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Basic Electrical Theory

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Title: Basic Electrical Theory


1
Chapter 1
  • Basic Electrical Theory

2
1.1 Introduction to Electrical Engineering
  • Electrical Engineering harnesses electrical
    energy for human good for transporting energy
    and information, for lifting the burdens of toil
    and tedium (motors).
  • Foundational Ideas in Electrical Engineering
  • 1. Conservation of charge (Kirchhoffs current
    law) is one of the principles used in writing
    circuit equations.
  • 2. Conservation of energy (Kirchhoffs voltage
    law) is one of the fundamental principles used in
    writing circuit equations, and conservation of
    energy.
  • 3. The frequency domain is a way of looking at
    the physical world in which frequency, not time,
    is the independent variable.

3
Foundational Ideas in Electrical Engineering
  • 4. Equivalent circuits model real devices by
    ideal electrical devices that have identical or
    similar characteristics.
  • 5. Impedance level determines how electrical
    devices interact.
  • 6. Feedback is a technique for bringing part of
    the output of an electronic device back to the
    input to improve performance.
  • 7. Analog information uses an electrical signal
    proportional to the information content.
  • 8. Digital information uses a two-valued code to
    represent the information content.

4
Circuit Theory
  • Practically every electrical device is a circuit.
  • A radio is a circuit, as is the power
    distribution system that runs your lights and air
    conditioner.
  • Hence, understanding of the methods of circuits
    opens the door to all the areas of electrical
    engineering.

5
1.2 Physical Basis of Circuit Theory
  • Charge, like mass, is a property of matter.
  • The unit of electric charge is the coulomb (C),
    named in honor of Charles de Coulomb.
  • There are two types of charge, positive and
    negative.
  • Traditionally the electron has been assigned a
    negative sign, and the proton a positive.
  • The magnitude of the charge on an electron is
  • e - 1.602 X 10-19 coulombs (C)

6
1.2 Physical Basis of Circuit Theory
  • Forces between charges and Energy
  • Charges attract or repel each other due to
    electrostatic forces. Electrostatic forces are
    responsible for lightening.
  • Magnetic forces depend on moving charges
    (current). Magnetic forces turn motors, and
    effect energy conversion in generators.
  • Energy is the medium of exchange in a physical
    system, like money is in an economic system.
  • In mechanics, it takes force and movement to do
    work (exchange energy).
  • In electricity, it takes electrical force
    (voltage) and movement of charges (current) to do
    work (exchange energy).

7
1.2 Physical Basis of Circuit Theory
  • Circuit Theory
  • Consider a circuit consisting of a battery,
    light, switch, two headlights, and connecting
    wires and chassis from a car, as shown in fig
    1.1(page 6).
  • When we pull the switch, the lights will glow and
    get hot, which suggests the battery is supplying
    energy to the headlights.
  • Figure 1.2 (page 7) shows an electric circuit
    representing the physical situation shown in fig.
    1.1.
  • We can use circuit theory to calculate the
    current in the wires, the power out of the
    battery, and the power into each headlight.
  • The solution of an engineering problem normally
    proceeds through four stages First, a real world
    problem is identified second, the problem is
    modeled third, the model is analyzed and forth,
    the results are applied to the original physical
    problem.

8
1.3 Current and Kirchhoffs Current Law
  • Current is charge in motion.
  • Current I ?Q/ ?t C/s or ampere, A
  • To specify a current we require a reference
    direction plus a numerical value (fig 1.4, page
    8).
  • Velocity is the simplest mechanical analogy for
    electric current, and displacement would be
    analogous to charge accumulation.
  • q t1?t2i(t) dt coulombs fig 1.5, page 9.

9
1.3 Current and Kirchhoffs Current Law
  • Kirchhoffs Current Law
  • The sum of currents entering a node is equal to
    the sum of currents leaving the node.
  • i1 i2 i3 i4 - Fig 1.6, page 11.
  • Example 1.2, page 11
  • i1 i2 iL
  • 8 i2 12
  • I2 12 8 4 A

10
1.4 Voltage and Kirchhoffs Voltage Law
  • Voltage is defined as the potential for doing
    work. It measures how much work would be done by
    the electrical system in moving a charge from one
    point to another in a circuit, divided by the
    charge.
  • V ab work done by the electrical system in
    moving q from a to b / q
  • The unit is energy/charge, joules per coulomb or
    volt (V) to honor Count Volta.
  • Force is a mechanical analog for voltage.

11
1.4 Voltage and Kirchhoffs Voltage Law
  • Kirchhoffs voltage law The voltage sum around a
    closed loop is zero.
  • ?loop voltages 0
  • In writing KVL equations, we write the voltage
    with a positive sign if the is encountered
    before the and with a negative sign if the is
    encountered first as we move around the loop.
  • In fig 1.9, page 16 -12.6 vsw vL 0

12
1.5 Energy Flow in Electrical Circuits
  • Power is defined as the rate of energy exchange.
    Power is by definition the product of voltage and
    current.
  • v (work/charge) x i (charge /time)
    work/ time power (1.30)
  • The unit for power is watts (W).

13
1.5 Energy Flow in Electrical Circuits
  • Energy W t1?t2 p dt t1?t2 vab i dt Joules
  • Example 1.7, page 22
  • p vi 12.6 x 60 756 W
  • Energy W 0?10 p dt 10 p 7560 J

14
1.6 Circuit Elements Resistance and Sources
  • Ohms Law v iR or i v/R . (1.41)
  • R is the resistance and has a unit of volt per
    ampere, but we use the unit ohm to honor Ohm,
    abbreviated by the Greek letter omega, O .
  • The resistance of a piece of wire is directly
    proportional to its length to the property of the
    material called resistivity, and inversely
    proportional to its cross sectional area.
  • R ? l / A
  • Where ? (rho) the resistivity, l is the length,
    and A the area of the wire.
  • Table 1.1, page 24 Property of copper wires,
    gage size (smaller the gage size, higher the
    current limit).

15
1.6 Circuit Elements Resistance and Sources
  • Conductance
  • Is the reciprocal of resistance.
  • Conductance G 1 / R
  • The unit is Siemens (S) and symbol is mho (upside
    down O).
  • Power in resistance
  • p vi (R i) i i2R v ( v/R) v2 /R
    (1.44)
  • Do example 1.8, page 25.

16
1.6 Circuit Elements Resistance and Sources
  • Open circuits and short circuits
  • Fig 1.19, page 25.
  • A short circuit (R0) permits current to flow
    without any resulting voltage (v0).
  • An open circuit (R8) permits voltage with no
    current (i0).
  • In both cases eq. (1.44) shows that no power is
    required for the open or short circuit.

17
1.6 Circuit Elements Resistance and Sources
  • Switches
  • An ideal switch is a special resistance that can
    be changed from a short circuit to an open
    circuit to turn an electrical device ON or OFF.
  • Fig 1.20(a), page 26 shows a single pole, single
    throw switch in its open (OFF) state.
  • Fig 1.20(b) shows a single pole, double throw
    switch, which switches one input line between two
    output lines.
  • Fig 1.20(c) shows a double pole, single throw
    switch the dashed line indicates mechanical
    coupling between the two components of the switch
    to cause simultaneous switching.
  • Switches can have any number of poles and throws.

18
1.6 Circuit Elements Resistance and Sources
  • Ideal voltage source
  • Fig 1.21, page 27 shows the circuit symbol,
    mathematical definition, and graphical
    characteristic of an ideal general and dc voltage
    source.
  • The ideal voltage source maintains its prescribed
    voltage, independent of its output current.

19
1.6 Circuit Elements Resistance and Sources
  • Ideal current source
  • Fig 1.22, page 27 shows the circuit symbol,
    mathematical definition, and graphical
    characteristic of an ideal general and dc current
    source.
  • The ideal current source maintains its prescribed
    current, independent of its output voltage.

20
1.6 Circuit Elements Resistance and Sources
  • Analysis of DC Circuits
  • Headlight circuit fig 1.24, page 29.
  • Going clockwise around the left loop
  • -12.6 vsw vL 0
  • KVL clockwise around the loop created by the
    resistors is
  • - vL vR 0
  • We must solve these equations for two cases the
    switch open (OFF) and the switch closed (ON).
  • With the switch OFF no current flows, vL vR
    0 and
  • -12.6 vsw 0 0. So vsw 12.6 V
  • With the switch ON vsw 0, and we get vL vR
    12.6V
  • The current iL vL/ RL 12.6 V/ 5.25 O 2.40 A
    iR
  • Current in the battery Applying KCL iL iR
    iB 2.4 2.4 4.8A
  • The power out of the battery pout 12.6V X 4.8
    A 60.5 W
  • Power in each resistance pL pR 12.6 V X 2.4
    A 30. 25 W

21
1.7 Series and Parallel Resistances Voltage and
Current Dividers
  • Series Resistances and Voltage Dividers
  • Two circuit elements are connected in series when
    the same current flows through them.
  • Fig 1.28, page 33 shows a series connection of
    three resistances and a battery.
  • We can write KVL around the loop going clockwise
  • -Vs v1 v2 v3 0
  • Or Vs V1 v2 V3
  • Or Vs iR1 iR2 iR3 (using Ohms Law)
  • Vs (R1 R2 R3) I
  • Vs Req I
  • Resistances in series Req R1 R2 R3

22
1.7 Series and Parallel Resistances Voltage and
Current Dividers
  • Voltage Dividers
  • Current i Vs/ Req
  • Vi R1 X i R1 / Req X Vs .(1.66)
  • Where Req R1 R2 R3(for series circuits)
  • The circuit of fig 1.30, page 34 models a
    flashlight. Calculate the voltage across the 2.5
    O resistance representing the flashlight bulb
    (Vb) when the switch is closed.
  • Applying KVL - 1.5 0.3 i 1.5 .3 i Vsw
    2.5 i 0
  • With the switch closed
  • Vsw 0 and i 3.0/(0.3 0.3 2.5)
  • Vb 2.5 i 2.42 V

23
1.7 Series and Parallel Resistances Voltage and
Current Dividers
  • Parallel Resistances
  • Resistances are said to be connected in parallel
    when they have the same voltage across them.
  • Fig 1.31, page 36 shows a parallel combination of
    three resistances and a current source.
  • KCL for node A Is i1 i2 i3
  • Is v/R1 v/R2 v/R3
  • Is v ( 1/ R1 1/ R2 1/ R3)
  • Is v ( 1/ Req) where
  • 1/ Req 1/ R1 1/ R2 1/ R3
  • Req (1/ (1/ R1 1/ R2 1/ R3) ..(1.74)

24
1.7 Series and Parallel Resistances Voltage and
Current Dividers
  • Current Dividers (page 37)
  • V Req Is
  • i1 v/R1 Req Is/ R1
  • (1/R1 / 1/ R1 1/ R2 1/ R3) Is
  • In general
  • Ii 1/Ri / 1/ R1 1/ R2 1/ R3..) It
    (1.76)
  • Where It is the total current entering the
    parallel combination.
  • Example 1.11 page 37
  • Req (4 4) II (8 4) 4.8 O
  • Voltage across combination is 5 X 4.8 24 V

25
Home Work
  • 1. What is electrical engineering?
  • 2. What are the foundational ideas in electrical
    engineering?
  • 3. What is a circuit? Give examples.
  • 4. Explain energy. Give examples.
  • 5. What are the four stages to the solution of an
    engineering problem?
  • 6. What is current? Give its formula with units.
    What is its mechanical analog?
  • 7. Define Kirchhoffs current law.
  • 8. What is voltage? Give its formula with units.
    What is its mechanical analog?
  • 9. Define Kirchhoffs voltage law.
  • 10. What is power? Give its formula with units.
  • 11. What is energy? Give its formula with units.
  • 12. What is Ohms law.
  • 13. Explain conductance.
  • 14. What are the several ways to express power in
    resistance.
  • 15. Define open and short circuit.
  • 16. What is the formula for resistances in
    series?
  • 17. What is the formula for resistances in
    parallel?

26
Test Study Questions
  • 1. Page 19, problem 3.
  • 2. Page 23, problem 3.
  • 3. Page 33, problem 2.
  • 4. Page 40, problem 4.
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