Lab 3 TF EIM: Difference between revisions

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= 1-50 kHz filter (20 pnts)=
= 1-50 kHz filter (20 pnts)=
# Design a low-pass RC filter with a break point between 1-50 kHz.  The break point is the frequency at which the filter starts to attenuate the AC signal.  For a Low pass filter, AC signals with a frequency above 1-50 kHz will start to be attenuated (not passed).
1.) Design a low-pass RC filter with a break point between 1-50 kHz.  The break point is the frequency at which the filter starts to attenuate the AC signal.  For a Low pass filter, AC signals with a frequency above 1-50 kHz will start to be attenuated (not passed).
#Now construct the circuit using a non-polar capacitor.
 
Enter your values for<math> R, C,</math> and <math>\omega</math>
{| border="3"  cellpadding="20" cellspacing="0"
|R||C || <math> \omega</math> || <math>\nu</math>
|-
|  || || ||
|}
 
 
2.)Now construct the circuit using a non-polar capacitor.
 
[[File:TF_EIM_Lab3.png | 400 px]]
[[File:TF_EIM_Lab3.png | 400 px]]
#use a sinusoidal variable frequency oscillator to provide an input voltage to your filter.
 
#Measure the input <math>(V_{in})</math> and output <math>(V_{out})</math> voltages for at least 8 different frequencies<math> (\nu)</math>  which span the frequency range from 1 Hz to 1 MHz.
3.)use a sinusoidal variable frequency oscillator to provide an input voltage to your filter.
 
4.)Measure the input <math>(V_{in})</math> and output <math>(V_{out})</math> voltages for at least 8 different frequencies<math> (\nu)</math>  which span the frequency range from 1 Hz to 1 MHz.






{| border="3"  cellpadding="20" cellspacing="0"
{| border="3"  cellpadding="20" cellspacing="0"
|<math>\nu</math> ||<math>V_{in}</math> || <math>V_{out}</math> || <math>\frac{V_out}{V_in}</math>
|<math>\nu</math> ||<math>V_{in}</math> || <math>V_{out}</math> || <math>\frac{V_{out}}{V_{in}}</math>
|-
|-
| Hz || Volts || Volts ||
| Hz || Volts || Volts ||
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|}
|}


#Graph the <math>\log \left(\frac{V_{out}}{V_{in}} \right)</math> -vs- <math>\log (\nu)</math>
5.) Graph the <math>\log \left(\frac{V_{out}}{V_{in}} \right)</math> -vs- <math>\log (\nu)</math>


=phase shift (10 pnts)=
=phase shift (10 pnts)=
#measure the phase shift between <math>V_{in}</math> and <math>V_{out}</math>
#measure the phase shift between <math>V_{in}</math> and <math>V_{out}</math> as a function of frequency <math>\nu</math>.  Hint: you could use<math> V_{in}</math> as an external trigger and measure the time until <math>V_{out}</math> reaches a max on the scope <math>(\sin(\omega t + \phi) = \sin\left ( \omega\left [t + \frac{\phi}{\omega}\right]\right )= \sin\left ( \omega\left [t + \delta t \right] \right ))</math>.


=Questions=
=Questions=


#compare the theoretical and experimentally measured break frequencies. (5 pnts)
#Compare the theoretical and experimentally measured break frequencies. (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>.  The Gain is defined as the ratio of <math>V_{out}</math> to <math>V_{in}</math>.(5 pnts)
#Calculate an expression for <math>\frac{V_{out}}{ V_{in}}</math> as a function of <math>\nu</math>, <math>R</math>, and <math>C</math>.  The Gain is defined as the ratio of <math>V_{out}</math> to <math>V_{in}</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>.(30 pnts)
#Calculate an expression for the phase shift <math>\theta</math> as a function of <math>\nu</math>, <math>R</math>, <math>C</math> and graph <math>\theta</math> -vs <math>\nu</math>. (20 pnts)
#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)
# what is the phase shift <math>\theta</math> for a DC input (the limit as frequency goes to zero)  and a very-high frequency input?(5 pnts)
# what is the phase shift <math>\theta</math> for a DC input and a very-high frequency input?(5 pnts)
# calculate and expression for the phase shift <math>\theta</math> as a function of <math>\nu</math>, <math>R</math>, <math>C</math> and graph <math>\theta</math> -vs <math>\nu</math>. (20 pnts)




[[Forest_Electronic_Instrumentation_and_Measurement]]
[[Forest_Electronic_Instrumentation_and_Measurement]]

Latest revision as of 17:59, 2 February 2015

RC Low-pass filter

1-50 kHz filter (20 pnts)

1.) Design a low-pass RC filter with a break point between 1-50 kHz. The break point is the frequency at which the filter starts to attenuate the AC signal. For a Low pass filter, AC signals with a frequency above 1-50 kHz will start to be attenuated (not passed).

Enter your values for[math]\displaystyle{ R, C, }[/math] and [math]\displaystyle{ \omega }[/math]

R C [math]\displaystyle{ \omega }[/math] [math]\displaystyle{ \nu }[/math]


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 [math]\displaystyle{ (V_{in}) }[/math] and output [math]\displaystyle{ (V_{out}) }[/math] voltages for at least 8 different frequencies[math]\displaystyle{ (\nu) }[/math] which span the frequency range from 1 Hz to 1 MHz.


[math]\displaystyle{ \nu }[/math] [math]\displaystyle{ V_{in} }[/math] [math]\displaystyle{ V_{out} }[/math] [math]\displaystyle{ \frac{V_{out}}{V_{in}} }[/math]
Hz Volts Volts

5.) Graph the [math]\displaystyle{ \log \left(\frac{V_{out}}{V_{in}} \right) }[/math] -vs- [math]\displaystyle{ \log (\nu) }[/math]

phase shift (10 pnts)

  1. measure the phase shift between [math]\displaystyle{ V_{in} }[/math] and [math]\displaystyle{ V_{out} }[/math] as a function of frequency [math]\displaystyle{ \nu }[/math]. Hint: you could use[math]\displaystyle{ V_{in} }[/math] as an external trigger and measure the time until [math]\displaystyle{ V_{out} }[/math] reaches a max on the scope [math]\displaystyle{ (\sin(\omega t + \phi) = \sin\left ( \omega\left [t + \frac{\phi}{\omega}\right]\right )= \sin\left ( \omega\left [t + \delta t \right] \right )) }[/math].

Questions

  1. Compare the theoretical and experimentally measured break frequencies. (5 pnts)
  2. Calculate an expression for [math]\displaystyle{ \frac{V_{out}}{ V_{in}} }[/math] as a function of [math]\displaystyle{ \nu }[/math], [math]\displaystyle{ R }[/math], and [math]\displaystyle{ C }[/math]. The Gain is defined as the ratio of [math]\displaystyle{ V_{out} }[/math] to [math]\displaystyle{ V_{in} }[/math].(5 pnts)
  3. Sketch the phasor diagram for [math]\displaystyle{ V_{in} }[/math],[math]\displaystyle{ V_{out} }[/math], [math]\displaystyle{ V_{R} }[/math], and [math]\displaystyle{ V_{C} }[/math].(30 pnts)
  4. Calculate an expression for the phase shift [math]\displaystyle{ \theta }[/math] as a function of [math]\displaystyle{ \nu }[/math], [math]\displaystyle{ R }[/math], [math]\displaystyle{ C }[/math] and graph [math]\displaystyle{ \theta }[/math] -vs [math]\displaystyle{ \nu }[/math]. (20 pnts)
  5. Compare the theoretical and experimental value for the phase shift [math]\displaystyle{ \theta }[/math]. (5 pnts)
  6. what is the phase shift [math]\displaystyle{ \theta }[/math] for a DC input (the limit as frequency goes to zero) and a very-high frequency input?(5 pnts)


Forest_Electronic_Instrumentation_and_Measurement