Lab 2 - ECE 420L 

Authored by Stephanie Silic

silics@unlv.nevada.edu

February 5th, 2017 

  

Lab Description

  

This lab details the reason for and operation of a compensated scope probe.

 

 

Lab Report

  

    An oscilloscope probe has a variable capacitor which compensates for the capacitance of its cable and the capacitance of the BNC connector on the scope. By adjusting this capacitor on the probe, we can compensate for these capacitances. Below is the 10X, or 10:1, probe used in the lab:

  

http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/10X_probe.PNG

  

We also notice in the photo shown above that the input resistance of the oscilloscope is 1M Ohm and its input capacitance is 11.5 pF, as noted in the gray lettering on the front of the scope, above the BNC connectors.

  

Undercompensated probe:
http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/overcompensated.PNG
 
Overcompensated probe:
http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/undercompensated.PNG  
 
Properly compensated probe:
http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/properly_compensated.PNG
 
    The type of scope probe the oscilloscope accounts for is set by pushing the color-coded channel button (I used the green channel 4) and selecting "Probe Setup". This button will toggle between a 1X or 10X setting, but it can also be set to a range of  values from 1X to 1000 using the menu buttons to the right of the oscilloscope screen (not shown here).
 
http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/setting_1X_vs_10X.PNG
 
http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/drafted_schematic.PNG
 
 
When we probe the square wave at the point marked "Probe tip" we expect to see the square wave at the scope input.
http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/paper_handcalcs.PNG
 
Simulating the circuit in LTSpice verifies what was calculated above:
 
 http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/sim_compensated.PNG
 
    With the value of C1 set to 11.3pF, the output is a good square wave. We note that Vout is a pulse of 0 to 0.1V, which is 1/10th Vin as we expect with the 1:10 attenuation. If we simulate with a capacitor value greater than 11.3pF, we will get the overcompensated waveform seen at the beginning of the lab. If we use a capacitor value smaller than 11.3 pF, we will get the undercompensated waveform. These two situations are shown below:
 
Overcompensated:
http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/sim_overcompensated.PNG
 
Undercompensated
http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/sim_undercompensated.PNG
 
     If we use the probe cable as the capacitor in an RC circuit, we can read the delay time, or the time it takes the output to reach 50% of the input and then calculate the capacitance using the formula for delay time: td = 0.7RC.
 
Delay time measured on oscilloscope:

http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/Devised_exp_tdelay.PNG
 
Hand Calculations:
http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/HandCalcs_cable-capacitance.PNG
 
Measured capacitance value of cable used:
http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/capacitance_multimeter.PNG
 
  The cable was longer than 1 ft., and a typical capacitance for a coaxial cable should be around 30pF per foot, so this value seems to be low.  Further experimentation and verification can be done to confirm this value.

  Measured with an uncompensated cable:
http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/cable.PNG  http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/uncomp_cable_1MHz.PNG
 
Measured with compensated 10X probe:
http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/compensated_probe_1MHz.PNG
 
    Using the uncompensated cable to measure the output of the voltage divider at a 1MHz input square wave, the RC time constant of the circuit is too large for the output to reach its full value in the "on"  time before the pulse goes low again.  The output wave seen above (top) versus the output wave above (bottom) illustrates the difference in this charging time.

    A test point on a printed circuit board (PCB) can be implemeted by adding a resisor and capacitor in parallel between the point on the board that needs to be probed and where you will actually connect the cable. Knowing the length of cable allows the correct capacitance value to be chosen to compensate for the cable's capacitance. In this way, a cable can be directly connected to the PCB. The value for the capacitor can be calculated in the same way as shown earlier in this lab.
 
http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/test_point.PNG
 

 
http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/Backupsnip1.PNG    http://cmosedu.com/jbaker/courses/ee420L/s17/students/silics/Lab2/Backupsnip2.PNG
 
 
 



 

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