Fund. of. Electronics Ch02 Diodes

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    Fundamentals Of Electronic Circuits

    Chapter 2:

    Semiconductors, PN Junction and

    o es

    Associate Prof. Dr. Soliman Mahmoud

    Electrical and Computer Engineering Department

    1

    . .

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    Chapter(2)

    ,Diodes

    Objectives and outline:

    1. Conductivit of Solids

    2. Semiconductors

    . pn unc on4. Diodes

    5. Diode applications

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    1. Conductivit of Solids

    Conductivit is the abilit of a material to carr

    an electrical current.

    ,

    1. Good conductor: very low resistance (metals)

    . oor con uc or or nsu a or : very gresistance (ceramics, oxides)

    3.Semiconductor: somewhere in between

    (silicon, germanium, gallium arsenide)

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    2. Semiconductors

    valence of four. This means an isolateda om o e ma er a as our e ec rons n

    its valence orbit.

    Conductors have 1 valence electrons,

    electrons and Insulators have 8 valence

    .

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    2.1 Silicon atom

    used semiconductor.

    An isolated atom has

    pro ons anelectrons as shown:

    Valence orbit with 4 electrons

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    2.2 intrinsic ure semiconductors

    properties:

    No impurities only covalent

    bonds.

    All bonds complete at 0K.

    Part of electrons from covalentbonds is released at higher

    .

    valence bonds model

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    2.3 Do in of semiconductors

    One wa to increase conductivit of a semiconductoris by doping.

    Doping This means adding impurity atoms to an intrinsic crystal to alter its

    electrical conductivity. A doped semiconductor is called anextrinsic semiconductor.

    some materials form an excess of electrons and produce an n-type semiconductor

    some materials form an excess of holes and roduce a -t esemiconductor

    both n-type and p-type materials have much greater conductivitythan ure semiconductors

    this is extrinsic conduction.

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    n-t e semiconductors

    ,

    pentavalent atoms are added to the pure.

    Pentavalent atoms include 5 electrons in

    the valence orbit( ex: Phosphorus atoms).

    extra electron to the silicon crystal, they

    are o en re erre o as onor mpur es.

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    n-t e semiconductors contd.

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    -t e semiconductors

    By using a trivalent impurity, one whose

    atoms have onl 3 valence electrons(ex:Boron).

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    p-type semiconductors (contd.)

    By using a trivalent impurity, one whose atoms haveonly 3 valence electrons (ex:Boron).

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    3. pn Junction

    - -joined, this forms apnjunction

    the ma orit char e carriers on

    each side diffuse across the

    junction where they combine withan remove e c arge carr ers o

    the opposite polarity.

    ,

    are few free charge carriers and wehave a depletion layer(also called

    a space-c arge ayer.

    The diffusion of positive charge in one

    direction and negative charge in theo er pro uces a c arge m a ance

    this results in a potential barrieracross the junction.

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    3.1 Isolated n JunctionPotential barrier the barrier opposes the flow

    o ma or y c arge carr ersand only a small number

    have enough energy to.

    This generates a smalldiffusion current.

    flow of minoritycarriers andany that come close to it willbe swept over

    This generates a smalldrift current.

    for an isolated junctionese wo curren s musbalance each other and thenet current is zero.

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    3.2 Forward bias n JunctionsForward bias

    if the p-type side is madepositive with respect to then-type side the height of the

    barrier is reduced

    have sufficient energy tosurmount it

    increases while the driftcurrent remains the same

    there is thus a net current flowacross the junction whichincreases with the applied

    voltage.

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    3.3 Reverse bias n Junction

    Reverse bias -

    with respect to then-type side the height of thebarrier is increased

    the number of majority chargecarriers that have sufficient energyto surmount it rapidly decreases

    e us on curren ere orevanishes while the drift currentremains the same

    leakage current caused by the(approximately constant) drift

    current the leakage current is usually

    negligible (a few nA).

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    3.4 n Junction Currents

    pnjunction current is given approximately by

    = 1expT

    s

    VII

    , Te is the electronic charge, Vis the applied voltage, k is

    Boltzmanns constant T is the absolute tem erature

    and (Greek lettereta) is a constant in the range 1 to

    2 determined by the junction material for most purposes we can assume =1.

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    3.4 n Junction Currents contd.

    Thus,

    1expeV

    II s

    at room temperature e/kT~ 40 V1

    If V> + 0.1 V,eV

    If V< 0.1 V,

    s skT

    IS is the reverse saturation current.

    ( ) ss

    III = 10

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    4. Diodes

    n ea o e passes e ec r c y n one rec on

    but not in the other.

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    4. Diodes contd.

    One a lication of diodes is in rectification

    the example below shows a half-wave rectifier.

    In practice, no real diode has ideal characteristics

    diodes.

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    4.1 Semiconductor diodes

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    4.1 Silicon diodes

    -

    device

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    4.2 Diode e uivalent circuits

    Sometimes we re resent a diode b an

    equivalent circuit. Models have different levels of

    so histication.

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    4.3 Diode circuit anal sis

    The non-linear behaviour of diodes makes anal sisdifficult consider this simple circuit.

    Applying Kirchoffs voltage law VVE RD+=IRVD+=

    From the diode equation

    expS D

    =

    these twosimultaneous

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    equations.

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    4.4 Diode circuit anal sis contd.

    One approach is through the use of a load line.

    VVE RD+=

    D

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    4.4 Diode circuit anal sis contd.

    circuits

    however, this is rarely done, since if an equivalentcircuit is used, the circuit can normally be analysed

    directly, without resorting to a graphical method.

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    4.4 Diode circuit anal sis

    VEI

    ON= ON

    rR

    VEI

    +

    =

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    4.5 Zener breakdown diode: Symbol

    Model for the zener diode.Circuit symbol for a

    zener diode.

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    5.Diode circuitsHalf-wave

    (AC DC)

    peak output

    voltage is equal to

    e pea npu

    voltage minus the

    of the diode

    used to produce a

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    .

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    5. Diode circuits contd.

    u -wave rec er

    use of a dioder ge re uces

    the time for which

    to maintain theoutput voltage

    and thus reduce

    the ripple voltage.

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