EE 420L
Engineering Electronics II - Lab 2
Authored
by David Flores
Email:
flored6@unlv.nevada.edu
Due:
February 5, 2019 (Extended Due Date: 02/09/19)
Lab Description
In
this lab we will be learning what compensating a scope probe is, different
kinds of scope probes (10:1,1:1) and the amount of capacitance a cable has
within. This can affect output waveforms
on the oscilloscope. So, we will learn exactly how these parameters are
affecting them.
Pre-lab
Lab Instructions
Perform, and document in
your html lab report, the following:
Experiment 1: Scope
Waveforms of 10:1 Probe
Undercompensated: Overcompensated:
Compensated
Correctly:
Comment:
There is a variable capacitor that can be modified with a small screw. In
undercompensated the waveform does not have enough capacitance in parallel with
the 9MEG resistor (10:1) to match the Z2 = 9Z1 equation that capacitance should
be around 11.7pF. This 11.7pF would be 1/9th of the capacitance
within the cable (~90pF, 30pF/ft) in parallel with the scope in capacitance
(~15pF) If there is too much capacitance it is overcompensated, to little
undercompensated, and just right would be correctly compensated.
The
type of Scope probe (i.e., 1:1, 10:1, 100:1, etc.) is set on the scope by clicking on
the channel number that will be used. It will multiply whatever signal is being
inputted by the number so if there is a 1V pk-pk step and you have the
oscilloscope set to 10 times it will show a 10V pk-pk signal.
10:1 scope probe schematic:
Comments:
Here is the schematic of a 10:1 scope probe 9 MEG resistor, 1 MEG scope
input resistance, capacitance of the cable, scope input capacitance,
and capacitance in the probe tip. The scope in resistance and capacitances 1MEG
and 15pF are part of the oscilloscope, the 90pF is the cable capacitance, and
the C1 and R1 and R3 are to get this formula to work Z2 = 9Z1 for all
frequencies that way we would get the correct waveform. If it is a 10:1 it
divides the input by 10 if the scope is set to 1.
10:1
hand calculation:
Comments:
Here are the calculations of the 10:1 scope probe schematic, using circuit analysis
shows that the value of Vscope (Vout)
is 1/10th the value at Vtip (Vin). Using a
Voltage divider and some algebra we can see that the value of Vout/Vin is 0.1.
Experiment 2: Measuring
the Capacitance of a Wire and Probe
For
this part we are building an RC circuit which allows us to solve for the
capacitance if we have the values for both the resistor and the time constant
knowing that the time constant is equal to 63% of the voltage input.
R
= 100k, Vin = 1V, Frequency = 10kHz
Measuring
the capacitance of the oscilloscope probe:
Comments:
Here the yellow wire on top shows how we connected one end of that oscilloscope
probe to the resistor and the other end to ground to make a RC circuit so that
we could calculate the capacitance using the time constant RC.
Oscilloscope
measurements: Measured
Capacitance of Probe LCR: 85.69pF
Comments:
From here we got a time constant of 8.4us. knowing this we have the resistance
of 100k so C=time-constant/Resistance = 11.6pF which gives us a percent error
of 1.97%
Experiment 3: Voltage
Divider
For
this experiment we built a voltage divider and we measured the output using
both a cable and a compensated scope probe to see the differences. The
experiment will be done at high frequencies so that we can see the effects that
the uncompensated cable has compared to the Compensated scope probe. Frequency
= 1MHz
Uncompensated
cable Oscilloscope Measurements Compensated
Oscilloscope Probe Measurements
Comment:
In this experiment we noticed that there was a lot more noise in the cable
measurements we used a cable about 3ft long which would have theoretically 90pF
of capacitance unaccounted for. The output wave from the cable looks pretty close to the o-scope output but this capacitance
could cause the amplitude of the output not to be outputted correctly because
of the charge up time since it would have an RC time constant.
Implementing a test point
on a PCB given length of a cable
The
way to approach this would be very similar to how the Oscilloscope probe. A
test point on a PCB would just need a resistor in parallel with a variable
capacitor. These two components would oversee compensating the waveform
correctly from the added capacitance of the wire. These values would depend on
the length of the wire which gives us the added capacitance. The way to
calculate these values would be Vout/Vin is equal to
1/1. We would do the exact same as the picture except we would not have the
scope capacitance or resistance, the cable would have X capacitance (30pF/ft), and C1 and R1 or Z1 would need to be
solved for. Having the values of vout/vin and Cable
Capacitance would allow us to do so.
10:1
hand calculation:
Conclusion:
This lab was very important, I feel like we should have learned this for previous
labs so that we would not be so lost. I remember seeing uncompensated waveforms
on the oscilloscope and I did not know what was going on. Now that we learned
the ins and outs of the probe we know exactly how to compensate and even
measure with any standard cable knowing the added capacitance.