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©M. S. Ramaiah University of Applied Sciences
1
Faculty of Engineering & Technology
Basic Network Concepts
©M. S. Ramaiah University of Applied Sciences
2
Faculty of Engineering & Technology
Lecture 2
Basic Circuit Elements and Energy
Sources
Lecture delivered by:
Kiran Kumar B M
©M. S. Ramaiah University of Applied Sciences
3
Faculty of Engineering & Technology
Topics
• Basic Circuit Elements
• (Energy Sources) Active Elements
• Independent sources
• Dependent sources
©M. S. Ramaiah University of Applied Sciences
4
Faculty of Engineering & Technology
Objectives
At the end of this lecture, student will be able to:
Explain basic circuit elements
Explain current, voltage, resistance, capacitance and inductance
Classify various energy sources
Describe Independent sources
Explain dependent sources
©M. S. Ramaiah University of Applied Sciences
5
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
5
Basic Circuit Elements
©M. S. Ramaiah University of Applied Sciences
6
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
6
Resistor
 Resistance is the physical property of an element or device that resist the
flow of current: it is represented by the symbol R
 Resistors dissipate electrical energy, converting it to heat
 Resistors lower voltage across an active circuit; the voltage on the positive
end will be higher than the voltage on the negative end
Resistance of a wire element is calculated using the relation:
©M. S. Ramaiah University of Applied Sciences
7
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
7
Resistor symbols:
I
L
A
V
R
Ohm’s law
Voltage difference  current
IRV 
R=Resistance Ω[ohms]
©M. S. Ramaiah University of Applied Sciences
8
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
8
Inductor
 An inductor is a circuit element that develops a magnetic field as current
flows through it.
 It stores energy in its magnetic field and this field resists and slows the
movement of electrons in the inductor
 The amount that an inductor resists electrical current is proportional to the
rate of change of current flowing through
+
-
Lv
where L is the inductance in henrys (H)
Note* Inductance is the property whereby an inductor exhibits opposition to the change of current
flowing through it


1
1
t
t
LL
L
o
dtv
L
i
dt
di
Lv
B field
©M. S. Ramaiah University of Applied Sciences
9
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
9
Sign Convention
 The sign convention used with an inductor is the same as for
a power dissipating device.
When current flows into the positive side of the voltage
across the inductor, it is positive and the inductor is
dissipating power.
When the inductor releases energy back into the circuit,
the sign of the current will be negative.
©M. S. Ramaiah University of Applied Sciences
10
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
10
Power and Energy
( )
di
p t vi Li
dt
 
 The energy stored in the magnetic field is thus
( ) ( )
t t
L
di
w t p t dt L i dt L idi
dt 
    
21
( ) ( ) joules
2
Lw t Li t
 The instantaneous power delivered to an inductor is
©M. S. Ramaiah University of Applied Sciences
11
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
11
Inductors in Series
DC
1L 2L NL
1v 2v Nv+ + + -- -
v
i
i
eqLv
+
-
DC
4321eq
4321
4433
2211
4321
L
dt
di
dt
di
dt
di
dt
di
dt
di
dt
di
dt
di
dt
di
dt
di
LLLL
Lv
LLLLv
LvLv
LvLv
vvvvv
eqin
in
in








S
s
seq LL
1
©M. S. Ramaiah University of Applied Sciences
12
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
12
Inductors in Parallel
         1
4321eq
t
t
t
t4
t
t3
t
t2
t
t1
t
t4
4
t
t3
3
t
t2
2
t
t1
1
4321
1111L
vdt
1
vdt
1
vdt
1
vdt
1
vdt
1
vdt
1
vdt
1
vdt
1
vdt
1
1
o
1
o
1
o
1
o
1
o
1
o
1
o
1
o
1
o











LLLL
L
i
LLLL
i
L
i
L
i
L
i
L
i
iiiii
eq
in
in
in
1
1
1

 







 
P
p p
eq
L
L
©M. S. Ramaiah University of Applied Sciences
13
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
13
General Equations for Leq
Series Combination Parallel Combination
• If S inductors are in
series, then
• If P inductors are in
parallel, then:
1
1
1

 







 
P
p p
eq
L
L

S
s
seq LL
1
Inductors in series Inductors in parallal
©M. S. Ramaiah University of Applied Sciences
14
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
14
Capacitors
A capacitor is a passive element that stores energy in its electric field
A capacitor consists of two conducting plates separated by an insulator.
The insulator is called dielectric. (e.g. polystyrene, oil or air)
When a voltage source is connected to the capacitor, the source deposits a
positive charge, +q, on one plate and a negative charge, –q, on the other
+Q –Q
©M. S. Ramaiah University of Applied Sciences
15
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
15
Capacitance is a measure of a capacitor’s ability to store charge on its plates
Consider any isolated pair of conductors with charge Q
C, called the capacitance of the capacitor
( )
( )
dq dv t
i t C
dt dt
 
q Cv
0
0
1 1 1
( ) ( ) ( ) ( )
t t t
t
v t i x dx i x dx i x dx
C C C 
    
0
0
1
( ) ( ) ( )
t
t
v t v t i x dx
C
  
Contd..
©M. S. Ramaiah University of Applied Sciences
16
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
16
Energy stored in the capacitor
 The instantaneous power delivered to the capacitor is
( )
t tdv
w p t dt C v dt C vdv
dt 
    
( )
dv
p t vi Cv
dt
 
 The energy stored in the capacitor is thus
21
( ) joules
2
w Cv t
©M. S. Ramaiah University of Applied Sciences
17
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
17
Capacitors in Series
1
1
1
v idt
C
 
1 2
1 2
1 1 1 1
N
N eq
v v v v idt idt
C C C C
 
       
 
 
1
1 1N
keq kC C
 
The equivalent capacitance of N series connected capacitors is the reciprocal of the sum of
the reciprocals of the individual capacitors. Capacitors in series act like resistors in parallel.
DC
1v 2v Nv
1C 2C NC
v
i
+ + + -- -
i
eqCv
+
-
DC
2
2
1
v idt
C
 
1
N
N
v idt
C
 
©M. S. Ramaiah University of Applied Sciences
18
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
18
Capacitors in Parallel
i
1i 2i Ni
1C 2C NCv
+
-
i
i
eqCv
+
-
1 1
dv
i C
dt
 2 2
dv
i C
dt
 N N
dv
i C
dt

 1 2 1 2N N eq
dv dv
i i i i C C C C
dt dt
      
1
N
eq k
k
C C

 
Thus, the equivalent capacitance of N capacitors in parallel is the sum of the individual
capacitances. Capacitors in parallel act like resistors in series.
©M. S. Ramaiah University of Applied Sciences
19
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
19
Active Elements (Energy Sources)
There are two types of energy sources
Independent sources
Dependent sources
Ideal Voltage Source
 An ideal voltage source is a two terminal device whose terminal voltage is
independent of the current drawn by the network connected to its
terminals
 Both the magnitude and wave form of voltage remain unaffected
 This means an ideal voltage source should have zero internal resistance
Sometimes
used
+
-Vs
©M. S. Ramaiah University of Applied Sciences
20
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
20
 However, in actual practice, there is no voltage source which does not have
internal resistance
 therefore, an actual voltage source is always associated with an internal
resistance
Contd..
©M. S. Ramaiah University of Applied Sciences
21
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
21
Ideal Current Source
 It is a two terminal device which delivers a constant current to the network
connected across its terminals irrespective of the elements of the network
 The current is independent of the voltage across its terminals
It can be seen that the voltage and current sources are dual in the sense that the roles for
current and voltage are interchanged in the two sources
is
©M. S. Ramaiah University of Applied Sciences
22
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
22
Dependent Sources (Controlled Sources)
A dependent voltage source (or current source) would have its terminal
voltage (or current) depend on another circuit quantity such as a voltage or
current
Thus four possibilities exist
o Voltage dependent (controlled) voltage source
It produces a voltage as a function of voltages elsewhere in the given circuit
o Current dependent (controlled) voltage source
It produces a voltage as a function of current elsewhere in the given circuit
o Voltage dependent (controlled) current source
It produces a current as a function of voltages elsewhere in the given circuit
o Current dependent (controlled) current source
It produces a current as a function of current elsewhere in the given circuit
©M. S. Ramaiah University of Applied Sciences
23
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
23
The Circuit Symbols
μ is a multiplying constant that is dimensionless
is a multiplying constant has the dimension volts per ampere
is a multiplying constant has the dimension amperes per volt
is a multiplying constant that is dimensionless
©M. S. Ramaiah University of Applied Sciences
24
Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences
24
Summary
 There are various types of basic Circuit Elements
 Inductors and capacitors can be connected in series or parallel
 There are two types of energy sources Independent sources and dependent
sources
 Output of an independent source does not depend upon the voltage or
current of any other part of the network
 There are four possible dependent sources
 Voltage dependent (controlled) voltage source
 Current dependent (controlled) voltage source
 Voltage dependent (controlled) current source
 Current dependent (controlled) current source

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Ecc203 a 2

  • 1. ©M. S. Ramaiah University of Applied Sciences 1 Faculty of Engineering & Technology Basic Network Concepts
  • 2. ©M. S. Ramaiah University of Applied Sciences 2 Faculty of Engineering & Technology Lecture 2 Basic Circuit Elements and Energy Sources Lecture delivered by: Kiran Kumar B M
  • 3. ©M. S. Ramaiah University of Applied Sciences 3 Faculty of Engineering & Technology Topics • Basic Circuit Elements • (Energy Sources) Active Elements • Independent sources • Dependent sources
  • 4. ©M. S. Ramaiah University of Applied Sciences 4 Faculty of Engineering & Technology Objectives At the end of this lecture, student will be able to: Explain basic circuit elements Explain current, voltage, resistance, capacitance and inductance Classify various energy sources Describe Independent sources Explain dependent sources
  • 5. ©M. S. Ramaiah University of Applied Sciences 5 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 5 Basic Circuit Elements
  • 6. ©M. S. Ramaiah University of Applied Sciences 6 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 6 Resistor  Resistance is the physical property of an element or device that resist the flow of current: it is represented by the symbol R  Resistors dissipate electrical energy, converting it to heat  Resistors lower voltage across an active circuit; the voltage on the positive end will be higher than the voltage on the negative end Resistance of a wire element is calculated using the relation:
  • 7. ©M. S. Ramaiah University of Applied Sciences 7 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 7 Resistor symbols: I L A V R Ohm’s law Voltage difference  current IRV  R=Resistance Ω[ohms]
  • 8. ©M. S. Ramaiah University of Applied Sciences 8 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 8 Inductor  An inductor is a circuit element that develops a magnetic field as current flows through it.  It stores energy in its magnetic field and this field resists and slows the movement of electrons in the inductor  The amount that an inductor resists electrical current is proportional to the rate of change of current flowing through + - Lv where L is the inductance in henrys (H) Note* Inductance is the property whereby an inductor exhibits opposition to the change of current flowing through it   1 1 t t LL L o dtv L i dt di Lv B field
  • 9. ©M. S. Ramaiah University of Applied Sciences 9 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 9 Sign Convention  The sign convention used with an inductor is the same as for a power dissipating device. When current flows into the positive side of the voltage across the inductor, it is positive and the inductor is dissipating power. When the inductor releases energy back into the circuit, the sign of the current will be negative.
  • 10. ©M. S. Ramaiah University of Applied Sciences 10 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 10 Power and Energy ( ) di p t vi Li dt    The energy stored in the magnetic field is thus ( ) ( ) t t L di w t p t dt L i dt L idi dt       21 ( ) ( ) joules 2 Lw t Li t  The instantaneous power delivered to an inductor is
  • 11. ©M. S. Ramaiah University of Applied Sciences 11 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 11 Inductors in Series DC 1L 2L NL 1v 2v Nv+ + + -- - v i i eqLv + - DC 4321eq 4321 4433 2211 4321 L dt di dt di dt di dt di dt di dt di dt di dt di dt di LLLL Lv LLLLv LvLv LvLv vvvvv eqin in in         S s seq LL 1
  • 12. ©M. S. Ramaiah University of Applied Sciences 12 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 12 Inductors in Parallel          1 4321eq t t t t4 t t3 t t2 t t1 t t4 4 t t3 3 t t2 2 t t1 1 4321 1111L vdt 1 vdt 1 vdt 1 vdt 1 vdt 1 vdt 1 vdt 1 vdt 1 vdt 1 1 o 1 o 1 o 1 o 1 o 1 o 1 o 1 o 1 o            LLLL L i LLLL i L i L i L i L i iiiii eq in in in 1 1 1             P p p eq L L
  • 13. ©M. S. Ramaiah University of Applied Sciences 13 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 13 General Equations for Leq Series Combination Parallel Combination • If S inductors are in series, then • If P inductors are in parallel, then: 1 1 1             P p p eq L L  S s seq LL 1 Inductors in series Inductors in parallal
  • 14. ©M. S. Ramaiah University of Applied Sciences 14 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 14 Capacitors A capacitor is a passive element that stores energy in its electric field A capacitor consists of two conducting plates separated by an insulator. The insulator is called dielectric. (e.g. polystyrene, oil or air) When a voltage source is connected to the capacitor, the source deposits a positive charge, +q, on one plate and a negative charge, –q, on the other +Q –Q
  • 15. ©M. S. Ramaiah University of Applied Sciences 15 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 15 Capacitance is a measure of a capacitor’s ability to store charge on its plates Consider any isolated pair of conductors with charge Q C, called the capacitance of the capacitor ( ) ( ) dq dv t i t C dt dt   q Cv 0 0 1 1 1 ( ) ( ) ( ) ( ) t t t t v t i x dx i x dx i x dx C C C       0 0 1 ( ) ( ) ( ) t t v t v t i x dx C    Contd..
  • 16. ©M. S. Ramaiah University of Applied Sciences 16 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 16 Energy stored in the capacitor  The instantaneous power delivered to the capacitor is ( ) t tdv w p t dt C v dt C vdv dt       ( ) dv p t vi Cv dt    The energy stored in the capacitor is thus 21 ( ) joules 2 w Cv t
  • 17. ©M. S. Ramaiah University of Applied Sciences 17 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 17 Capacitors in Series 1 1 1 v idt C   1 2 1 2 1 1 1 1 N N eq v v v v idt idt C C C C               1 1 1N keq kC C   The equivalent capacitance of N series connected capacitors is the reciprocal of the sum of the reciprocals of the individual capacitors. Capacitors in series act like resistors in parallel. DC 1v 2v Nv 1C 2C NC v i + + + -- - i eqCv + - DC 2 2 1 v idt C   1 N N v idt C  
  • 18. ©M. S. Ramaiah University of Applied Sciences 18 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 18 Capacitors in Parallel i 1i 2i Ni 1C 2C NCv + - i i eqCv + - 1 1 dv i C dt  2 2 dv i C dt  N N dv i C dt   1 2 1 2N N eq dv dv i i i i C C C C dt dt        1 N eq k k C C    Thus, the equivalent capacitance of N capacitors in parallel is the sum of the individual capacitances. Capacitors in parallel act like resistors in series.
  • 19. ©M. S. Ramaiah University of Applied Sciences 19 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 19 Active Elements (Energy Sources) There are two types of energy sources Independent sources Dependent sources Ideal Voltage Source  An ideal voltage source is a two terminal device whose terminal voltage is independent of the current drawn by the network connected to its terminals  Both the magnitude and wave form of voltage remain unaffected  This means an ideal voltage source should have zero internal resistance Sometimes used + -Vs
  • 20. ©M. S. Ramaiah University of Applied Sciences 20 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 20  However, in actual practice, there is no voltage source which does not have internal resistance  therefore, an actual voltage source is always associated with an internal resistance Contd..
  • 21. ©M. S. Ramaiah University of Applied Sciences 21 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 21 Ideal Current Source  It is a two terminal device which delivers a constant current to the network connected across its terminals irrespective of the elements of the network  The current is independent of the voltage across its terminals It can be seen that the voltage and current sources are dual in the sense that the roles for current and voltage are interchanged in the two sources is
  • 22. ©M. S. Ramaiah University of Applied Sciences 22 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 22 Dependent Sources (Controlled Sources) A dependent voltage source (or current source) would have its terminal voltage (or current) depend on another circuit quantity such as a voltage or current Thus four possibilities exist o Voltage dependent (controlled) voltage source It produces a voltage as a function of voltages elsewhere in the given circuit o Current dependent (controlled) voltage source It produces a voltage as a function of current elsewhere in the given circuit o Voltage dependent (controlled) current source It produces a current as a function of voltages elsewhere in the given circuit o Current dependent (controlled) current source It produces a current as a function of current elsewhere in the given circuit
  • 23. ©M. S. Ramaiah University of Applied Sciences 23 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 23 The Circuit Symbols μ is a multiplying constant that is dimensionless is a multiplying constant has the dimension volts per ampere is a multiplying constant has the dimension amperes per volt is a multiplying constant that is dimensionless
  • 24. ©M. S. Ramaiah University of Applied Sciences 24 Faculty of Engineering & Technology©M. S. Ramaiah University of Applied Sciences 24 Summary  There are various types of basic Circuit Elements  Inductors and capacitors can be connected in series or parallel  There are two types of energy sources Independent sources and dependent sources  Output of an independent source does not depend upon the voltage or current of any other part of the network  There are four possible dependent sources  Voltage dependent (controlled) voltage source  Current dependent (controlled) voltage source  Voltage dependent (controlled) current source  Current dependent (controlled) current source