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HBAT-5402 Datasheet(PDF) 7 Page - AVAGO TECHNOLOGIES LIMITED

Part # HBAT-5402
Description  High Performance Schottky Diode for Transient Suppression
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Manufacturer  AVAGO [AVAGO TECHNOLOGIES LIMITED]
Direct Link  http://www.avagotech.com
Logo AVAGO - AVAGO TECHNOLOGIES LIMITED

HBAT-5402 Datasheet(HTML) 7 Page - AVAGO TECHNOLOGIES LIMITED

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7
Figure 7. Forward Current vs. Forward Voltage at 25°C.
Becausetheautomatic,pick-and-placeequipmentused
toassembletheseproductsselectsdicefromadjacent
sitesonthewafer,thetwodiodeswhichgointotheHBAT-
540orHBAT-540C(seriespair)arecloselymatched—
withouttheaddedexpenseoftestingandbinning.
Current Handling in Clipping/Clamping Circuits
Thepurposeofaclipping/clampingdiodeistohandle
high currents, protecting delicate circuits downstream
of the diode. Current handling capacity is determined
bytwosetsofcharacteristics,thoseofthechipordevice
itselfandthoseofthepackageintowhichitismounted.
Maximum reliability is obtained in a Schottky diode
when the steady state junction temperature is main-
tainedatorbelow150°C,althoughbriefexcursionsto
higherjunctiontemperaturescanbetoleratedwithno
significant impact upon mean-time-to-failure, MTTF. In
ordertocomputethejunctiontemperature,Equations
(1)and(3)belowmustbesimultaneouslysolved.
Figure 7. Forward Current vs.
Forward Voltage at 25
°C.
VF – FORWARD VOLTAGE (V)
.01
10
1
.1
300
100
0
0.1
0.3
0.2
0.5
0.4
0.6
HSMS-270x
HBAT-540x
current
limiting
pull-down
(or pull-up)
long cross-site cable
noisy data-spikes
Vs
0V
voltage limited to
Vs + Vd
0V – Vd
Figure 8. Two Schottky Diodes Are Used for Clipping/Clamping in a Circuit.
Consider the circuit shown in Figure 8, in which two
Schottkydiodesareusedtoprotectacircuitfromnoise
spikesonastreamofdigitaldata.Theabilityofthediodes
tolimitthevoltagespikesisrelatedtotheirabilitytosink
theassociatedcurrentspikes.Theimportanceofcurrent
handlingcapacityisshowninFigure9,wheretheforward
voltagegeneratedbyaforwardcurrentiscomparedin
twodiodes.ThefirstisaconventionalSchottkydiodeof
thetypegenerallyusedinRFcircuits,withanRSof7.7Ω.
ThesecondisaSchottkydiodeofidenticalcharacteris-
tics,savetheRSof1.0Ω.Fortheconventionaldiode,the
relativelyhighvalueofRScausesthevoltageacrossthe
diode’sterminalstoriseascurrentincreases.Thepower
dissipatedinthediodeheatsthejunction,causingRSto
climb,givingrisetoarunawaythermalcondition.Inthe
seconddiodewithlowRS,suchheatingdoesnottake
placeandthevoltageacrossthediodeterminalsismain-
tainedatalowlimitevenathighvaluesofcurrent.
Figure 9. Comparison of Two Diodes.
0
0.1
0.2
0.3
0.5
0.4
IF – FORWARD CURRENT (mA)
0
3
2
1
6
4
5
Rs = 7.7 Ω
Rs = 1.0 Ω
IF = IS e
–1
11600 (VF – IFRS)
nTJ
(1)
IS = I0
e
TJ
298
2
n
1
TJ
1
298
–4060
(2)
TJ = VFIFθJC + TA
(3)
where:
IF=forwardcurrent
IS=saturationcurrent
VF=forwardvoltage
RS=seriesresistance
TJ=junctiontemperature
IO=saturationcurrentat5°C
n=diodeidealityfactor
θJC=thermalresistancefromjunctiontocase
(diodelead)
packagechip
TA=ambient(diodelead)temperature
Equation(1)describestheforwardV-IcurveofaSchottky
diode.Equation()providesthevalueforthediode’ssat-
urationcurrent,whichvalueispluggedinto(1).Equation
(3)givesthevalueofjunctiontemperatureasafunction
of power dissipated in the diode and ambient (lead)
temperature.
Figure 9. Comparison of Two Diodes.


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