ENGR337 Lab 2020 Spring
Lab 2: More Spice and the Compensated Probe
Name: Audra Benally
Email: albenally1@fortlewis.edu
1. Title: More Spice and the Compensated Probe
2. Introduction: The purpose
of this lab was to become more familiar with LTSpice and to get
hands-on experience with the oscilloscope and the compensated probe.
3. Materials and Methods:
Materials:
- Computer with LTSpice
- Breadboard
- 1k Ohm Resistor
- 100k Ohm Resistor
- 100pF Capacitor
- 680pF Capacitor
- Oscilloscope and 2 oscilloscope probes
- Function Generator
Methods:
The majority of this study
was done simulating circuits on LTSpice using the symbols and
components to build the circuit. Different components were chosen from
the given component list and assembled on the new schematic space. Then
the program was run using certain .tran conditions. Sections 1.3 and
2.1 were the only parts that were physically built on the breadboard.
The function generator was set to square waves with certain
specifications according to the lab. The oscilloscope had two probes
that were set in the Vout and Vin positions to measure the time delay
of the circuit. The various knobs on the oscilloscope were adjusted to
compare the Vin and Vout waves.
4. Results:
1. Time Delay of Pulses:

Figure 1. The Vout is oscillating throughout the Vin but
not fully meeting the the input because the capacitor does not have
enough time to charge fully.

Figure 2. The same circuit with a lower Vin. The charge
time does not depend on voltage so the same oscillating Vout outcome is
shown.

Figure 3. The circuit with the period changed. Nothing changes except
the look of the graph.

Figure 4. The circuit with the Ton changed. Again, nothing really
changes except the look of the graph.

Figure 5. The circuit with both Ton and the period changed. This
changes the time given for the capacitor to charge. Though it does fix
the issue, the method is unrealistic.

Figure 6. The
original circuit with the 100pF capacitor replaced with a 10pF
capacitor. It takes less time to charge this capacitor so Vout is able
to reach the full 5V in time.

Figure 7. The
original circuit with the 1k ohm resistor replaced with a 100 ohm
resistor. The new resistors allows more flow and so the 100pF capacitor
is able to charge in time.

Figure 8. The measured time delay of the circuit from part 1.3
2. Time Delay and Amplitude Attenuation of Sinewaves

Figure 9. LTSpice simulation of the circuit from part 2

Figure 10. Oscilloscope measurement of the circuit.

Figure 11. Time delay calculations
Table 1. Time delay from the 3
methods: Simulation via LTSpice, Hand calculations, and measurements
from oscilloscope.

3. The Compensated Probe

Figure 12. Calculations for AC and DC attenuation

Figure 13.
The probe circuit with the resistor added in for DC attenuation.

Figure 14.
The probe circuit with the resistor and the capacitor values calculated
above.
5. Discussion