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    Basics about Circuits

    Basic Electric Circuit Concepts

    System of Units:

    We use the SI (System International) units. The system uses meters (m),

    kilograms (kg), seconds (s), ampere (A), Resistance (? ) & Volts (V)

    as the fundamental units.

    We use the following prefixes:

    pica (p): 10-12

    nano (n): 10-9

    micro (): 10-6

    milli (m): 10-3

    tera (T): 1012

    giga (G) : 109

    mega (M): 106

    kilo (k): 103

    1

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    Basic Electric Circuit Concepts

    Basic Quantities: Current

    The unit of current is the ampere (A). We note that

    1 ampere = 1 coulomb/second

    We normally refer to current as being either direct (dc) or

    alternating (ac).

    i(t)i(t)

    t t

    dc currentac current

    0 0.5 1 1 . 5 2 2 .5 3 3.5-1

    -0.8

    -0.6

    -0.4

    -0.2

    0

    0.2

    0.4

    0.6

    0.8

    1

    ac current3

    Basic Electric Circuit Concepts

    Basic Quantities: Current

    In solving for current in a circuit, we must assume a direction, solve

    for the current, then reconcile our answer. This is illustrated below.

    Circuit 1 Circuit 2

    (a) (b)

    I1 = 4 A I2= - 3 A

    In the diagram above, current I1 is actually 4 A as assumed. The

    actual positive direction of current I2 (equal to -3 A) in the opposite

    direction of the arrow for I2.

    4

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    Basic Electric Circuit Concepts

    Basic Quantities: Voltage

    The next quantity of interest is voltage. Voltage is also called an

    electromotive force (emf). It is also called potential energy.

    Suppose one coulomb of charge is located at point b and one joule

    of energy is required to move the charge to point a. Then we say

    that Vab = 1 volt = 1 joule/coulomb = 1 newton.meter/coulomb.

    Vab = 1 volt states that the potential of point a (voltage at point a)

    is l volt (positive) with respect to point b.

    The sign associated with a voltage is also called its polarity.

    5

    Basic Electric Circuit Concepts

    Basic Quantities: Voltage

    As in the case for current, we must assume a positive direction (polarity) for

    the voltage. Consider the three diagrams below.

    .+

    -

    .

    v = 4 v

    a

    b

    vab = 4 v v = 4 v

    (a) (b) (c)

    Each of the above gives the same information.6

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    Basic Electric Circuit Concepts

    Basic Quantities:Voltage

    We need to keep in mind that we assume a polarity for the

    voltage. When we solve the circuit for the voltage, we may find

    that the actual polarity is not the polarity we assumed.

    +

    -

    v = -6 v

    The negative sign for 6 v indicates that if

    the red lead(probe) of a voltmeter is

    placed on + terminal and the black

    lead(probe) on the terminal the meter

    will readdownscale or6v.

    Adigital meter would read 6 v.7

    Basic Electric Circuit Concepts

    Circuit Elements:

    We classify circuit elements as passive and active.

    Passive elements cannot generate energy. Common examples

    of passive elements are resistors, capacitors and inductors. We

    will see later than capacitors and inductors can store energy

    but cannot generate energy.

    Active elements can generate energy. Common examples of

    active elements are power supplies, batteries, operational

    amplifiers.

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    circuits

    Fundamentals

    Introduction to Electronics

    (Semiconductor Devices)

    Why Semiconductors?

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    Ge has 32 orbiting electrons andneutrons and protons in Nucleus

    Bohr Atomic Model of Ge

    Nucleus

    1st shell electrons

    2nd shell electrons

    3rd shell electrons

    4th and Valence shell electrons

    Bohr Atomic Model of Si

    Si has 14 orbiting electrons andneutrons and protons in Nucleus

    Nucleus

    1st shell electrons

    2nd shell electrons

    3rd shell and Valence shell

    electrons

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    E

    E

    The characteristics of a semiconductor

    material can be altered significantly bythe addition of certain impurity atoms

    into the relatively pure semiconductor

    material.

    Terms: Doping, impurity, intrinsic

    semiconductor

    A semiconductor material that has been subjected to the

    doping process is called as an Extrinsic

    Materials

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    Intrinsic Semiconductor Materials

    Free electrons in an intrinsic semiconductorare only due to natural causes (photon lightand thermal heating). A free electron willhave its complementary hole. Electrons andholes due to only natural causes are alsocalled as intrinsic carriers.

    Extrinsic Semiconductor

    Base Material

    (Si and Ge)

    Impurity Pentavalentor Trivalent

    Base Material+Pentavalent impurity n-typesemiconductor

    Base Material+Trivalent impurity p-typesemiconductor

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    Trivalent Impurity (p-type impurity)

    Boron (B), Gallium (Ga) and Indium:

    have 3 electrons in valence cellAcceptor impurity

    Pentavalent Impurity(n-type impurity)

    Antimony (Sb), Arsenic (As) and

    Phosporous (P) : have 5 electron in valence

    shell Donar Impurity

    P NJunction

    Doping a crystal with both types of impurities forms a

    P-N junction diode.

    Some electrons will cross the junction and fill holes.A pair of ions is created each time this happens.

    Negativeion

    Positiveion

    As this ion charge builds up, it prevents furthercharge migration across the junction.

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    P N

    Each electron that migrates across the

    junction and fills a hole effectivelyeliminates both as current carriers.

    This results in a region at the junction that isdepleted of carriers and acts as an insulator.

    Depletion layer

    Energy

    Abrupt junction

    P-side

    Valence band

    Conduction band

    N-side

    In an abrupt junction, the p side bandsare at a slightly higher energy level.

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    Energy

    P-side

    Valence band

    N-side

    Conduction band

    Energy bands after the depletion layer has forme

    To an electron trying to diffuse across the junctiothe path it must travel looks like an energy hill. It

    must receive the extra energy from an outside sour

    Energy hill

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    Diode Types

    Rectifier Diodes

    Light Emitting Diodes (LED)

    Photodiodes

    Zener Diodes, etc

    Diode Applications

    Against Reverse Voltage Protection

    Rectifying {AC DC }

    Display (indicators, Advertise hoardings)

    Light Sensing (Solar panals etc)

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    Light Emitting Diode (LED) circuit How to connect LED

    A

    K

    V s

    VR

    R

    V

    ILED

    Expected ILED = 20mA,

    Assuming LED has V =1.5V.

    Find the value of R, if the source

    voltage 5 volts.

    LED

    S

    I

    VVR

    =

    7 Segment Display Consist of 7+1 LEDs Available in :

    Commond Anode configuration

    Commond Cathode configuration

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    7 Segment Display Commond anode and Commond

    Cathode configuration

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    7 Segment Display

    Commond anode and CommondCathode configuration

    7 Segment Display Application: Logic Display

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    Classification of TransistorsTRANSISTORS

    Bipolar Junction

    Transistors

    (BJT)

    Field Effect

    Transistors

    (FET)

    NPN - B JT PNP - B JTJunction

    FET (JFET)

    Metal Oxyde

    Semiconductor FET

    (MOSFET)

    N-Channel

    JFET

    P-Channel

    JFET

    DepletionMode

    MOSFET

    EnhancedMode

    MOSFET

    N-Channel

    D-MOSFET

    P-Channel

    D-MOSFET

    N-Channel

    E-MOSFET

    P-Channel

    E-MOSFET

    A bipolar (junction) transistor (BJT) is athree-terminal electronic device constructed

    of doped semiconductor material and may

    be used in amplifying or switchingapplications. Bipolar transistors are so

    named because their operation involves

    both electrons and holes.

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    Classification of Bipolar Junction

    Transistors

    Base

    Collector

    Emitter

    IC

    IB

    IE

    VCE

    VBE

    Base

    Collector

    Emitter

    IC

    IB

    IE

    VCE

    VBE

    Bipolar Junction Transistor (BJT)

    NPN Transistor PNP Transistor

    ass ca on o po ar unc onTransistors

    Base

    Collector

    Emitter

    IC

    IB

    IE

    V

    CE

    VBE

    NPN Transistor

    Current Gain : or hFE

    Then

    And

    So

    B

    C

    I

    I =

    BCII =

    CBE

    III +=

    ( )II BE += 1

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    NPN

    NPN is one of the two types of bipolar

    transistors, consisting of a layer of P-dopedsemiconductor (the "base") between two N-doped layers.

    A small current entering the base is

    amplified to produce a large collector andemitter current.

    That is, an NPN transistor is ON" when its

    base is pulled high relative to the emitter.

    PNP

    The other type of BJT is the PNP, consisting

    of a layer of N-doped semiconductorbetween two layers of P-doped material.

    A small current leaving the base is

    amplified in the collector output.

    That is, a PNP transistor is "on" when itsbase is pulled low relative to the emitter.

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    Applications of Transistors

    1. Darlington transistor (often called aDarlington pair) is a compound structureconsisting of two bipolar transistors (eitherintegrated or separated devices) connectedin such a way that the current amplified by

    the first transistor is amplified further by thesecondone

    2. Transistor As a Switch

    An electronic amplifier, in which the input " signal" is

    usually a voltage or a current. In audio applications,

    amplifiers drive the loudspeakers used in PA systemsto make the human voice louder or play recorded

    music.

    Amplifiers may be classified according to the input

    (source) they are designed to amplify (such as a guitar

    amplifier, to perform with an electric guitar), the

    device they are intended to drive (such as a headphone

    amplifier), the frequency range of the signals (Audio,

    IF, RF, and VHF amplifiers, for example), whether

    they invert the signal (inverting amplifiers and non-inverting amplifiers), or the type of device used in the

    amplificat ion (valve or t ube am plifier s, F ET

    amplifiers, etc.).

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    If for a small change in input voltage, a proportional

    large change in output voltage is obtained, then we say

    that, voltage amplification has taken place

    Biasing in Transistor

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    In order to use transistor as an amplifier, it must be operated in its

    active region. The biasing of the PNP and NPN transistor for theiractive region operation and the directions of the currents are

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    The field-effect transistor(FET), sometimes called aunipolar transistor, uses either electrons (in N-

    channel FET) or holes (in P-channel FET) forconduction.

    In FETs, the drain-to-source current flows via aconducting channel that connects the sourceregionto the drainregion.

    The conductivity is varied by the electric field that is

    produced when a voltage is applied between the gateand source terminals; hence the current flowingbetween the drain and source is controlled by thevoltage applied between the gate and source.

    N-CHANNELP-CHANNEL

    The four terminals of the FET are named source, gate,

    drain, andbody(substrate).

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    Operation of N-channel with VGS =0

    Due to the supply voltage VDS , current starts flowingthrough the channel.

    Therefore current flow through the channel get voltageacross the channel.

    This voltage will Reverse BIAS the G to S p-n junction

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    Thanks