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    Department of Electronics and Communication Engineering, MIT, Manipal

    Department of Electronics and Communication Engineering, MIT, Manipal 21

    ECE 1001 : BASIC ELECTRONICS

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Part I : Analog Electronics

    1

    CHAPTER-1: DIODES AND APPLICATONS

    Reference:

    Robert L. Boylestad, Louis Nashelsky, Electronic Devices &

    Circuit Theory, 11thEdition, PHI, 2012

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Module 1 : Diodes

    Learning outcomes

    At the end of this module, students will be able to: Explain the operation of PN junction diode under different biasing

    condition.

    Draw the I-V characteristic of diode and differentiate between ideal andpractical diodes

    Explain the concept of static and dynamic resistance of the diode.

    Explain various breakdown phenomenon observed in diodes.

    Describe the working of Zener diode and its I-V characteristic.

    Explain the operation of diode as capacitor.

    3

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Department of Electronics and Communication Engineering, MIT, Manipal 2

    Review

    Basic of Semiconductors

    Doping in Semiconductors

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Semiconductors

    5

    Common semicond uct ing mater ialsCrystal st ructure of s i l icon

    http://fourier.eng.hmc.edu/e84/le

    ctures/ch4/node1.htmlhttp://www.austincc.edu/HongXiao/overvie

    w/basic-semi/sld007.htm

    http://fourier.eng.hmc.edu/e84/lectures/ch4/node1.htmlhttp://fourier.eng.hmc.edu/e84/lectures/ch4/node1.htmlhttp://www.austincc.edu/HongXiao/overview/basic-semi/sld007.htmhttp://www.austincc.edu/HongXiao/overview/basic-semi/sld007.htmhttp://www.austincc.edu/HongXiao/overview/basic-semi/sld007.htmhttp://www.austincc.edu/HongXiao/overview/basic-semi/sld007.htmhttp://www.austincc.edu/HongXiao/overview/basic-semi/sld007.htmhttp://www.austincc.edu/HongXiao/overview/basic-semi/sld007.htmhttp://fourier.eng.hmc.edu/e84/lectures/ch4/node1.htmlhttp://fourier.eng.hmc.edu/e84/lectures/ch4/node1.html
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    Department of Electronics and Communication Engineering, MIT, Manipal

    Doping in Sem iconductors

    6

    Schemat ic o f a si l icon crys tal latt ice doped with impu r i t ies to

    produ ce n- type and p -type semico ndu ctor material .

    [ht tp: / /www.pveducat ion.org/pvcdrom/pn- junct ion/dopingl] .

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    Self test

    7

    1.Why silicon is preferred over germanium for

    semiconductor devices?

    2.List different elemental and compound semiconductors.

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    P-N Junct ion Diode

    8

    P N

    Anode Cathode

    Common pract ical diodes avai lable in market

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    P-N Junc t ion Diode- conti

    9

    Used in numerous applications Switch,

    Rectifier,

    Regulator,

    Voltage multiplier, Clipping,

    Clamping, etc.

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    P-N Junc t ion Diode under b ias ing

    10

    P-N junc t ion (a) in contact (b) form ation of deplet ion region

    [http://www.imagesco.com/articles/photovoltaic/photovoltaic-pg3.html].

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    P-N Junct ion Diode under bias ing cond i tion

    11

    Unbias condition

    Diode under zero b ias c ondi t ions

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    Forw ard bias

    Positive of battery connected to p-type (anode)

    Negative of battery connected to n-type (cathode)

    Diode under forward biasing c ondi t ions

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    Reverse b ias

    Positive of battery connected to n-type material (cathode) Negative of battery connected to p-type material (anode)

    Diode under reverse biasing condit io ns

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    Self test

    14

    1. The arrow direction in the diode symbol indicates

    a. Direction of electron flow.

    b. Direction of hole flow (Direction of conventional current)

    c. Opposite to the direction of hole flow

    d. None of the above

    2.When the diode is forward biased, it is equivalent to

    a. An off switch b. An On switch

    c. A high resistance d. None of the above

    .

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    I-V character ist ic of pract ical diode

    15

    P N

    Diode symbol

    Vis 0.6 ~ 0.7 Vfor Si

    0.2 ~ 0.3 V for Ge

    (mA)

    (A)

    I-V characterist ic of Practical dio de

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    Sil icon vs. Germanium

    16

    I-V characteristic of silicon and germanium practical diode

    http://www.technologyuk.net/physics/electrical_principles/the_diode.shtm

    l

    Di d t t i

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    Diode cu rrent equat ion

    IDis diode current

    Iois reverse saturation current

    VDis voltage across diode VTis thermal voltage = T / 11600

    is a constant = 1 for Ge and 2 for Si

    )1( TD VVoD eII

    o

    VV

    o IeI TD

    For positive values of VD(forward bias),

    For large negative values of VD(reverse bias), ID Io

    TD VV

    oD eII

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    Effect of Temperature on the Reverse cu rrent

    18

    10/)(

    12 122 TT

    oo II

    Q. A Silicon diode has a saturation current of 1pA at 200C. Determine (a)

    Diode bias voltage when diode current is 3mA (b) Diode bias current when

    the temperature changes to 1000C, for the same bias voltage.

    A.

    10

    T

    D

    V

    V

    D eII mV

    TVT 25.25

    11600

    293

    11600

    V

    I

    IVV DTD 103.11ln

    0

    pA2562102II 10

    )10100(

    12)/10T(T0102

    12

    mAex xx 21.710256I )11015.322(

    103.1

    12D

    3

    Reverse current doublesfor every 10 degree rise in temperature.

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    Effect of Temperature on the Reverse cu rrent

    19

    I (mA)

    V (volts)

    I (A)

    75oC

    25oC125oC

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    Diode resistances

    20

    Static or DC resistance:

    ratio of diode voltage and

    diode current

    D

    DD

    I

    VR

    AC resistance:

    D

    Dd

    IVr

    D

    T

    D

    Dd

    IV

    IVr

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    Diode Equ ivalent Circui t

    21

    Used during circuit analysis Characteristic curve replaced by straight-line segments

    Forward bias

    Reverse bias

    V

    RF

    A K

    A K

    A K

    V

    1/RF

    RR

    =

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    Ideal d iod e : I-V charac terist ics

    22

    I-V characterist ic of Ideal diod e and ideal models

    [http://conceptselectronics.com/diodes/diode-equivalent-models/].

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Diode Equ ivalent Circui t

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    As further approximation, we can neglect the slope of the

    characteristic i.e., RF= 0

    V

    A K

    A K

    A K

    Forward bias

    Reverse biasV

    RR

    =

    RF

    = 0

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Diode Equ ivalent Circui t

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    As third approximation, even the cut-in voltage can be

    neglected (Ideal diode)

    Forward bias

    Reverse bias

    A K

    A K

    A KV= 0

    RR

    =

    RF

    = 0

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Self test

    1.The break-point voltage of Si diode is

    a. 0.2V b. 0.7V c. 0.8V d. 1.0V

    2.Why would you use silicon diodes instead ofgermanium diodes?

    25

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Breakdown phenomenon in diodes

    26

    Two breakdown mechanisms: Avalanche breakdown :

    Occurs in Lightly doped diodes,

    Occurs at high reverse Voltage.

    Zener Breakdown:

    Occurs in heavily doped diodes.

    at lower reverse bias voltages.

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Avalanche Breakdown

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    Schematic of Avalanche phenomenon

    http://shrdocs.com/presentations/12656/index.html

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Zener B reakdown

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    Schematic of Zener phenomenon

    http://shrdocs.com/presentations/12656/index.html

    Z Di d d i h i i

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Zener Diode and its character ist ic s

    29

    Anode Cathode

    P N

    I-V characterist ic s of Zener diode

    P N

    IZKor IZminIZMor IZMax

    PZMor PZMax

    PZM= VZ.IZM

    E i l t i i t

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Equivalent c ircui t

    30

    V

    RF

    RR R

    Z

    VZ

    +

    +N

    P

    N NN

    P P P

    Equivalent circuits of Zener diode

    Forward Reverse Breakdown

    Note: RZis usually very small, can be neglected

    Diode as capacitor Varacto r diode

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Diode as capacitor- Varacto r diode

    31

    d

    AxC

    S lf t t

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Self test

    32

    1. Explain the principle of PIN diode.

    2.What is the difference between PN diode and Schottky diode.

    3.Which type of diode exhibits negative resistance and why?

    4. Which of the following is not an essential element of a dcpower supply

    a. Rectifier

    b. Filter

    c. Voltage regulator

    d. Voltage amplifier

    S lf t t

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    Department of Electronics and Communication Engineering, MIT, Manipal

    Self test

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    5. What is true about the breakdown voltage in a Zener diode?

    a. It decreases when current increases.b. It destroys the diode.

    c. It equals the current times the resistance.

    d. It is approximately constant

    6. Which of these is the best description of a Zener diode?a. It is a rectifier diode.

    b. It is a constant voltage device.

    c. It is a constant current device.

    d. It works in the forward region.

    E i

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    Exercises

    1. Calculate the dynamic forward and reverse resistance of a P - N

    junction diode, when the applied voltage is 0.25V for Germanium

    Diode. I0 = lAand T = 300 K.(Ans:rf=1.734 ; rr=390 M)

    2. A germanium diode has reverse saturation current of 0.19A.

    Assuming =1, find the current in the diode when it is forward biased

    with 0.3 V at 27o

    C. (Ans: 19.5mA)

    3. The forward current in a Si diode is 15 mA at 27oC. If reverse

    saturation current is 0.24nA, what is the forward bias voltage?

    (Ans: 0.93V)

    4. A germanium diode carries a current of 10mA when it is forward

    biased with 0.2V at 27oC. (a) Find reverse sat current. (b) Find the

    bias voltage required to get a current of 100mA.

    (Ans: 4.42A,0.259V)