Difference between revisions of "Lab 4 RS"
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==Calculate and expression for <math>\frac{V_{out}}{ V_{in}}</math> as a function of <math>\nu</math>, <math>R</math>, and <math>C</math>.(5 pnts)== | ==Calculate and expression for <math>\frac{V_{out}}{ V_{in}}</math> as a function of <math>\nu</math>, <math>R</math>, and <math>C</math>.(5 pnts)== | ||
+ | |||
+ | We have: | ||
+ | |||
+ | :<math>1)\ V_{in} = I \left(R+R_C\right) = I\left(R+\frac{1}{i\omega C}\right)</math> | ||
+ | |||
+ | :<math>2)\ V_{out} = I R </math> | ||
+ | |||
+ | |||
+ | Dividing second equation into first one we get the voltage gain: | ||
+ | |||
+ | :<math>\ \frac{V_{out}}{V_{in}} = \frac{I R}{I\left(R+\frac{1}{i\omega C}\right)} = \frac{i\omega RC}{1 + i\omega RC}</math> | ||
+ | |||
+ | |||
+ | And we are need the real part: | ||
+ | |||
+ | :<math>\left |\frac{V_{out}}{V_{in}} \right | = \sqrt{ \left( \frac{V_{out}}{V_{in}} \right)^* \left( \frac{V_{out}}{V_{in}} \right)} = \sqrt{\left ( \frac{1}{1+i\omega RC}\right ) \left ( \frac{1}{1-i\omega RC}\right )} = \frac{1}{\sqrt{(1 + (\omega RC)^2}} = \frac{1}{\sqrt{(1 + (2\pi \nu RC)^2}}</math> | ||
+ | |||
==Compare the theoretical and experimental value for the phase shift <math>\theta</math>. (5 pnts)== | ==Compare the theoretical and experimental value for the phase shift <math>\theta</math>. (5 pnts)== | ||
==Sketch the phasor diagram for <math>V_{in}</math>,<math> V_{out}</math>, <math>V_{R}</math>, and <math>V_{C}</math>. Put the current <math>I</math> along the real voltage axis. (30 pnts)== | ==Sketch the phasor diagram for <math>V_{in}</math>,<math> V_{out}</math>, <math>V_{R}</math>, and <math>V_{C}</math>. Put the current <math>I</math> along the real voltage axis. (30 pnts)== |
Revision as of 05:53, 26 January 2011
- RC High-pass filter
1-50 kHz filter (20 pnts)
1. Design a high-pass RC filter with a break point between 1-50 kHz. The break point is the frequency at which the filter's attenuation of the AC signal goes to 0(not passed). For a High pass filter, AC signals with a frequency below the 1-50 kHz range will be attenuated .
- To design low-pass RC filter I had:
So
2. Now construct the circuit using a non-polar capacitor.
3. Use a sinusoidal variable frequency oscillator to provide an input voltage to your filter.
4. Measure the input and output voltages for at least 8 different frequencies which span the frequency range from 1 Hz to 1 MHz.
0.1 | |||
1.0 | |||
2.0 | |||
3.0 | |||
4.0 | |||
5.0 | |||
6.0 | |||
7.0 | |||
8.0 | |||
9.0 | |||
10.0 | |||
11.0 | |||
12.0 | |||
15.0 | |||
20.0 | |||
30.0 | |||
40.0 | |||
50.0 | |||
100.0 | |||
200.0 |
5. Graph the -vs-
phase shift (10 pnts)
- measure the phase shift between and
Questions
Compare the theoretical and experimentally measured break frequencies. (5 pnts)
Calculate and expression for as a function of , , and .(5 pnts)
We have:
Dividing second equation into first one we get the voltage gain:
And we are need the real part:
Compare the theoretical and experimental value for the phase shift . (5 pnts)
Sketch the phasor diagram for , , , and . Put the current along the real voltage axis. (30 pnts)
What is the phase shift for a DC input and a very-high frequency input?(5 pnts)
Calculate and expression for the phase shift as a function of , , and graph -vs . (20 pnts)
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