Diodes and Applications
Diodes and Applications
Abhishek Sawant)
Vz VE A
Ve
Anode Cathode
Rererse
Chorac+ensc
Sgmbol
JIR oF 2enes Diode
P. As +he ererse vtq is ince osed to breakdown Vt.
a lorge numbe of ele ctron-hole pais ae produced
and +he Cusent Shatply incseas es.
rereS e
Zener curent
9. This reves se Curoent s known as
Voltaqe.
& boeakdown Vtg: iS Zene
beyond zener
h. If the vo l+age 1S agin inceased
but the Vol+age
Voltaqe Zener Cuten+ 1nceaseS
emains cons+ont:
actOSS the zenet d Tode
1S Conn ected
be+ ween the output
requlo+o
ne Zener used +o n e v e
undesied oc
(Nhich s
0f +he filter
Componen+s f o dc) ond lood.
Is TL
Rs
Untequl ot ed ARL
Vs Vz
Powes Supply
Is = Iz + IL
* EFfec+ of Supply voltoge voiotions i
nceose in the ineut oltoe Vs he Curent
aLt there is
thouqh Zener diode CI) increoses and the lood
Curen+ C I ) emans conston+
forwad
bias region
-Ve
Izmin Io
Zene
cut in Voltage
breakdouwn
egion
I2nax.
Cons+ on+ ZenesIVoltaâc IR
oPPied t0 the diode
C. When o revesse biased vol+aqe
oeaches close to zenet Vo 1+age, the electic Field
in the depletion Teqion is Stong enough to Pu1
electons From thei Valence bond.
d. The valence elec+rons cwhich qains Sufficient enes
From the S+ong electic fievd of deple +ion reqion
tubil breaks bonding with paent atom. and become
free electons.
fom
e.These Faee elec+70ns Catty elec+ic Cuttent
One Ploce +0 ono+hes place.
E. A the zener breakdown region , a smal increase
voltage win apidly increase the electic Cusren+.
Breakdown eqion is noal
Narow
operating vegion for
a Zener diode. Deple+ion eqion Stonqerecic
fiend Pulls volence
elec+ons fromhe
IOns.
Negative Posi+ive
ion ion
Bat+e
* Light - Emi44ing Diode cLED) ;
- Cons+uction & wotking f LED.
- If an ordinaty diode is Foswardbì osed, free electons
Cross the junction and Fal into holes. AS these electons
fol from a hiqhe energy level +o a lower eneay
levelthey odiate eneray. In 0rdinary, diod esi +his
eneqy is radio+ed in the form oF heat but in LED
eneray is rodiated in the form of ight.
By using compounds of qollium, arsenic and phosphous,
LEDs +hot rodiotes red qeen yeilow blue orange.
or infrared light con be Poduc ed.
* Light - Emitting Diode -(CED) -
LED is a special +ype of diode thot emits ight when a
current pass +houghi+ in forword biased condition.
A k
Anode JAnode
Contact,s Contac+S
Symbol of LED
Ac+ive Region
Hole Ele+on
N- +y pe conductior
Subst>0te band
Liqht
Band
Gold Recombìnot'on
Cathode layer Valence
* Cons4ruction - band
50
30
20 LED TyPe
& colout
>Ve
1 2
Voltoge
2 0 3
a. When the LED is forwatd biased by aPpling
Vot. a c o S S i4's termin ol then i+ eri+S theviSible
Coloured light:
constant
b. In +his Condi+ion foruw ard Cut ent is almost
+hen the
at eatly Staqe bu+ when it is ful ly 'oN'
Forward Curret is increased up constantlY.
C. The iaht inte nsiy depends upon the Forw ard Cuten+
When this Curent is high then intensity oF outPut
curtent
iqht would be hgh. The voitaqeat which
toruatvol+age.
jG incoeased Constantly Called
A. Tn reverse bias Condition the eVese or leakoge
Current is almoSt near constant but Point is
Come wher it's p-n junctiOn beaks ond oevese
Curen+ is increased constant\y in nega+ive eon.
The voita qe at which beak down is occuted s calle d
break down Voltaqe.
Rs
Aeplications ofF LEDs -
LED
Vin
S
Load
FG8
* Photodiode& (Mo. Abhishek Sawant)
qeranium
everse -biased Silicon or
A photo-diode iS a CUrent nceases hen
which eyerSe
Pn uncton in
exposed +0 iqht.
the junction is
* con stuction -
availoble ina metallic Pckaqe.
des are
a. The Photo- dio mounted n an inSulo+ed
b. The diode is p-n
junc+ion
Plost ic Substrae.
Subs+ate is Seoled n metal case.
plastic
C. Then +he
the metal Cose +here 1s a tanspaent
d on the top of p-n
which allouS liqh+ to entet up to +he
Cwindow
junction.
anode and cathode ofF +he diode Come
e. Two leods met al ca Se.
Fomn the botton of the
out
Side of +he bottom
f. A +ab extending Faom the
the metal Case iderntifies the cathode
Potion of
Light ays
Iead.
Silicon Silicon
window Ni+ide
Diffusion mas k
coating
Anode
Depletion P-type Moterial P-N
Junc+
Layer
* V- T Characteistics of photo-diode -
Reverse voltage
Ve
-5 -4 -3 -2 +5 VE
Dark Cutent
200o lux
400
2500 lux
Ig(uA)
mode.
evese bias
a. It is always oPetated in
hoi2on+ally in volt5
b. Reverse Voltages are plott ed vestical|y in the
and evese Cuent S plot+ed
microampers(uA).
C. Re verse curtentS Independent From the eVee
VoIta qé.
d. when iluminotion is Zero the eVese Cutent is
appso ximo+ey Zer0 but there is o n y a Small
amount oF Cuten+ is P e s e n t and this Cutent
1S Caled d a k Cuent.
ilumino+ion, the reVeseCurrent
e. As increase +he
also increase linearl
Photo Diode
Counter
* Ad Vantages of photo- diode
I+ b as lo wer noise
2. I+t has better fequency response than LDR.
3. It Can be opebated at high foequencies in otder
of | MHZ
1. Positive Cippet
Cscles of
The cippe \which remnoves the poSitive haif
poSi+ive cipper.
the input voI+a qe is caled as the
a. Positive Series CiPper -
D
RL
-Vmax
Input OutPut Wavefon
Wave Form
i Diode is connected Series wIt the Load.
i) Fro mobove fiq. it is Seen that when ineut i5 PoSitive
diode is everse bi0sed and So outPut ermains at
2ero. e posi+ive haif Cycle is CliPped off.
iS Duing Neqative hof cycle of the input the diode
19 Fo wasd biased and So Negotive haif cycle aPpears
acsoss +he Output.
b. Posi+ive shunt cipper circuit8
R
+Vmoxt
D RL
- Vmux
Input OUtPut
Wave Forn Wave form
) Dio de in
paralel with the Load
i) Foom above fiq. it is se en that when input is positiVe
4he diode'Dis forw ard bias ed, ac45 like closed
Switch So con ducts heavily. So voitaqe dtop across
loadresistan ce RL iS 2er0. Thus the ou+put Voltoge
duinq Posi+ive holf cycle is zeo.
i ) Duing Negative hof cycle of the input Voltage,the
diode p' is evese biased and behaves as an open
Switch. The entire input o1taqe aPPeas aCoSS the
Lood oesist ance RL and we qet wave for mo+ Neqative
hof cycle.
2. Neqative cLipper -
Neqative clipper is one which emoves ol+he Negatie
haif cycles oF +he in put voltaqe.
a. Negative Seies Cipper;
+Vmax D +vmax
RL
Vmox
Iopu+
WaveFon
Wavefom
D Diode is Conec+ed Seies wi+hthe Load
) From obove fig. it is Seen that when input is
Neqative. diode is everse biased. and so Du Put
emains at zero ie. Ne qative haif cycle isclipped
ofF.
I) Duinq Positive ha |f cycle the diode is Forward
biased and So posi+ive haiF Cycle appeats aCtoss
+he oUtput
b. Neqotive Shunt cipper
4Vmax +Vmax!
RL
-Vmc
Input
nave fom
-Vmax +
4. Combino+ion cippey -
Whena potion oF bo+h poSitiVe ond Negative of each
haf cycle oF +he input Voltage is to be cipped or
Yemoved +he cIcuit Called as Combinaton Clipper.
R 4Vmaxt
Vma
Di
RL
V, V2
-V2
-Vmax -Vmax
Inpu Wavefom a Outpu+ Wave form
+5V +iov
Positive
clamper
-5V
wi+h
a" lhe in put Siqnol is assu med to be Squae WoVe
+ime peiod'T:
b The clamped outpu+ is obtained acoss RL.
C. The values oFCand RL are so Selec+ed that the
tine Constant C = CRL iS very age. This Theans that
Vol+age aco55 the capacitor will not disharge
Siqnifican+ly duing, the in+erval when diode is not
conducting
* opeotion -
a- Duing negative hoifF Cycle
of input Siqnal +he diodeis V
forw ard biased There Fore V
+ RL Vout
+he diode behaves aS a Shot.
Chatqing time conston+
CT= CRE)iS verySma| Sothat
Capacitor wil Choge +o'v'volt+
very guickiy the out put Voltage
iS acoss +he Shot Citcui+ Vout = oV.
b. Duing the positive hoif cycle
the diode everse bias ed
V
behaves as open switch.
Dischatqing tirme onstont Vout RL Vout
T= CRL is qoeate than +ine
Peiod of inPut Siqnal. the
Capacitor remains almost fully
chataed to v Volts duing+he
oFf +ime of the diode.
PP kvL in inpu+ Loop, We have
Vt V- Vout = 0
Vout =2V
Tnput siqnal hos been Pushed upword byY Vol+ So
+hot neqative Peaks fall on +he zero level.
Vin
-V
Vouth +2V
* Negative clampe C
Vin
RL Vout
Vin
C
+
haifcycle
a.Duing the positive diodeis
Signalthe
Of the input V+
forword biosed so it behaves RL Vout
as a Short citcuit. The charqinq
+ime Constant CRf iS Vey Sall
So +hat the CapacitoY ui chaqe
+o' v 'volts Vey gickly, The
across
output vortage is direc+ly = oV.
+he Short circuit Vout
there Foe
Vout RL Vout
>t
CMA:S-Sawon+)