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Circuit Theory (EE102) Lecture 1(a) Basic Concepts & Basic Laws Text Book: Fundamentals of Electric Circuits (4 th Ed/3 rd Ed) By Alexander & Sadiku. McGraw-Hill [CH1] Faculty of Engineering Page 1

Lecture 1a [compatibility mode]

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Page 1: Lecture 1a [compatibility mode]

Circuit Theory (EE102)

Lecture 1(a)

Basic Concepts & Basic Laws

Text Book:Fundamentals of Electric Circuits (4th Ed/3rd Ed) By Alexander & Sadiku. McGraw-Hill [CH1]

Faculty of Engineering Page 1

Page 2: Lecture 1a [compatibility mode]

Basic Concepts

1.1 Systems of Units.

1.2 Electric Charge.

1.3 Current.

1.4 Voltage.

1.5 Power and Energy.

1.6 Circuit Elements.

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1.1 System of Units (1)

Quantity Basic unit Symbol

Length meter m

Mass kilogram Kg

Time second s

Electric current ampere A

Thermodynamic

temperature

kelvin K

Luminous intensity candela cd

Six basic units

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1.1 System of Units (2)

The derived units commonly used in electric circuit theory

Decimal multiples and

submultiples of SI units

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1.2 Electric Charges

• Charge is an electrical property of the atomic particles of which matter consists, measured in coulombs (C).

• The charge e on one electron is negative and equal in magnitude to 1.602 × 10-19 C which is called as electronic charge. The charges that occur in nature are integral multiples of the electronic charge.

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1.3 Current (1)

• Electric current i = dq/dt. The unit of ampere can be derived as 1 A = 1C/s.

• A direct current (dc) is a current that remains constant with time.

• An alternating current (ac) is a current that varies sinusoidally with time. (reverse direction)

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1.3 Current (2)

• The direction of current flow

Positive ions Negative ions

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1.3 Current (3)

Example 1

A conductor has a constant current of 5 A. How many electrons pass a fixed point on the conductor in one minute?

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1.3 Current (4)

Solution

1 A = 1C/s, 1e=1.602 × 10-19 C /electron

Total no. of charges pass in 1 min is given by

5 A = (5 C/s)(60 s/min) = 300 C/min.

Total no. of electronics pass in 1 min is given

minelectrons/ 1087.1C/electron 10602.1

C/min 300 21

19x

x=

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1.4 Voltage (1)• Voltage (or potential difference) is the energy

required to move a unit charge through an element, measured in volts (V).

• Mathematically, (volt)

– w is energy in joules (J) and q is charge in coulomb (C).

• Electric voltage, vab, is always across the circuit

element or between two points in a circuit.

– vab > 0 means the potential of a is higher than potential of b.

– vab < 0 means the potential of a is lower than potential of b.

dqdwvab /=

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1.5 Power and Energy (1)

• Power is the time rate of expending or absorbing energy, measured in watts (W).

• Mathematical expression: vidt

dq

dq

dw

dt

dwp =⋅==

i

+

v

i

+

v

Passive sign conventionP = +vi p = –vi

absorbing power supplying power

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1.5 Power and Energy (2)

• The law of conservation of energy

∑ = 0p

• Energy is the capacity to do work, measured in joules (J).

• Mathematical expression ∫ ∫==t

t

t

tvidtpdtw

0 0

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1.6 Circuit Elements (1)

Active Elements Passive Elements

Independentsources

Dependantsources

• A dependent source is an active element in which the source quantity is controlled by another voltage or current.

• They have four different types: VCVS, CCVS, VCCS, CCCS. Keep in minds the signs of dependent sources.

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1.6 Circuit Elements (2)

Example 2

Obtain the voltage v in the branch shown in Figure 2.1.1P for i2= 1A.

Figure 2.1.1P

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1.6 Circuit Elements (3)

Solution

Voltage v is the sum of the current-independent 10-V source and the current-dependent voltage source vx.

Note that the factor 15 multiplying the control current carries the units Ω.

Therefore, v = 10 + vx = 10 + 15(1) = 25 V

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Text Book:Fundamentals of Electric Circuits (4th Ed/3rd Ed) By Alexander & Sadiku. McGraw-Hill [CH2]

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Basic Laws

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Basic Laws

2.1 Ohm’s Law.

2.2 Nodes, Branches, and Loops.

2.3 Kirchhoff’s Laws.

2.4 Series Resistors and Voltage Division.

2.5 Parallel Resistors and Current Division.

2.6 Wye-Delta Transformations.

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2.1 Ohms Law (1)

• Ohm’s law states that the voltage across a resistor is directly proportional to the current I flowing through the resistor.

• Mathematical expression for Ohm’s Law is as follows:

• Two extreme possible values of R: 0 (zero) and ∞∞∞∞ (infinite) are related with two basic circuit concepts: short circuit and open circuit.

iRv =

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2.1 Ohms Law (2)• Conductance is the ability of an element to

conduct electric current; it is the reciprocal of resistance R and is measured in mhos or siemens.

• The power dissipated by a resistor:

v

i

RG ==

1

R

vRivip

22 ===

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2.2 Nodes, Branches and Loops (1)

• A branch represents a single element such as a voltage source or a resistor.

• A node is the point of connection between two or more branches.

• A loop is any closed path in a circuit.

• A network with b branches, n nodes, and l independent loops will satisfy the fundamental

theorem of network topology:

1−+= nlb

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2.2 Nodes, Branches and Loops (2)

Example 1

How many branches, nodes and loops are there?

Original circuit

Equivalent circuit

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2.2 Nodes, Branches and Loops (3)

Example 2

How many branches, nodes and loops are there?

Should we consider it as one branch or two branches?

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2.3 Kirchhoff’s Laws (1)

• Kirchhoff’s current law (KCL) states that the algebraic sum of currents entering a node (or a closed boundary) is zero.

01

=∑=

N

n

niMathematically,

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2.3 Kirchhoff’s Laws (2)

Example 3

• Determine the current I for the circuit shown in the figure below.

I + 4-(-3)-2 = 0

⇒I = -5A

This indicates that the actual current for I is flowing in the opposite

direction.We can consider the whole enclosed area as one “node”.

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2.3 Kirchhoff’s Laws (3)

• Kirchhoff’s voltage law (KVL) states that the algebraic sum of all voltages around a closed

path (or loop) is zero.

Mathematically, 01

=∑=

M

m

nv

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2.3 Kirchhoff’s Laws (4)

Example 4

• Applying the KVL equation for the circuit of the figure below.

va-v1-vb-v2-v3 = 0

V1 = IR1 v2 = IR2 v3 = IR3

⇒ va-vb = I(R1 + R2 + R3)

321 RRR

vvI ba

++

−=

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2.4 Series Resistors and Voltage Division (1)

• Series: Two or more elements are in series if they are cascaded or connected sequentially and consequently carry the same current.

• The equivalent resistance of any number of resistors connected in a series is the sum of the individual resistances.

• The voltage divider can be expressed as

∑=

=+⋅⋅⋅++=N

n

nNeq RRRRR1

21

vRRR

Rv

N

n

n+⋅⋅⋅++

=21

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Example 5

10V and 5ΩΩΩΩare in series

2.4 Series Resistors and Voltage Division (2)

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2.5 Parallel Resistors and Current Division (1)

• Parallel: Two or more elements are in parallel if they are connected to the same two nodes and consequently have the same voltage across them.

• The equivalent resistance of a circuit with N resistors in parallel is:

• The total current i is shared by the resistors in inverse proportion to their resistances. The current divider can be expressed as:

Neq RRRR

1111

21

+⋅⋅⋅++=

n

eq

n

nR

iR

R

vi ==

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Example 6

2ΩΩΩΩ, 3ΩΩΩΩ and 2A are in parallel

2.5 Parallel Resistors and Current Division (2)

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2.6 Wye-Delta Transformations

)(1

cba

cb

RRR

RRR

++=

)(2

cba

ac

RRR

RRR

++=

)(3

cba

ba

RRR

RRR

++=

1

133221

R

RRRRRRRa

++=

2

133221

R

RRRRRRRb

++=

3

133221

R

RRRRRRRc

++=

Delta -> Wye Wye -> Delta

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Example 7

Transform the wye network to a delta network

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Solution