Lab2 - EE 420L 

Authored by Allan Pineda
pineda3@unlv.nevada.edu
February 10, 2017   
Lab Description: Operation of Compensated Probe

Experiment_1:
Compensated Correctly




UnderCompensated




OverCompensated




Experiment_2:
 
  
 

The image above shows the type of probe used in the lab experiment. The details about the cable is labeled and found in the input of the cable. The 10X attenuation indicates that the probe is a 10:1 probe. Other parameter  can also be found such as input resistance of 10M, 200MHz frequency and input capacitance 12pF. The channel menu in the oscilloscope allows the user to change the proper attenuation ranging from 1X up to 1000X. By changing the attenuation the voltage reading in the scope is also changing depend on the set X.

Experiment_3:



The schematic circuit above represent the circuits probe that was presented in the pre-lab video. Running the simulation using LTspice will give us a ratio of 1000mV input and 100mV output which indicates a 10:1 ratio. Thus the probe ratio has been verified.
Experiment_4:


Experiment_5:
  

Hand Calculation: for 50% Reach Output



To measure the cable capacitance, one must create an RC circuit using the cable probe and a resistance value of 108.5k connected in series. Using a voltage pulse as an input and measuring the time delay for the output to reach the 50% of voltage pulse, we can obtain the value of the capacitance by deriving the formula from above. The image above shows that the capacitance is approximately 11.1pF by subtracting the value from the multi meter (i.e 0.0181nF-0.007nF). Comparing the value obtain from hand calculation, the value are slightly off because of some other parameters involve during the experiment. However, we can conclude that the two are comparatively close.

Experiment_6:

 
   

The reading from the left is when the probe is compensated. It is measures by taking the input and output voltage of the divider. It has an attenuation probe of 10:1, which mean there is a result of 100mV output per 1V of  input. This is due to the introduced capacitance in the circuits that compensate the capacitance from the scope which help the capacitor take time to charge up resulting in a measurable signal. On the other hand, the reading from the right is when the probe is uncompensated. The introduce capacitance in this manner is large that makes the reading almost linear due to the extended time necessary for the capacitance to fully charge. It makes the cable to act like a wire.

Experiment_7:

We can implement a test point on a PCB by including a resisitor and a variable capacitor connected in parallel to prevent the unnecessary effects that may occur when a known length of cable is attached to the test point. By having this in the circuitry board, we have the ability to adjust the capacitor to make the compensated probe into uncompensated cable to minimized the effect of the scope input capacitance.

Conclusion:
The experiment is about learning on how to compensate and uncompensate probe as well as the technique used in probing. It is very important to know the theory behind these method because it can have a significant effects in designing a circuits. Having the ability to understand the effect of this method, can help reduce the unnecessary results and allow for a faster  signals in designing a circuits.