order to make the above circuit's output ripple have a [math]\Delta V[/math] less than 0.5 Volt.


The output ripple in this case can be found by [math]\Delta V=\frac{I (\Delta t/2)}{C}[/math]

Because we are now using [math](\Delta t/2)[/math] instead of [math](\Delta t)[/math] than in previous case for half-wave rectifier theoretiacally we will be able to make [math]\Delta V[/math] two times less then in previous case just by using exactly the same elements and input parameters as before. But here I realized by experiment that my Zener diode has low power limit and for this kind of circuit I need to use more powerful diode. Instead of 4.7 Zener Diode which has power limit 0.5 W I used rectifier diode 1N4001 which has power limit 50 W.


List the components below and show your instructor the output observed on the scope and sketch it below.

I have used the following components:

[math]R = 96.9\ k\Omega[/math]
[math]R_L = 98.7\ k\Omega[/math]
[math]R_{scope} = 1\ M\Omega[/math]
[math]C = 2.2\ uF[/math]
[math]2\ \mbox{1N4001}\ \mbox{Diode}\ 50\ W[/math]


Because now I need to replace [math]\Delta t[/math] by [math](\Delta t)/2[/math] my output voltage now becomes two times less:

[math]\Delta V = \frac{0.9\ V}{2} = 0.45\ V[/math]

Now my DC output voltage becomes about [math]V = 5.2\ V[/math] and ripple you can not even see for that scale.

Tek00053.png


To see ripple I used the AC mode of scope and they are plotted below. As we can see from this sketch my output voltage has ripple about [math]\Delta V = 68.4\ mV[/math], and the ripple time period now is two times less than input time period and is about [math]\Delta t = 8.4\ ms[/math].

Tek00054.png


Now I have almost perfect output DC current with small ripple.


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