bekg1113 principle of electrical and electronics
DESCRIPTION
BEKG1113 PRINCIPLE OF ELECTRICAL AND ELECTRONICS. CHAPTER 2 (WEEK 3) FACULTY OF ELECTRONIC AND COMPUTER ENGINEERING. Chapter 2. The topics for this chapter: Voltage and current sources Resistor Resistor Color code Ohm’s Law Types of circuit - series, parallel and series-parallel circuit - PowerPoint PPT PresentationTRANSCRIPT
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BEKG1113PRINCIPLE OF ELECTRICAL AND ELECTRONICS
CHAPTER 2 (WEEK 3)
FACULTY OF ELECTRONIC AND COMPUTER ENGINEERING
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Chapter 2
• The topics for this chapter:– Voltage and current sources– Resistor– Resistor Color code– Ohm’s Law– Types of circuit - series, parallel and series-
parallel circuit– Circuit ground, KVL, KCL, Power dissipation
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Voltage source
– Ideal voltage source
Can provide a constant voltage for any current required by a circuit [1].
– Voltage source can either be AC (Alternating current) or DC (Direct current) [2].
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Voltage source
• The symbols for voltage sources are represented here [1]:
• VI characteristics for an ideal voltage source is shown by the graph [1]
VI characteristics
0
1
2
3
4
5
6
1 2 3 4 5 6 7
I (Ampere)
V (
Vo
lts)
V
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Voltage source
• Six categories of voltage sources [1]:– Batteries– Solar cells– Generator– The electronic power supply– Thermocouples– Piezoelectric sonsors
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• Thermocouples– It is a thermoelectric type of voltage source
that is commonly used to sense temperature. The operation is based on Seebeck effect.
– The types of thermocouples are categorized by letters (J,K,E,N, B and R) that depends on the range of temperature.
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• The graph of thermocouple characteristics.• Note that K is the most common
thermocouple used.
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• A few types of thermocouples which depend on their specification requirements.
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• Piezoelectric sensors– They act as voltage sources and are based
on the piezoelectric effect where a voltage is generated when a piezoelectric material is mechanically deformed by an external force.
– Types of piezoelectric material; quartz & ceramic
– Applications: pressure sensor, force sensor
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Chapter 2: D
irect Current (D
C)
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Chapter 2: Direct Current (DC) Circuit
• The current source– Definition: The ideal current source can
provide a constant voltage for any load.– The symbol for a current source is shown
below
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Current Source
• Constant current sources – a type of power supply
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Current Source
• Constant current sources from most transistor circuits
• Constant current battery chargers
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Basic DC Circuit
• It consists of a source of electrical energy, some sort of load to make use of that energy, and electrical conductors connecting the source and the load.
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SOURCE LOAD
+
-
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Electrical Circuit Requirements
• Control Device: Allows the user control to turn the circuit on or off. Switches are the devices commonly used for controlling the oppening or closing of circuits.
• Protection Device: Current must be monitored and not allowed to exceed a safe level as to protect users from shock, to protect the equipment from damage, and to prevent fire hazards.
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Protective Devices
• Fuses: Fuses use a metallic element that melts when current exceeds a preset value. It will blow if more current passes through it.
• Circuit breaker: Circuit breaker works on the different principle. When the current exceeds the rated value of breaker, the magnetic field produced by excessive current operates a mechanism that trips open a switch. After the fault or overload condition has been cleared, the breaker can reset and used again.
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Current Direction
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Circuit Ground
• Grounding is achieved in an electrical system when one of the conductive wires serving as part of the circuit path is intentionally given a direct path to the earth. This method of grounding is called earth ground.
• In most electronic equipment, a large conductive area on printed circuit board or the metal housing is used as the circuit ground or chassis ground.
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• Ground is the reference point in electric circuits and has a potential of 0 V with respect to other points in the circuit. All of the ground points in a circuit are electrically the same and therefore common points.
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Resistors
• Definition: – A component that is specifically designed to
have a certain amount of resistance is called resistor.
Color bands
Resistance material(carbon composition)
Insulation coating
Leads
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Resistors
• Fixed resistors: provides a specific constant value of resistance– Carbon-composition – Chip resistor– Film resistor– Wirewound resistor
• Variable resistor: values can be changed easily with manual or an automatic adjustment– Potentiometer– Rheostat
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Carbon-composition
• Mixture of finely ground carbon, insulating filler and resin binder.
• The ratio of carbon to insulating filler sets the resistance value.
• Commonly use fixed resistor.
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Chip Resistors
• SMT (Surface Mount Technology) component
• Very small in size ,suitable for compact assemblies.
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Film Resistors
• The resistive material could be carbon film or metal film.
• The desired resistance value is obtained by removing part of resistive material in a spiral pattern along the rod
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• Another type of film type resistor
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Wirewound Resistors
• Constructed with resistive wire wound around an insulating rod and then sealed.
• Used in application that require higher power rating resistance
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• Several types of wirewound resistors
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Potentiometer
• used to divide voltage
• Has 3 terminal; terminal 1&2 have a fixed resistance between them, which is the total resistance. Terminal 3 is connected to moving contact.
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Rheostat
• Used to control current
• Potentiometer can be used as a rheostat by connecting terminal 3 to either terminal 1 or terminal 2
Chapter 2: D
irect Current (D
C)
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Resistors
• Resistor color code
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Ohm’s Law
• Ohm’s law states that current is directly proportional to voltage and inversely proportional to resistance. The formula given are:
V = IR where: I = current in amperes (A)
V = voltage in volts (V)
R = resistance in ohms (Ω)
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• Voltage - is not affected by either current or resistance. It is either too low, normal, or too high. If it is too low, current will be low. If it is normal, current will be high if resistance is low, or current will be low if resistance is high. If voltage is too high, current will be high.
• Current - is affected by either voltage or resistance. If the voltage is high or the resistance is low, current will be high. If the voltage is low or the resistance is high, current will be low.
• Resistance - is not affected by either voltage or current. It is either too low, okay, or too high. If resistance is too low, current will be high at any voltage. If resistance is too high, current will be low if the voltage is fix.
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The linear relationship of current and voltage.
• The relationship can be portrayed by the graph below:
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Example 1
Show that if the voltage in the circuit is increased to three times its present value, the current will triple in value.
R 10V 4.7kΩ
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Example 2
Assume that you are measuring the current in a circuit that is operating with 25V. The ammeter reads 50mA. Later, you notice that the current has dropped to 40mA. Assuming that the resistance did not change, you must conclude that the voltage source has changed. How much has the voltage changed, and what is its new value?
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The inverse relationship of current and resistance.
• As you have seen, current varies inversely with resistance as expressed by Ohm’s law, I = V/R. When the resistance is reduced, the current goes up; when the resistance is increased, the current goes down. For example, if the source voltage is held constant and the resistance is halved, the current doubles in value; when the resistance is doubled, the current is reduced by half.
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Chapter 2: D
irect Current (D
C) C
ircuit
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The Inversely Proportional Relationship
• The inversely proportional can be explained by this graph
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Example 3How many amperes of current are in the circuit of figure below?
R
100V 22Ω
If the resistance in above figure is changed to 47 Ω and the voltage to 50 V, what is the new value of current?
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Example 4
• Calculate the current in figure below.
R
50V 1.0kΩ
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Example 5
– How many milliamperes are in the circuit below?
R
30V 5.6kΩ
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Example 6
– In the circuit below, how much voltage is needed to produce 5 A of current?
R V 100Ω
5 A
5 A
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Example 7
– How much voltage will be measured across the resistor below?
V
V 5 mA
R 56Ω
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Example 8
– Suppose that there is a current of 8 µA through a 10 Ω resistor. How much voltage is across the resistor?
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Example 9
– In the circuit of figure below, how much resistance is needed to draw 3.08 A of current from battery?
12 V R
3.08 A
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Example 10
– Suppose that the ammeter in figure below indicates 4.55 mA of current and the voltmeter across the supply reads 150V. What is the value of R?
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Types of Circuit
• Series
• Parallel
• Series-parallel circuit
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Series Circuit
• Resistor in series
• A series circuit provides only one path for current between two points so that the current is the same through each series resistor [1].
R41k
R31k
R21k
R11k
A B
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• The equation of a series resistors circuit
• The current flow is the same through each element of the series circuit.
• The voltage across the source or power supply is equal to the sum of the voltage drops across the separate resistors in series.
NT IIIII ...321
NT VVVVV ....321
NT RRRRR ....321
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Power Distribution
• Power distribution in series circuit – It is represented by this equation [2]:
– The power delivered by the supply can be determined using the equation [2]:
1 2 3E R R RP P P P
E sP EI
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• Voltage sources in series [2]:
Voltage Sources
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Example 11
• In figures below, find out the total resistance between point A and point B
RT
B
A
R45.6k
R31.2k
R2220
R120
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B
A
R43.3k
R33.3k
R23.3kR1
3.3k
RT
B
A
R41k
R31k
R21k
R11k
RT
BA
R101k
R91k
R81k
R71k
R61k
R51k
RT
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Voltage Divider
• The voltage across a resistor in a series circuit is equal to the value of that resistor times the total applied voltage divided by the total resistance of the series configuration [2].
TT
XR V
R
RV
X
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Example 12a. Find the total resistance RT.
b. Calculate the resulting source current Is.c. Determine the voltage across each resistor.
R3
5
R2 1
R1
2
+E 20V
Is
2
5
1
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Example 13
R3 2k
R2
3k
R1
1k
+E 36V
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Example 13
a. Determine the total resistance RT.
b. Calculate the source current IS.
c. Determine the voltage across each resistor.
d. Find the power supplied by the battery.
e. Determine the power dissipated by each resistor.
f. Comment on whether the total power supplied equals the total power dissipated.
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Parallel Circuit
• The parallel resistors circuit
+ V110V
R51k
R41k
R31k
R21k
R11k
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• The equation of a parallel resistors circuit
• Voltage across each resistor is the same as the voltage across the parallel combination.
• The current flowing through the parallel combination is the sum of the current in the separate branches.
1 2 3
1 1 1 1 1...
eq NR R R R R
VT VVVVV ....321
NT IIIII .....321
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Power in Parallel Circuits
• Total power in a parallel circuit is found by adding up the powers of all the individual resistors, the same as for the series circuits.
BE
NG
1113: C
HA
PT
ER
2 WE
EK
5
60
NT PPPPP ....321
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Exercise 14
• What is the total resistance between point A and point B
R51k
R61k
R71k
R81k
R91k
R101k
A B
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Current Divider
• A parallel circuit acts as a current divider because the current entering the junction of parallel branches “divides” up into several individual branch currents.
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TX
TX I
R
RI
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Series-Parallel
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KVL
• KVL is the abbreviation of Kirchoff’s Voltage Law
• The sum of the voltage drops around a closed loop is equal to the sum of the voltage sources of that loop
• Total voltage = 0
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R3
5
R2 1
R1
2
+E 20V
321 RRR VVVE
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KCL
• Kirchoff’s Current Law
• The current arriving at any junction point in a circuit is equal to the current leaving that junction
• Current in = current out
66
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BE
NG
1113: C
HA
PT
ER
2 WE
EK
5
67
+ V110V
R51k
R41k
R31k
R21k
R11k
54321 RRRRRT IIIIII
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The Branch Current Method
• The branch current method is a circuit analysis method using KVL and KCL to find the current in each branch of a circuit by generating simultaneous equation.
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Example: The Branch Current Method
20V 8V
5Ω 2Ω
10ΩI1 I2
I3
a
b
+
-
++ - -
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• Currents I1, I2 and I3 are assigned to the branches a as shown.
• Applying KCL at node a
• Appling KVL at both loops resulting;
1 2 3I I I
08102
010520
32
31
II
II
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• The following equations can be written
• Solving all three equations will give us
1
2
3
2
1
1
I A
I A
I A
8102
20155
32
32
II
II
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The Mesh Current Method
• In the loop current method, you will work with loop current instead of branch current.
BE
NG
1113: C
HA
PT
ER
2 WE
EK
5
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The Mesh Current Method
20V 8V
5Ω 2Ω
10ΩI1 I2
a
b
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• Appling KVL at both loops resulting;
• Solving both equations will give us;
08102
010520
122
211
III
III
AI
AI
1
2
2
1
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The Node Voltage Method
• Another method of analysis is node voltage method.
• It is based on finding the voltages at each node in the circuit using KCL.
BE
NG
1113: C
HA
PT
ER
2 WE
EK
5
75
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The Node Voltage Method
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20V 8V
5Ω 2Ω
10ΩI1 I2
I3
a
b
+
-
++ - -
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• Currents I1, I2 and I3 are assigned to the branches a as shown.
• Applying KCL at node a
• Express the currents in terms of circuit voltages using Ohms’s law
1 2 3I I I
10
2
85
20
3
2
1
VaI
VaI
VaI
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• Substituting these terms into the current equation yields;
BE
NG
1113: C
HA
PT
ER
2 WE
EK
5
78
VVa
VaVaVa
10102
8
5
20
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Superposition
• A linear network which contains two or more independent sources can be analyzed to obtain the various voltages and branch currents by allowing the sources to act one at a time, then superposing the results.
• This principle applies because the linear relationship between current and voltage.
• Voltage sources are replaced by short circuits; current sources are replaced by open circuits.
• Superposition can be applied directly to the computation of power.
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R423ohmR3
27ohm
R247ohm
R14ohm
+
-
Vs1200V
Is120A
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o.c R423ohmR3
27ohm
R247ohm
R14ohm
+
-
Vs1200V
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• By applying superposition principle, with the 200V acting alone, the 20A current source is replaced by an open circuit.
AI
AI
R
T
T
65.1
31.3
5.60
23
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s.c
Is120A
R423ohmR3
27ohm
R247ohm
R14ohm
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• When the 20-A source acts alone, the 200V source is replaced by a short circuit.
• The total current in the 23Ω resistor is
23 23 23 11.23old newI I I A
AI
RT
58.92023
02.11
02.11
23
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Source Transformation
b
a
2A 5ohm
5ohm
+
-10V
a
b
Thevenin’s equivalent Norton’s equivalent
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Example: The Node Voltage Method
VA
RA
RB
RC RE
VBRD
4 1 2 5
3
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• Assign all currents are going out from node 1 &2.
• From node 1;
• From node 2;
1 1 1 2 0A
A B C
V V V V V
R R R
2 1 2 2 0B
C D E
V V V V V
R R R
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Example: Mesh Analysis
25V
2Ω
5Ω
10Ω 2Ω
50V4ΩI1 I2 I3
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• The matrix that we’ll get
• Solving
05024
0410525
02552
323
32212
211
III
IIIII
III
AI
AI
AI
45.10
17.3
31.1
3
2
1
-ve sign in I1 represents that the assigned current direction opposed the actual current direction.
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• Solve the same circuit using node voltage method
25V
2Ω
5Ω
10Ω 2Ω
50V4ΩI1 I2 I3
1 2
3
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Solution
• at node 1
• At node 2
1 1 1 2250
2 5 10
V V V V
2 1 2 2 500
10 4 2
V V V V
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• From these
• The currents can be determined
11
1 22
23
1.312
3.1710
5010.45
2
VI A
V VI A
VI A
VV
VV
1.29
61.2
2
1
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Test 1 Week 7
• Scientific notation and engineering notation, Resistor color code
• Ohm’s Law, KVL and KCL in Mesh or Node Analysis
• Basic Circuit measurement and measurement equipment
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References
[1] Thomas L.Floyd; Principle of Electric Circuits 8th Ed; Pearson Education; 2007
[2] Robert L.Boylestad; Introductory Circuit Analysis11th Ed; Pearson Education; 2007