1. Circuit (1)
2. Charge (3-5)
3. Voltage (6-15)
4. Current (16-22)
5. Resistance (23-29)
6. Current and voltage (30-31)
7. Resistance and current (32)
8. Ohm’s Law (33-38)
9. Electrical machine (39-40)
10. Conductor and Insulator (42-44)
11. Semiconductor (45)
12. Ammeter and voltmeter (46-50)
13. Single phase and Triple phase
(51-55)
14. KVL and KCL (56- 62)
15. Resistance in series and parallel
(63-65)
Basic Electrical Engineering (MID COURSE)
By Engr Sharif Ur Rahman
Sharif Arain
Circuits
 Closed Circuit
 Allows a complete path for electrons to travel
 Open Circuit
 Does not allow a complete path for the electrons to
travel
Flow of Charge
 When the ends of an
electric conductor are at
different electric potentials
(voltages)
Charge continues to flow
until the ends of the
conductor has the same
voltage
Charge
 Electrical property of atomic particles
 Electrons are negatively charged
 Protons are positivity charged
 The absolute value of the charge on an electron is 1.6x10-
19 C
 The symbol used is Q or q
Flow of Charge Diagram:
Alessandro Volta (1745 – 1827)
 Italian physicist
 known especially for
the invention of the
electrochemical cell,
aka the battery in
1800.
Voltage
 The flow of charge is established by an external “pressure”
derived from the energy that a mass has by virtue of its position:
Potential energy
 Energy: the capacity/ability of to do work
1. Kinetic energy: Energy an object has due to its motion
2. Potential energy
 If a mass (m) is raised to some height (h) above a reference plane,
it has a measure of potential energy expressed in joules (J) that is
determined by
 W (potential energy) = mgh
where g is the gravitational acceleration (9.8 m/s2)
o Energy that is stored
o Potential energy due to an object’s position
Explanation:
 Potential difference between two points
 Either side of a voltage source is not an eqipotential
surface
 A wire is an equipotential surface
 It has the same potential
 If the wire is attached to a voltage source it is still an
equipotential surface
Equation:
 The electromotive force (emf) that causes charge
to move.
 1 Volt = 1 Joule/1 Coulomb
Q
W
V
dq
dw


 ;v
 Note:
 A potential difference or voltage is always
measured between two points in the system.
 Changing either point may change the potential
difference between the two points under
investigation.
 Potential difference between two points is
determined by: V = W/Q (volts)
Voltage unit define:
 A potential difference of 1 volt (V) exists between
two points if 1 joule (J) of energy is exchanged in
moving 1 coulomb (C) of charge between the
two points
 The unit of measurement volt was chosen to
honor Alessandro Volta
Summary
 The applied potential difference (in volts) of a
voltage source in an electric circuit is the
“pressure” to set the system in motion and
“cause” the flow of charge or current through the
electrical system.
Ideal Voltage Sources
 Independent voltage source outputs a voltage, either
dc or time varying, to the circuit no matter how much
current is required.
Note:
 Potential difference: The algebraic difference in
potential (or voltage) between two points of a network.
 Voltage: When isolated, like potential, the voltage at a
point with respect to some reference such as ground.
 Voltage difference: The algebraic difference in voltage
(or potential) between two points of a system. A
voltage drop or rise is as the terminology would
suggest.
 Electromotive force (emf): The force that establishes
the flow of charge (or current) in a system due to the
application of a difference in potential.
Current
 “The flow of free electron in a copper wire or any other solid
conductor of electricity”
 With no external forces applied, the net flow of charge in a
conductor in any one direction is zero
 Basic electric circuit
 Charge will only flow if there is a voltage source (potential
difference).
 The flow of electric charge
 The loosely bound outer electrons of conductors
carry the charge through circuits
 Protons tightly bound to the nuclei of atoms
André Ampère (1775 – 1836)
 French physicist and
mathematician.
 One of the main
discoverers of
electromagnetism.
 SI unit of measurement of
electric current, the
ampere, is named after
him.
Equation/formula:
 The flow of charge through a cross-sectional area as a
function of time or the time rate of change of charge
 Symbol used is I or i
)(;
;
12
2
1
ttIQdtiQ
t
Q
I
dt
dq
i
t
t





current = charge / time
or
I = q/t
Units: Amps (A)
An amp is the flow of 1 C of charge
per second
NOTE: 1 C = the charge of
6,240,000,000,000,000,000 electrons
Current’s Direction
 Electrons Travel from – to +
 Current is actually the opposite direction of the
flow of electrons
Current Sources
 An ideal current source outputs a dc or ac current to
the circuit no matter how much voltage is required.
 There are no ideal current sources as all known
current sources are unable to generate an unlimited
force (voltage) that is needed to deliver a constant
current to a circuit.
Summary
 Safety considerations
 Even small levels of current through the human
body can cause serious, dangerous side effects
 Any current over 10 mA is considered dangerous
 currents of 50 mA can cause severe shock
 currents over 100 mA can be fatal
 Treat electricity with respect – not fear
Electric Resistance
 “The ability of a material to resist the flow of charge”
 Units: Ohms (W)
 The amount of charge that flows through a circuit
depends on two things:
1. Voltage provided by source
2. Electric resistance of the conductor
 opposes the push from the voltage source.
 Resistance affects the speed of the current.
Georg Ohm (1789 – 1854)
 German physicist
 Ohm determined that
there is a direct
proportionality between
the voltage applied
across a conductor and
the electric current.
 This relationship is known
as Ohm's law.
Equation:
 Resistance takes into account the
physical dimensions of the material
where:
 L is the length of
conductor along which
the carriers are moving
 A is the cross sectional
area of the conductor
that the free electron
move through.
 ρ is the specific resistivity
of a material
A
L
R 
Resistivity, 
 Resistivity is a material property
 Dependent on the number of free electron or
mobile charges (usually electrons) in the material.
 In a metal, this is the number of electrons from the
outer shell that are ionized and become part of the
‘sea of electrons’
 Dependent on the mobility of the charges
 Mobility is related to the velocity of the charges.
 It is a function of the material, the frequency and
magnitude of the voltage applied to make the
charges move, and temperature.
Resistivity of Common Materials at
Room Temperature (300K)
Material Resistivity (W-m) Usage
Silver 1.64x10-8 Conductor
Copper 1.72x10-8 Conductor
Aluminum 2.8x10-8 Conductor
Gold 2.45x10-8 Conductor
Carbon (Graphite) 4x10-5 Conductor
Germanium 0.47 Semiconductor
Silicon 640 Semiconductor
Paper 1010 Insulator
Mica 5x1011 Insulator
Glass 1012 Insulator
Teflon 3x1012 Insulator
Electric Resistance Factors
Thick wires have less resistance than
thin wires
Short wires have less resistance than
long wires
Higher temperatures usually cause
more resistance
The resistance in some materials
becomes almost zero at very low
temperatures
Current vs. Voltage
Current – Flow rate
Measured in Amperes
Amount of flowing water
Voltage – Potential
Measured in Volts
Water Pressure
 If the voltage in a circuit increases,
the current will increase.
 If the voltage in a circuit decreases,
the current will decrease.
 This is a direct proportional
relationship.
Resistance and Current
 If the resistance in a circuit
increases, the current will
decrease.
 If the resistance in a circuit
decreases, the current will
increase.
 This is an inversely proportional
relationship.
OHM’S Law:
 State the relationship between
current, voltage, and resistance.
 German physicist George Ohm had
the law named after him, because of
his extensive research.
V=IR
Ohm’s Law
Voltage is equal to the current multiplied by
the resistance.
Voltage,
measured in
Volts, V
Current, measured
in Amps, A
Resistance,
measured in
Ohms, Ω
Ohm’s Law Examples…
If you want to find
Voltage in Volts:
V = IR
If I= 2 A and R = 5 Ohms
Then, V= (2A)(5Ω) = 10 V
Examples…
If you want to find Resistance in
Ohm’s:
R = V / I
If V = 9 Volts and I = 4 A
Then R = 9 V/ 4A = 2.25 Ω
Electrical Machine:
Conductance, G
 Conductance is the reciprocal of resistance
G = R-1 = i/v
Unit for conductance is S (siemens) or (mhos)
G = As/L
where s is conductivity,
which is the inverse of resistivity, 
Conductors and Insulators
 Conductors are those materials that permit a generous flow of
electrons with very little external force (voltage) applied
In addition,
 Good conductors typically have only one electron in the valance
(most distant from the nucleus) ring.
 Insulators are those materials that have very few
free electrons and require a large applied
potential (voltage) to establish a measurable
current level
 Insulators are commonly used as covering for
current-carrying wire, which, if uninsulated, could
cause dangerous side effects
 Rubber gloves and rubber mats are used to help
insulated workers when working on power lines
 Even the best insulator will break down if a
sufficiently large potential is applied across it
Semiconductors
 Semiconductors are a specific group of elements that
exhibit characteristics between those of insulators and
conductors
 Semiconductor materials typically have four electrons
in the outermost valence ring
 Semiconductors are further characterized as being
photoconductive and having a negative temperature
coefficient
 Photoconductivity: Photons from incident light can increase
the carrier density in the material and thereby the charge flow
level
 Negative temperature coefficient: Resistance will decrease
with an increase in temperature (opposite to that of most
conductors)
Ammeters and Voltmeters
 Ammeter (Millimeters or Micro ammeter)
 Used to measure current levels
 Must be placed in the network such that the
charge will flow through the meter
 Voltmeter
 Used to measure the potential difference between
two points
 Volt-ohm-milliammeter (VOM) and digital
multimeter (DMM)
 Both instruments will measure voltage and current and a third
quantity, resistance
 The VOM uses an analog scale, which requires interpreting the
position of the pointer on a continuous scale
 The DMM provides a display of numbers with decimal point accuracy
determined by the chosen scale.
Applications
 Flashlight
 Simplest of electrical circuits
 Batteries are connected in series to provide a
higher voltage (sum of the battery voltages)
Applications
 12-V Car battery charger
 Used to convert 120-V ac outlet power to dc charging power for
a 12-V automotive battery, using a transformer to step down the
voltage, diodes to rectify the ac (convert it to dc), and in some
cases a regulator to provide a dc voltage that varies with level of
charge.
Applications
 Answering machines/Phones dc supply
 A wide variety of devices receive their dc
operating voltage from an ac/dc conversion
system
 The conversion system uses a transformer to step
the voltage down to the appropriate level, then
diodes “rectify” the ac to dc, and capacitors
provide filtering to smooth out the dc.
Kirchhoff’s Current Law (KCL)
 The sum of currents entering any point in a circuit is equal to the sum of currents leaving
that point.
 Otherwise, charge would accumulate at the point, reducing or obstructing the
conducting path.
 The algebraic sum of currents entering a node is zero
 Add each branch current entering the node and subtract each branch current leaving
the node
 Σ currents in - Σ currents out = 0
 Or Σ currents in = Σ currents out
 Kirchhoff’s Current Law may also be stated as
IIN = IOUT
AND





nodenode
1
0
leaveenter
N
n
n
ii
i Where N is the total number of
branches connected to a node.
Kirchhoff's Voltage Law
(KVL)
 The algebraic sum of voltages around each loop
is zero
 Beginning with one node, add voltages across
each branch in the loop (if you encounter a + sign
first) and subtract voltages (if you encounter a –
sign first)
 Σ voltage drops - Σ voltage rises = 0
 Or Σ voltage drops = Σ voltage rises
Kirchhoff’s Voltage Law
 Or KVL for short
 Based upon conservation of energy – the algebraic
sum of voltages dropped across components
around a loop is zero.
 




risesdrops
M
1m
vv
0v Where M is the total number of
branches in the loop.
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  • 1.
    1. Circuit (1) 2.Charge (3-5) 3. Voltage (6-15) 4. Current (16-22) 5. Resistance (23-29) 6. Current and voltage (30-31) 7. Resistance and current (32) 8. Ohm’s Law (33-38) 9. Electrical machine (39-40) 10. Conductor and Insulator (42-44) 11. Semiconductor (45) 12. Ammeter and voltmeter (46-50) 13. Single phase and Triple phase (51-55) 14. KVL and KCL (56- 62) 15. Resistance in series and parallel (63-65) Basic Electrical Engineering (MID COURSE) By Engr Sharif Ur Rahman Sharif Arain
  • 2.
    Circuits  Closed Circuit Allows a complete path for electrons to travel  Open Circuit  Does not allow a complete path for the electrons to travel
  • 3.
    Flow of Charge When the ends of an electric conductor are at different electric potentials (voltages) Charge continues to flow until the ends of the conductor has the same voltage
  • 4.
    Charge  Electrical propertyof atomic particles  Electrons are negatively charged  Protons are positivity charged  The absolute value of the charge on an electron is 1.6x10- 19 C  The symbol used is Q or q
  • 5.
  • 7.
    Alessandro Volta (1745– 1827)  Italian physicist  known especially for the invention of the electrochemical cell, aka the battery in 1800.
  • 8.
    Voltage  The flowof charge is established by an external “pressure” derived from the energy that a mass has by virtue of its position: Potential energy  Energy: the capacity/ability of to do work 1. Kinetic energy: Energy an object has due to its motion 2. Potential energy  If a mass (m) is raised to some height (h) above a reference plane, it has a measure of potential energy expressed in joules (J) that is determined by  W (potential energy) = mgh where g is the gravitational acceleration (9.8 m/s2) o Energy that is stored o Potential energy due to an object’s position
  • 9.
    Explanation:  Potential differencebetween two points  Either side of a voltage source is not an eqipotential surface  A wire is an equipotential surface  It has the same potential  If the wire is attached to a voltage source it is still an equipotential surface
  • 10.
    Equation:  The electromotiveforce (emf) that causes charge to move.  1 Volt = 1 Joule/1 Coulomb Q W V dq dw    ;v
  • 11.
     Note:  Apotential difference or voltage is always measured between two points in the system.  Changing either point may change the potential difference between the two points under investigation.  Potential difference between two points is determined by: V = W/Q (volts)
  • 12.
    Voltage unit define: A potential difference of 1 volt (V) exists between two points if 1 joule (J) of energy is exchanged in moving 1 coulomb (C) of charge between the two points  The unit of measurement volt was chosen to honor Alessandro Volta
  • 13.
    Summary  The appliedpotential difference (in volts) of a voltage source in an electric circuit is the “pressure” to set the system in motion and “cause” the flow of charge or current through the electrical system.
  • 14.
    Ideal Voltage Sources Independent voltage source outputs a voltage, either dc or time varying, to the circuit no matter how much current is required.
  • 15.
    Note:  Potential difference:The algebraic difference in potential (or voltage) between two points of a network.  Voltage: When isolated, like potential, the voltage at a point with respect to some reference such as ground.  Voltage difference: The algebraic difference in voltage (or potential) between two points of a system. A voltage drop or rise is as the terminology would suggest.  Electromotive force (emf): The force that establishes the flow of charge (or current) in a system due to the application of a difference in potential.
  • 16.
    Current  “The flowof free electron in a copper wire or any other solid conductor of electricity”  With no external forces applied, the net flow of charge in a conductor in any one direction is zero  Basic electric circuit  Charge will only flow if there is a voltage source (potential difference).  The flow of electric charge  The loosely bound outer electrons of conductors carry the charge through circuits  Protons tightly bound to the nuclei of atoms
  • 17.
    André Ampère (1775– 1836)  French physicist and mathematician.  One of the main discoverers of electromagnetism.  SI unit of measurement of electric current, the ampere, is named after him.
  • 18.
    Equation/formula:  The flowof charge through a cross-sectional area as a function of time or the time rate of change of charge  Symbol used is I or i )(; ; 12 2 1 ttIQdtiQ t Q I dt dq i t t     
  • 19.
    current = charge/ time or I = q/t Units: Amps (A) An amp is the flow of 1 C of charge per second NOTE: 1 C = the charge of 6,240,000,000,000,000,000 electrons
  • 20.
    Current’s Direction  ElectronsTravel from – to +  Current is actually the opposite direction of the flow of electrons
  • 21.
    Current Sources  Anideal current source outputs a dc or ac current to the circuit no matter how much voltage is required.  There are no ideal current sources as all known current sources are unable to generate an unlimited force (voltage) that is needed to deliver a constant current to a circuit.
  • 22.
    Summary  Safety considerations Even small levels of current through the human body can cause serious, dangerous side effects  Any current over 10 mA is considered dangerous  currents of 50 mA can cause severe shock  currents over 100 mA can be fatal  Treat electricity with respect – not fear
  • 23.
    Electric Resistance  “Theability of a material to resist the flow of charge”  Units: Ohms (W)  The amount of charge that flows through a circuit depends on two things: 1. Voltage provided by source 2. Electric resistance of the conductor  opposes the push from the voltage source.  Resistance affects the speed of the current.
  • 24.
    Georg Ohm (1789– 1854)  German physicist  Ohm determined that there is a direct proportionality between the voltage applied across a conductor and the electric current.  This relationship is known as Ohm's law.
  • 25.
    Equation:  Resistance takesinto account the physical dimensions of the material where:  L is the length of conductor along which the carriers are moving  A is the cross sectional area of the conductor that the free electron move through.  ρ is the specific resistivity of a material A L R 
  • 27.
    Resistivity,   Resistivityis a material property  Dependent on the number of free electron or mobile charges (usually electrons) in the material.  In a metal, this is the number of electrons from the outer shell that are ionized and become part of the ‘sea of electrons’  Dependent on the mobility of the charges  Mobility is related to the velocity of the charges.  It is a function of the material, the frequency and magnitude of the voltage applied to make the charges move, and temperature.
  • 28.
    Resistivity of CommonMaterials at Room Temperature (300K) Material Resistivity (W-m) Usage Silver 1.64x10-8 Conductor Copper 1.72x10-8 Conductor Aluminum 2.8x10-8 Conductor Gold 2.45x10-8 Conductor Carbon (Graphite) 4x10-5 Conductor Germanium 0.47 Semiconductor Silicon 640 Semiconductor Paper 1010 Insulator Mica 5x1011 Insulator Glass 1012 Insulator Teflon 3x1012 Insulator
  • 29.
    Electric Resistance Factors Thickwires have less resistance than thin wires Short wires have less resistance than long wires Higher temperatures usually cause more resistance The resistance in some materials becomes almost zero at very low temperatures
  • 30.
    Current vs. Voltage Current– Flow rate Measured in Amperes Amount of flowing water Voltage – Potential Measured in Volts Water Pressure
  • 31.
     If thevoltage in a circuit increases, the current will increase.  If the voltage in a circuit decreases, the current will decrease.  This is a direct proportional relationship.
  • 32.
    Resistance and Current If the resistance in a circuit increases, the current will decrease.  If the resistance in a circuit decreases, the current will increase.  This is an inversely proportional relationship.
  • 33.
    OHM’S Law:  Statethe relationship between current, voltage, and resistance.  German physicist George Ohm had the law named after him, because of his extensive research.
  • 36.
    V=IR Ohm’s Law Voltage isequal to the current multiplied by the resistance. Voltage, measured in Volts, V Current, measured in Amps, A Resistance, measured in Ohms, Ω
  • 37.
    Ohm’s Law Examples… Ifyou want to find Voltage in Volts: V = IR If I= 2 A and R = 5 Ohms Then, V= (2A)(5Ω) = 10 V
  • 38.
    Examples… If you wantto find Resistance in Ohm’s: R = V / I If V = 9 Volts and I = 4 A Then R = 9 V/ 4A = 2.25 Ω
  • 39.
  • 42.
    Conductance, G  Conductanceis the reciprocal of resistance G = R-1 = i/v Unit for conductance is S (siemens) or (mhos) G = As/L where s is conductivity, which is the inverse of resistivity, 
  • 43.
    Conductors and Insulators Conductors are those materials that permit a generous flow of electrons with very little external force (voltage) applied In addition,  Good conductors typically have only one electron in the valance (most distant from the nucleus) ring.
  • 44.
     Insulators arethose materials that have very few free electrons and require a large applied potential (voltage) to establish a measurable current level  Insulators are commonly used as covering for current-carrying wire, which, if uninsulated, could cause dangerous side effects  Rubber gloves and rubber mats are used to help insulated workers when working on power lines  Even the best insulator will break down if a sufficiently large potential is applied across it
  • 45.
    Semiconductors  Semiconductors area specific group of elements that exhibit characteristics between those of insulators and conductors  Semiconductor materials typically have four electrons in the outermost valence ring  Semiconductors are further characterized as being photoconductive and having a negative temperature coefficient  Photoconductivity: Photons from incident light can increase the carrier density in the material and thereby the charge flow level  Negative temperature coefficient: Resistance will decrease with an increase in temperature (opposite to that of most conductors)
  • 46.
    Ammeters and Voltmeters Ammeter (Millimeters or Micro ammeter)  Used to measure current levels  Must be placed in the network such that the charge will flow through the meter  Voltmeter  Used to measure the potential difference between two points
  • 47.
     Volt-ohm-milliammeter (VOM)and digital multimeter (DMM)  Both instruments will measure voltage and current and a third quantity, resistance  The VOM uses an analog scale, which requires interpreting the position of the pointer on a continuous scale  The DMM provides a display of numbers with decimal point accuracy determined by the chosen scale.
  • 48.
    Applications  Flashlight  Simplestof electrical circuits  Batteries are connected in series to provide a higher voltage (sum of the battery voltages)
  • 49.
    Applications  12-V Carbattery charger  Used to convert 120-V ac outlet power to dc charging power for a 12-V automotive battery, using a transformer to step down the voltage, diodes to rectify the ac (convert it to dc), and in some cases a regulator to provide a dc voltage that varies with level of charge.
  • 50.
    Applications  Answering machines/Phonesdc supply  A wide variety of devices receive their dc operating voltage from an ac/dc conversion system  The conversion system uses a transformer to step the voltage down to the appropriate level, then diodes “rectify” the ac to dc, and capacitors provide filtering to smooth out the dc.
  • 58.
    Kirchhoff’s Current Law(KCL)  The sum of currents entering any point in a circuit is equal to the sum of currents leaving that point.  Otherwise, charge would accumulate at the point, reducing or obstructing the conducting path.  The algebraic sum of currents entering a node is zero  Add each branch current entering the node and subtract each branch current leaving the node  Σ currents in - Σ currents out = 0  Or Σ currents in = Σ currents out  Kirchhoff’s Current Law may also be stated as IIN = IOUT AND      nodenode 1 0 leaveenter N n n ii i Where N is the total number of branches connected to a node.
  • 59.
    Kirchhoff's Voltage Law (KVL) The algebraic sum of voltages around each loop is zero  Beginning with one node, add voltages across each branch in the loop (if you encounter a + sign first) and subtract voltages (if you encounter a – sign first)  Σ voltage drops - Σ voltage rises = 0  Or Σ voltage drops = Σ voltage rises
  • 60.
    Kirchhoff’s Voltage Law Or KVL for short  Based upon conservation of energy – the algebraic sum of voltages dropped across components around a loop is zero.       risesdrops M 1m vv 0v Where M is the total number of branches in the loop.