Basics Electricity

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    Physical laws

    Variables and units

    Electrical definitions

    Breaking techniques

    Types of networks

    Device functions

    A

    B

    C

    D

    E

    F

    Understand the basics of electricity March 20071

    UNDERSTAND THE BASICS OF ELECTRICITY

    Understand the basic laws andvocabulary of electricity

    Duration: 29 mn

    Expert: P. GIVORD / D. FULCHIRONPedagogy: F. FINCHELSTEINProduction: M. ALLAGNAT / E. RODRIGUES

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    Physical laws

    Variables and units

    Electrical definitions

    Breaking techniques

    Types of networks

    Device functions

    A

    B

    C

    D

    E

    F

    Understand the basics of electricity March 20072

    VARIABLES AND UNITS

    Variables and units

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    - multiples and sub-multiples of units

    Multiples

    103 106 109 1012k M G T

    kilo mega giga tera

    Sub-multiples

    10-3 10-6 10-9 10-12m n p

    milli micro nano pico

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    - international system of measurement units

    Base units

    Dimensional equation: examples

    Speed: LT-1 Acceleration: LT-2

    Force: MLT-2 Electric charge:IT Voltage:ML2T-3 I-1

    L length meter mM mass kilogram kg

    T time second sI electric current ampere A

    These variables form the base of all other units

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    - particular measurement units

    Length:

    1 centimeter = 0.3937 inch

    1 meter = 1.094 yards

    1 kilometer = 0.6214 mile

    Weight:

    1 gram = 15.4 grains

    1 kilogram = 2.2046 pounds

    1 metric ton = 0.9842 ton

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    - main variables and related units

    rs

    l

    U = R I

    R =

    force N Newtonenergy J Joulepower W Wattacceleration m / s2pressure Pa Pascalmoment of inertia kg.m2

    electric charge C Coulombvoltage V Voltelectric field V / mimpedance W ohmresistance Wreactance W

    inductance H Henrycapacitance F Faradmagnetic induction T Teslamagnetic field A / mmagnetic flux Wb Weberpermeability m H / mpermittivity e F / m

    conductance S Siemensresistivity W . mfrequency Hz Hertz (s-1)angular frequency rd / s

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    - sun - earth power emission

    10 TWhuman activity

    180.103 TW1400 W / m received

    200 TWphotosynthesis

    35 TW

    internal

    180.103TWre-emitted

    loss of

    mass:

    4.109kg /s

    390.1012TWradiation

    1000 nuclear reactors = 1 TW

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    Physical laws

    Variables and units

    Electrical definitions

    Breaking techniques

    Types of networks

    Device functions

    A

    B

    C

    D

    E

    F

    Understand the basics of electricity March 20078

    ELECTRICAL DEFINITIONS

    Electrical definitions

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    - voltages

    Equipment operating characteristics are defined by three voltagevalues:

    rated voltage

    service voltage

    rated insulation level

    overvoltage withstand at power frequency for one minute

    standardized impulse withstand voltage

    l

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    - voltages

    rated voltage

    rated insulation level rated impulse withstandvoltage

    STANDARD IEC VOLTAGES

    t

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    - currents

    Equipment

    rated normal current

    rated short-time withstand current

    The peak value of rated short-time withstand current is equal to2.5 times the rms value

    Network

    service current

    short-circuit current (or Isc)

    f

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    - frequency

    Two frequencies are commonly used in the world:

    50 Hz in Europe

    60 Hz in North America

    Some countries use both frequencies:

    Japan, Saudi Arabia...

    PHYSICAL LAWS

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    Physical laws

    Variables and units

    Electrical definitions

    Breaking techniques

    Types of networks

    Device functions

    A

    B

    C

    D

    E

    F

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    PHYSICAL LAWS

    Physical laws

    how is electrical energy produced?

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    - how is electrical energy produced?

    A magnet rotating near a circuit containing turns generatesalternating voltage (Lenz's law)

    e

    = magnetic flux

    e =dt

    d

    representation of an alternating variable

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    - representation of an alternating variable

    An alternating variable may be represented by a rotating vector anda sine wave

    3p/2

    q 02p

    p/2

    p0 p/2 p 3p/2 2p

    y = a sin qy y

    r

    q

    r

    qq

    rr

    q

    alternating current

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    I rms = Isc / 2

    - alternating current

    Root mean square (rms) value: the value of direct current thatwould give off the same energy by the Joule effect in a resistor

    0 q/w p/w 2p/w

    I

    t

    IscI rms

    i = Isc . sin wt

    ... The same thing applies to voltage

    Ohm's law applied to direct current

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    P in W

    in . m

    I in m

    S in m

    r

    - Ohm s law applied to direct current

    U = RI

    Wire resistance: R = l / s

    r = 1.8.10- .m copper

    r = 2.9.10- .m aluminumr = 100.10- .m nickel - chromium (alloy for resistors)

    I inA

    U inV

    R in

    U

    I R

    P = U I = R I = U / R

    Ohm's law applied to alternating current (AC)

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    - Ohm s law applied to alternating current (AC)

    z =impedanceof the AC curcuit with afrequency fw = 2 p f current angular frequency

    RL

    Ci

    u

    u = z . i in complex numbers

    equivalent circuit

    u

    z

    i

    X Z

    R

    z is a complex number,the real part of which is resistance Rand the imaginary part reactance X

    z = R + j.X z in Wwhere X = Lw - 1/ Cw X in WL: inductance in Henry f in HzC: capacitance in Farad

    Ohm's law applied to alternating current (AC)

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    - Ohm s law applied to alternating current (AC)

    z

    iu

    z = R + j X

    z = (Z , ) in polar formwhere Z2 = R2 + X2and tg = X / Rz = Z e j

    i = I e j w t

    u = z . i = Z.I ej

    . ej w t

    = Z.I e j(w t + ) = U e j(w t + )

    z

    i

    u

    U = ZIX

    R

    u = z . iin complex numbers

    - active power and reactive power

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    active power and reactive power

    P(t) = U(t) . I(t) = U . I sin(wt) sin(wt)

    P(t) = U . I cos (1 cos2 wt) + U . I sin sin (2 wt)

    The integral cycle shows:

    S = U.I apparent power in VA

    Q = U.I.sin reactive power in VARP = U.I.cos active power in W

    P Q

    - line losses and voltage drops

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    line losses and voltage drops

    Source Load

    Line

    z = R + j X

    V1 V2

    I

    The Joule effect depends only on R

    P I Rline= .2

    (in Watts)

    Depend on R and X

    D V = V1 - V2(in Volts)

    Line losses Voltage drops

    - law of impedance combination

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    law of impedance combination

    z1

    z2

    z = z1 + z2

    The impedances add up

    z1 z2

    1 / z = 1 / z1 + 1 / z2

    z = z1 . z2 / (z1 + z2)

    The admittances add up

    Series:

    Parallel:

    Admittance = reciprocal of impedance

    - three-phase diagram

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    V2 lagging behind V1

    3

    2p

    three phase diagram

    N

    Ph3

    Ph 2

    Ph1

    2V

    V3

    V1

    U23

    U12

    3

    2p

    3

    2p

    3

    p2

    U31

    V1, V2, V3: phase voltages

    U12, U23, U31: phase-to-phase voltages

    U12 = V2 - V1 in vectors

    In balanced three-phase operatingconditions,U = V . 3

    3 coils with phase

    displacement of 120 (2 p / 3)

    - why three-phase current?

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    why three phase current?

    The most economical way to transmit movement: minimum numberof coils to create a rotating magnetic field

    AC generator motor

    - three-phase power diagram

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    Apparent power

    S = U.I. in VA (= 3 VI)3

    Active power

    Pr = U.I. cos in W (= 3VI cos)3

    Pa

    Pr

    RII

    jXI

    p p g

    Reactive power

    Pr = U.I. sin in VAR3

    - Coulomb's law

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    q M Er4p e r2

    q

    E =

    Electric field created on M by a point charge q

    Interaction between two electric point charges

    q q' FdFq . q'

    F =

    4p e r2q in CE in Vr in md in me in F/m e0 = dielectric constant in a vacuum

    er

    = relative permittivity of ambient material

    Dielectric constant e = e0 . e re0 = 10

    -7 / 4 p c0 = 8.85 . 10-12 F / m

    Two charges of the same sign repel each otherTwo charges of the opposite sign attract each other

    - Kirchhoff's law

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    On a node

    S i = 0N

    A

    B

    C D

    E

    Around a loop

    S D u = 0

    - Ampre's law

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    p

    A continuous straight conductor, through which a current (I) flows,creates magnetic induction B in the surrounding space

    I

    B

    rMagnetic permeability m = m0.mrm0 = 4 p 10

    -7 = 12.6 .10-7 0 in H/m

    mr = 1 for vacuum, air, aluminum

    mr= 600 800 for iron

    e0. m0 . c02 = 1

    B in T

    I in A

    R in m

    m0 I

    div B = 0

    B =2pr

    -Laplace's law of force

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    Induction B exerts force F on a conductor through which a current(I) is flowing

    F = i . dl . B . sin aF = i . dl L B

    I

    B

    a

    F

    Right hand

    Thumb

    Middle finger

    Index finger

    - Lenz's law

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    A conductive circuit forms a ring around a surface through whichthe induction varies. The circuit is subjected to an electromotiveforce E along the circuit.

    B variable(increasing)

    E

    E = - d / dt

    - Ampre's and Laplace's laws

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    II

    Force of repulsion---> loop effect

    Proportional tothe product

    of the currentsI I

    Force of attraction

    - Lenz's and Laplace's laws

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    Circular currents induced in metal frames by a variation in magneticflux

    Aluminumdisk

    - calculation of voltage drop

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    Voltage drop in vectors V1 - V2 = z . I = (R + j.X).I

    As an absolute value, this is very close to AB = AH + HB

    Hence DV = R I cos + X I sin PLEASE NOTE: voltage drop may be negative....

    Source Load

    line

    z = R + jX

    V2

    Z , V1

    I

    D V

    V2 R.I

    A H B

    V1

    X.I

    I DV

    TYPES OF NETWORKS

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    Physical laws

    Variables and units

    Electrical definitions

    Breaking techniques

    Types of networks

    Device functions

    A

    B

    C

    D

    E

    F

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    Types of networks

    - different types of MV networks

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    Overhead or underground

    Two types of configuration

    Radial

    Loop

    - radial configuration

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    Substation

    Clusteredconnection

    Direct connection

    Substation

    - open loop configuration

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    substation substation substation

    - networks

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    - public network

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    LVconsumer

    MVconsumer(service sector,small industry)

    HVconsumer(heavy industry)

    EHVnational

    MVlocal

    LVlocal

    HVregional

    DEVICE FUNCTIONS

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    Physical laws

    Variables and units

    Electrical definitions

    Breaking techniques

    Types of networks

    Device functions

    A

    B

    C

    D

    E

    F

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    Device functions

    - safety functions: isolation, earthing

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    DESIGNATION FUNCTION Switching on/off Closing/breakingAND SYMBOL of service currents of fault current

    DisconnectorIsolate NO NO

    Earthing switch

    Isolate NO NO(capable ofclosing on

    short-circuit)

    - control functions

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    NO

    DESIGNATION FUNCTION Switching Closing and breakingAND SYMBOL on/off of of fault currents

    service currents

    YESSwitch on / off

    not isolate

    SwitchNO

    NOYESSwitch on / offnot isolate

    DisconnectorNO

    NOYESSwitch on / offnot isolate

    NOContactor

    - protection functions

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    Protectnot isolate YES

    (once)

    NOFuse

    Switch on / off

    Protect - isolatein "disconnected"

    position

    DESIGNATION FUNCTION Switching on-off Closing and breaking

    AND SYMBOL the service currents the faulted currents

    Protectnot isolate

    YES YESFixed circuit breaker

    DESIGNATION FUNCTION Switching on/off Closing and breakingAND SYMBOL of service currents of fault currents

    YESYESWithdrawable circuit-breaker

    BREAKING TECHNIQUES

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    Physical laws

    Variables and units

    Electrical definitions

    Breaking techniques

    Types of networks

    Device functions

    A

    B

    C

    D

    E

    F

    Understand the basics of electricity March 200744

    Breaking techniques

    - the electric arc

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    An arc is created when the voltage between two conductors isgreater than the maximum dielectric withstand of the mediumbetween the conductors

    Irreversible deterioration in solid insulating materials

    Ionization of the medium between the contacts air

    SF6 gas

    oil vacuum: vaporization of metal on the contacts

    The ionized insulating medium becomes temporarily conductive

    Presence of an arc voltage according to the ionized medium andthe type of electrodes

    - the "puffer" technique

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    Movingcontact

    Fixed

    contact

    I

    Flow ofcurrent

    Separationof contacts &

    arcing

    Lengtheningof the arc &

    blow-out

    Extinction of the arcwhen the current

    reaches zero

    - the vacuum technique

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    Movingcontact

    Fixedcontact

    I

    Flow of

    currentInitial

    AMF

    Diffuse

    U net

    RMF

    Constricted

    Control of the arc Interruption

    - end of the module

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    Thank you for your attentionAnd don't hesitate to discover: