Download Lab 8: Series RC Circuit

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Transcript
Series RC Circuit
It is good practice to short
the unused pin on the
trimpot when using it as a
variable resistor
Velleman
function
generator
Note; 0.1 mF = 100 nF
Shunt
resistor

Oscilloscopes can measure voltage as a function of
time, but not current.
◦ To measure time-varying current, we include a small
resistor at the bottom of the branch in which the current
measurement is desired.
 The value of the resistor chosen should be at least a factor of 10
times smaller than the other resistors in the branch.
 The voltage across the small resistor divided by its resistance
yields the current through the branch.
Measurement
point for voltage
across capacitor
Measurement
point for
input voltage
100nF
10
Measurement
point for current
through resistor
where
V(t)/10W equals
the current.
Steady state values for the capacitor’s voltage and current
are assumed to be reached by the time t = 5t.
The capacitor never fully charges or discharges. The maximum and minimum
capacitor voltage oscillates around ½ of the voltage source connected to the RC
combination. The range of the capacitor voltage depends on how small the period
is compared to 5t. The smaller the period, the smaller the range.
•
•
Plot a graph of vC(t) versus t when the frequency of the square
wave using Equations (7) + (8) form the background section
for Experiment 14 in the lab manual.
Plot a graph of iC(t) versus t, which is found by multiplying the
capacitance by the derivative of Equations (7) + (8) from the
lab manual.
• Equations 7 and 8 are the general equations for the voltage across
the capacitor as it charges and discharges, respectively. Equations
(2) and (3) are only correct when t ≤ 1/10 f.
• You will have to do a piecewise calculation (i.e., switch from equation (7)
to equation (8) for the second half of each period of the square wave when
writing your MATLAB code.
• Examples are given in the Resources/Technical Support MatLAB folder on the
course Scholar site.
• You will run the program for the two different time constants and
include all of the plots mentioned in the lab manual in the lab reports.
•
Plot of the voltage across the capacitor as a function
time
– Use either Vpulse or Digclock as the voltage source
• Instructions on setting up a transient simulation using these sources
are posted under Resources/Technical Support: Circuit Simulation
• Include the input voltage in the plot and show three periods.
• Plot of the current through the capacitor as a function time
– Plot of the voltage across the shunt resistor divided by its
resistance as a function time
• Instructions on how to perform calculations in the PSpice plotting
routine are posted under Resources/Technical Support: Circuit
Simulation.
– Use a current marker instead of a voltage marker
• Show three periods.
•
Calculated using multiple methods:
– Analytically (Step 1)
– Experimentally after measurements of R, C, and Rshunt
• Note that you have the ability to measure capacitance on your
digital multimeter.
– From a curve fit of v(t) as the voltage across the capacitor
decreases when the input voltage changes from +5V to
ground.
• This is done for each time constant.
•
Set the Velleman function generator such that Vin is
a square wave that swings from 0V to +5V.
• Settings for the square wave are 5V amplitude with 2.5V offset.
• The duty cycle is 50%.
• Frequency should be set to 1 kHz.
– Use DC coupling on Channel 1 and Channel 2
• Ignore the comments in the lab manual about AC coupling
unless you select AC Coupling when performing the
measurements.
• Ignore all comments about a sound card or the Zeitnitz
oscilloscope software program.

No credit will be given for step 32 so you do not
need to complete this step.