Fund. of. Electronics Ch02 Diodes
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Transcript of Fund. of. Electronics Ch02 Diodes
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7/17/2019 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
Fund. Of Electronic
Circuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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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)
Fund. Of Electronic
Circuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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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
.
Fund. Of Electronic
Circuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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2.1 Silicon atom
used semiconductor.
An isolated atom has
pro ons anelectrons as shown:
Valence orbit with 4 electrons
Fund. Of Electronic
Circuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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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
Fund. Of Electronic
Circuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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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.
Fund. Of Electronic
Circuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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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.
Fund. Of Electronic
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Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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n-t e semiconductors contd.
Fund. Of Electronic
Circuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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-t e semiconductors
By using a trivalent impurity, one whose
atoms have onl 3 valence electrons(ex:Boron).
Fund. Of Electronic
Circuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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p-type semiconductors (contd.)
By using a trivalent impurity, one whose atoms haveonly 3 valence electrons (ex:Boron).
Fund. Of Electronic
Circuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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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.
Fund. Of Electronic
Circuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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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.
Fund. Of ElectronicCircuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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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.
Fund. Of ElectronicCircuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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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).
Fund. Of ElectronicCircuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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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.
Fund. Of ElectronicCircuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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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
Fund. Of ElectronicCircuits
Associate Prof. Dr. Soliman Mahmoud
Electronics and Electrical Engineering Department
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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.
Fund. Of ElectronicCircuits
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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.
Fund. Of ElectronicCircuits
Associate Prof. Dr. Soliman MahmoudElectronics and Electrical Engineering Department
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4.1 Semiconductor diodes
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4.1 Silicon diodes
-
device
Fund. Of ElectronicCircuits
Associate Prof. Dr. Soliman MahmoudElectronics and Electrical Engineering Department
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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.
Fund. Of ElectronicCircuits
Associate Prof. Dr. Soliman MahmoudElectronics and Electrical Engineering Department
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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
Fund. Of ElectronicCircuits
Associate Prof. Dr. Soliman MahmoudElectronics and Electrical Engineering Department
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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
Fund. Of ElectronicCircuits
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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.
Fund. Of ElectronicCircuits
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4.4 Diode circuit anal sis
VEI
ON= ON
rR
VEI
+
=
Fund. Of ElectronicCircuits
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4.5 Zener breakdown diode: Symbol
Model for the zener diode.Circuit symbol for a
zener diode.
Fund. Of ElectronicCircuits
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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
Fund. Of ElectronicCircuits
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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.
Fund. Of ElectronicCircuits
Associate Prof. Dr. Soliman MahmoudElectronics and Electrical Engineering Department
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