EMNG1001_Lab8_RC-Circuits_InClass(2)
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School
George Brown College Canada *
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Course
EMNG1001
Subject
Electrical Engineering
Date
Dec 6, 2023
Type
docx
Pages
7
Uploaded by AgentGuanaco3627
Student First Name:
Karma
Student Last Name:
Jangchup
Student Number:
101494666
Submission Date:
24/11/2023
General Notes:
1.
Type your name, student ID, and the submission date of the lab in the above fields.
2.
Practice safety at all times. Carefully follow the directions of the lab. Do not use broken power
cords or broken devices powered directly from the mains such as the DC supply.
3.
Use only the electronic kit and devices provided by George brown college. Also, ensure that all
equipment in the kit stays in good working condition.
4.
Carefully read and follow
ALL
lab instructions provided in the lab write-up.
5.
Complete all measurements, calculations, tables, drawings, and images required for all labs.
6.
Answer all questions neatly and concisely in the spaces provided (preferably in bold red).
7.
All Labs must be submitted by their due dates in Blackboard and cannot be made up. A grade of
“Zero”
will be assigned for missed labs.
8.
The mark and possible feedback will be posted in Blackboard after the due date of each lab.
Submission: This original word document with answers included in full is required to be submitted in
Blackboard by the due date. It is not allowed to submit another separate document that
includes only answers to the questions.
Lab 8 RC Circuits
Objectives
Upon completion of this lab students will be able to:
1.
Identify and describe the main characteristics of capacitors.
2.
Use the digital multimeter to perform simple capacitor tests.
3.
Construct simple RC circuits.
4.
Use LEDs to provide a visual indication of the charge and discharge cycles of RC circuits.
5.
Describe and verify the charging and discharging cycles of RC circuits.
Introduction
A capacitor is formed whenever two conductors are separated by an insulating material which is called a
dielectric. When a voltage is present between the conductors, there will also be an electric charge
Ali A. Hussein, Ph.D., P. Eng.
EMNG 1001, Circuit Analysis Lab
Page 1
EMNG1001 Circuit Analysis
Lab 8 RC Circuits
between the conductors. The ability to store an electric charge is a fundamental property of a capacitor.
A capacitor’s ability to store charge is directly proportional to the area of the plates and inversely
proportional to the plate separation. The amount of charge stored by a capacitor is given by the
following equation:
Q
=
CV
where
Q
is the charge in Coulombs,
C
is the capacitance in Farads, and
V
is the voltage in
Volts. Recall that current is defined as the amount of charge per time
I
=
Q
/
T
. Hence;
Q
=
IT
where
I
is the current in Ampers, and
T
is the time in seconds. When two capacitors are
connected in series, the same current flows through both capacitors for the same amount of time.
Hence;
Q
1
=
Q
2
→
V
1
V
2
=
C
2
C
1
where
Q
1
(
Q
2
) and
V
1
(
V
2
) are the charge and voltage, respectively, of the capacitor
C
1
(
C
2
). For this reason, the capacitor with the larger capacitance value will take a smaller
voltage than the one with the smaller capacitance value. In a series circuit of
N
capacitors the total
capacitance decreases with the addition of more series capacitors and is found by the following
equation:
C
T
=
[
1
C
1
+
1
C
2
+
…
+
1
C
N
]
−
1
In a parallel circuit of
N
capacitors the total capacitance increases with the addition of more parallel
capacitors and is found by the following equation:
C
T
=
C
1
+
C
2
+
…
+
C
N
The ohmmeter function of the multimeter can be used to check the capacitor before using it in
constructing a circuit. The ohmmeter test can be done as follows:
a.
At first, make sure the capacitor is fully discharged. This can be easily done by shorting the leads of
the capacitor for a moment.
b.
Set the ohmmeter to a very high resistance scale and connect the ohmmeter to the capacitor
leads. Make sure the polarity is correct; i.e. the positive (negative) lead of ohmmeter is connected
to the positive (negative) lead of the capacitor.
c.
At the moment the ohmmeter is connected to the capacitor leads, the ohmmeter should start
changing its reading ideally from a very small resistance to a very large resistance aiming to infinity
(i.e. open circuit). This indicates that the capacitor is in good condition.
d.
The charging time of the capacitor depends on the
RC
time constant of the resulted circuit. So
for large capacitances, you may have to decrease the ohmmeter setting to a lower resistance
range to speed the counting process. For small capacitances, the counting process is so quick that
you might not be able to observe it, so in such a case you have to set the ohmmeter to the
available maximum resistance range. For this reason, testing small capacitances is harder than
testing large capacitances. If you notice that the ohmmeter display flickers on the testing of a
small capacitance (i.e. it changes its displayed number so quick on contacting the capacitor leads),
Ali A. Hussein, Ph.D., P. Eng.
EMNG 1001, Circuit Analysis Lab
Page 2
then that could be considered as enough indication that the capacitor is good. However, if the
display of the ohmmeter never changes showing the symbol of infinity before and after
connecting the small capacitance, then that would indicate the ohmmeter test has failed. This
does not necessarily mean that the small value capacitor is bad in this case. Instead, other
different methods may be utilized to verify the validity of the capacitor.
e.
When conducting the ohmmeter test, the resistance should never remain near zero as this
indicates a capacitor short. On the other hand, an immediate high resistance reading, particularly
for larger capacitors, indicates an open circuit.
The two simple steps of the ohmmeter test are explained in Figure 1 below.
Figure 1 Two steps of the ohmmeter test.
Part 1 Procedure
1.
Obtain five capacitors from your toolbox as listed in Table 1. Use the DMM to perform the
ohmmeter test as explained in the Introduction section of the lab. Base on your observation
indicates the result of the testing of each capacitor (pass or fail) in Table 1.
Table 1 Ohmmeter test results.
Capacitor
Capacitance
Value (µF)
Ohmmeter Test
Result (Pass/Fail)
C
1
100
Pass
C
2
47
Pass
C
3
10
Pass
C
4
0.1
Pass
C
5
0.01
Pass
2.
Construct the circuit shown in Figure 2 on the prototype board. Adjust the DC power source to 12
V. For the switches, S
1
and S
2
, use the push button switches provided in the toolbox. The push-
button switch is normally-opened (OFF status), and it is turned ON when you hold press the
button. The LEDs (LED
1
and LED
2
) are polarized components, so the anode and cathode of each
Ali A. Hussein, Ph.D., P. Eng.
EMNG 1001, Circuit Analysis Lab
Page 3
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LED have to be connected as shown in Figure 2. A reversed polarity LED will not be functioning but
it will not cause damage to this particular circuit unless if the circuit is constructed badly with
errors. Also pay attention that the electrolyte capacitor used in the circuit is also a polarized
component, so its positive and negative leads must be connected as shown in the figure with the
correct polarity. A reversed polarity electrolyte capacitor behaves badly in the circuit and it could
become busted if a strong reverse voltage was applied for time duration enough to blow the
capacitor. Therefore, be careful and always check the constructed circuit before connecting it to
the power supply. At this step leave both S
1
and S
2
in the OFF status (open).
Figure 2 Experimental capacitor circuit.
3.
Close S
1
and observe the LEDs. Record your observations below indicating which LED gives a pulse
of light. Explain what happened.
when we close S1 then LED1 gives a pulse of light it means C1 is charging
.
.....................................................................................................................................................
4.
Open S
1
and then close S
2
. Observe the LEDs and record your observations below indicating which
LED gives a pulse of light. Explain what happened.
when S1 open and S2 close then LED 2 gives a pulse of light it means C1 is discharging at that
time.
5.
Capacitors in series:
a.
Modify the circuit of Figure 2 by adding another capacitor
C
2
=
47
μF
in series with the
capacitor
C
1
=
100
μF
. Draw the resulted circuit (possibly in Multisim) and insert an image
of the drawn circuit in Figure 3.
b.
Make sure that both switches S
1
and S
2
are opened.
c.
Make sure that each capacitor is fully discharged by temporarily shorting its leads.
d.
Close S
1
for a while until LED
1
fully dims again after it gives a pulse of light indicating fully
charging the series capacitors. Measure the voltage of each capacitor handling this step as
quickly as possible to prevent the meter from discharging the capacitors. You might have to
repeat steps “c” and “d” to get a reasonable reading of the voltages as expected in theory.
Record your results below:
The voltage of
C
1
,
V
C
1
=
¿
3.3V
Ali A. Hussein, Ph.D., P. Eng.
EMNG 1001, Circuit Analysis Lab
Page 4
The voltage of
C
2
,
V
C
2
=
¿
6.2V
e.
Using the voltages measured in the previous step, compute the charge of each capacitor:
Charge of
C
1
,
Q
C
1
=
¿
330 J
Charge of
C
2
,
Q
C
2
=
¿
291.4 J
Figure 3 Experimental circuit drawn in Multisim using two series capacitors.
6.
Capacitors in Parallel:
a.
Modify the circuit of the previous section by connecting both of
C
1
=
100
μF
and
C
2
=
47
μF
in parallel with each other. Draw the resulted circuit (possibly in Multisim) and
insert an image of the drawn circuit in Figure 4.
b.
Make sure that both switches S
1
and S
2
are opened.
c.
Make sure that both capacitors are fully discharged by temporarily shorting their leads.
d.
Close S
1
for a while until LED
1
fully dims again after it gives a pulse of light indicating fully
charging the parallel capacitors. Measure the voltage of both capacitors one time (because
they both receive the same voltage) handling this step quickly to prevent the meter from
discharging the capacitors. Record your measurement results below:
The voltage of
C
1
and
C
2
,
V
C
1
=
V
C
2
=
¿
9.79V
e.
Using the voltage measured in the previous step, compute the charge of each capacitor:
Ali A. Hussein, Ph.D., P. Eng.
EMNG 1001, Circuit Analysis Lab
Page 5
Charge of
C
1
,
Q
C
1
=
¿
979 J
Charge of
C
2
,
Q
C
2
=
¿
460.13 J
Figure 4 Experimental circuit drawn in Multisim using two parallel capacitors.
Part 2 Questions & Answers
1.
Based on the results obtained in Table 1.0, what conclusions you can make about testing
capacitors using the Ohmmeter?
Based on results obtained in table one . observation were analyzed were as follows for
conclusion :-
Resistance increase up to threshold value and then overload sign appears on ohmmeter ie 1
Conclusion it has passed ohm meter test and hence we can say that there is no leakage in
capacitor and its good to use in lab.
2.
Given the results in step 5 of Part 1, what can you conclude about capacitors in series?
Demonstrate how your results support your answer.
The voltage distribution of capacitors connected in series is asymmetrical, with C2 having a
larger voltage than C1. This confirms the hypothesis that, in a series circuit, the capacitor with
Ali A. Hussein, Ph.D., P. Eng.
EMNG 1001, Circuit Analysis Lab
Page 6
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the larger capacitance value needs a lower voltage than the capacitor with the smaller
capacitance value, based on the equation V1/V2 = C2/C1.
3.
Given the results in step 6 of Part 1, what can you conclude about capacitors in parallel?
Demonstrate how your results support your answers.
The voltage across two capacitors that are connected in parallel is the same; it is the same across C1
and C2. This is in line with the theory that when the total capacitance increases, every capacitor in a
parallel circuit receives the same voltage. The voltage measured in a parallel configuration for C1 and
C2 is the same, indicating that V(C1) = V(C2).
Ali A. Hussein, Ph.D., P. Eng.
EMNG 1001, Circuit Analysis Lab
Page 7
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