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Basics of Circuit
Circuit Theory
Prof. Mohsin A
Mulla
Asst. Professor, EE
SITCOE, Yadrav.
2
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.
3
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 
4
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
R
G 
1
R
v
Rivip
2
2

5
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
6
2.2 Nodes, Branches and
Loops (2)
Example 1
How many branches, nodes and loops are there?
Original circuit
Equivalent circuit
7
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?
8
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.
0
1

N
n
niMathematically,
9
2.3 Kirchhoff’s Laws (2)
Example 4
• 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”.
10
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, 0
1

M
m
nv
11
2.3 Kirchhoff’s Laws (4)
Example 5
• 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
vv
I ba



12
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 RRRRR
1
21
v
RRR
R
v
N
n
n


21
13
Example 3
10V and 5W
are in series
2.4 Series Resistors and Voltage
Division (1)
14
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
n
R
iR
R
v
i 
15
Example 4
2W, 3W and 2A
are in parallel
2.5 Parallel Resistors and Current
Division (1)
16
2.6 Wye-Delta Transformations
)(
1
cba
cb
RRR
RR
R


)(
2
cba
ac
RRR
RR
R


)(
3
cba
ba
RRR
RR
R


1
133221
R
RRRRRR
Ra


2
133221
R
RRRRRR
Rb


3
133221
R
RRRRRR
Rc


Delta -> Star Star -> Delta

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Basics of Electric circuit theory

  • 1. 1 Basics of Circuit Circuit Theory Prof. Mohsin A Mulla Asst. Professor, EE SITCOE, Yadrav.
  • 2. 2 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.
  • 3. 3 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 
  • 4. 4 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 R G  1 R v Rivip 2 2 
  • 5. 5 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
  • 6. 6 2.2 Nodes, Branches and Loops (2) Example 1 How many branches, nodes and loops are there? Original circuit Equivalent circuit
  • 7. 7 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?
  • 8. 8 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. 0 1  N n niMathematically,
  • 9. 9 2.3 Kirchhoff’s Laws (2) Example 4 • 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”.
  • 10. 10 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, 0 1  M m nv
  • 11. 11 2.3 Kirchhoff’s Laws (4) Example 5 • 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 vv I ba   
  • 12. 12 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 RRRRR 1 21 v RRR R v N n n   21
  • 13. 13 Example 3 10V and 5W are in series 2.4 Series Resistors and Voltage Division (1)
  • 14. 14 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 n R iR R v i 
  • 15. 15 Example 4 2W, 3W and 2A are in parallel 2.5 Parallel Resistors and Current Division (1)