Philips Semiconductors
Power Diodes Introduction
NEW PRODUCTS
Philips Semiconductors are working intensively on
bringing new Power Diode products to the market. The
products listed below appear for the first time in this data
handbook.
25 V SCHOTTKY DIODES
A range of low voltage schottky diodes with a reverse
voltageratingof25 V,withextremelylowforwardvoltage
and ultra fast switching. These products are intended for
use in switched mode power supplies with 3 V and 3.3 V
outputs. They are also ideal for use as or-ing diodes in
fault tolerant designs or current sharing configurations.
Types: BYV116, PBYR225CT, PBYR1025,
PBYR1525CT, PBYR2025CT, PBYR2525CT.
DEFLECTION DIODES
Further extensions to our range of high voltage, fast
recovery diodes, designed for use in the horizontal
deflection stages of multisync computer monitors with
scan rates up to 82 kHz. These devices complement our
range of high voltage bipolar deflection transistors and
have fast forward recovery time, low forward recovery
voltage and reverse voltage ratings up to 1700 V.Types:
BY479X-1700, BY559-1500.
ISOLATED 45 V SCHOTTKY AND 200 V EPITAXIAL DIODES
A wide range of 45 Vschottky diodes and 200 V ultrafast
recovery epitaxial diodes in the SOT186A envelope. This
package is an isolated version of TO220AB with
2500 Vrms isolation between leads and case. Types:
BYV118X, BYV133X, BYV143X, PBYR745X,
PBYR1045X, PBYR1545CTX, PBYR1645X,
PBYR2045CTX, PBYR2545CTX, BYQ28X, BYQ28EX,
BYW29EX, BYV32EX, BYV42EX,
SURFACE MOUNT POWER DIODES IN SOT404
A wide range of schottky and 200 V epitaxial diodes in a
SOT404 envelope suitable for surface mounting. This
package is a surface mounting version of TO220AB with
the same thermal resistance and current rating. Types:
BYV118B, BYV143B, PBYR745B, PBYR1045B,
PBYR10100B, PBYR1545CTB, PBYR1645B,
PBYR2045CTB, PBYR20100CTB, PBYR2545CTB,
BYQ28EB,BYW29EB,BYV32EB,BYV42EB,BYV79EB.
SURFACE MOUNT BREAKOVER DIODES IN SOD106
The BR211 range of breakover diodes in a SOD106
surface mounting envelope. Used for transient
overvoltage protection in line based telecommunications
equipment. BR211SM series.
FORTHCOMING PRODUCTS
The products listed below are planned for release within
the next 12 months, before the next edition of this data
handbook. Contact your Philips Regional or National
Sales office for further details.
SURFACE MOUNT POWER DIODES IN SOT428
Available towards the end of 1996, a range of schottky
and200 VepitaxialdiodesinaSOT428envelopesuitable
for surface mounting. The SOT428 envelope is slightly
larger than our present subminiature surface mounting
package, SOT223 and may be mounted on the same
printed circuit pad layout. However, it has lower thermal
resistance and can accommodate larger crystal sizes,
thereby allowing higher current ratings to be achieved in
a smaller package.
SCHOTTKY AND 200 V EPITAXIAL DIODES IN TO247
Available during the first quarter of 1997, a range of
schottkyand 200 V epitaxial diodesin a TO247 envelope
suitableforhigh powerapplications,featuringlowthermal
resistance and output current ratings up to 60 Amps.
POWER FACTOR CORRECTION DIODES
Available during the first quarter of 1997, a range of
ultrafast, 600 V epitaxial diodes specifically designed for
power factor correction and other forced commutation
applications. These diodes are designed to minimise
switching losses both in the diode and in the switching
transistor.Otherapplicationsincludefreewheelingdiodes
in full and half bridge switched mode power supplies,
where they complement our new range of 400 V, 500 V
and 600 V power mosfets.
APPLICATIONS
Application information for Power Diodes and other
Philips power products is published in Philips Power
Semiconductor Applications Handbook. (Order
code: 9398-652-85011)
September 1996
Philips Semiconductors
Power Diodes Introduction
POWER DIODE CHARACTERISTICS
Back diffused rectifier diodes
A single-diffused P-N diode with a two layer structure
cannotcombine ahighforwardcurrentdensitywithahigh
reverse blocking voltage.
A way out of this dilemma is provided by the three layer
structure, the so-called P-I-N diode, where ’I’ is a lightly
doped (nearly intrinsic) layer. This layer, called the base,
is sandwiched between the highly doped diffused P+and
N+outer layers giving a P+-P-N+or P+-N-N+structure.
Generally, the base gives the diode its high reverse
voltage,andthetwodiffusedregionsgivethehighforward
current rating.
Such a three layer diode can be realised using a
’back-diffused’ structure. A lightly doped silicon wafer is
given a very long N+diffusion on one side, followed by a
relatively shallow P+diffusion on the opposite side. This
asymmetricdiffusionallowsbettercontrolofthethickness
of the base layer than the conventional double diffusion
method,resultinginabettertrade-offbetweenlowforward
voltage and high reverse blocking voltage. Generally, for
a given silicon area, the thicker the base layer the higher
the VRand the lower the IF. Reverse switching
characteristics also determine the base design. Fast
recoverydiodes usuallyhaveN-typebase regions togive
’soft’ recovery with a narrow base layer to give fast
switching.
Ultra fast rectifier diodes
Ultra fast rectifier diodes, made by epitaxial technology,
areintendedfor usein applications wherelowconduction
and switching losses are of paramount importance and
relatively low reverse blocking voltage (VRWM = 150V) is
required: e.g. Switched mode power supplies operating
at frequencies of about 50 kHz.
The use of epitaxial technology means that there is very
close control over the almost ideal diffusion profile and
base width giving very high carrier injection efficiencies
leading to lower conduction losses than conventional
technologypermits. Thewell defineddiffusion profilealso
allowsatightcontrolofstoredminoritycarriersinthebase
region, so that very fast turn-off times (35 ns) can be
achieved. The range of devices also has a soft reverse
recovery and a low forward recovery voltage.
Schottky-barrier rectifier diodes
Schottky-barrier rectifiers find application in low-voltage
switched-mode power supplies (e.g. a 5 V output) where
they give an increase in efficiency due to the very low
forward drop, and low switching losses. Power Schottky
diodes are made by a metal-semiconductor barrier
process to minimise forward voltage losses, and being
majority carrier devices have no stored charge. They are
therefore capable of operating at extremely high speeds.
Electricalperformanceinforwardandreverseconduction
is uniquely defined by the device’s metal-semiconductor
’barrierheight’.Philipsprocessminimisesforwardvoltage
drop, whilst maintaining reverse leakage current at full
rated working voltage and Tj max at an acceptable level.
Philips range of power schottky-barrier diodes can
withstand reverse voltage transients and have
guaranteed reverse surge capability.
Power diode ratings
A rating is a value that establishes either a limiting
capability or a limiting condition for an electronic device.
It is determined for specified values of environment and
operation, and may be stated in any suitable terms.
Limiting conditions may be either maxima or minima.
All limiting values quoted in this data handbook are
Absolute Maximum Ratings - limiting values of operating
and environmental conditions applicable to any device of
a specified type, as defined by its published data, which
should not be exceeded under the worst probable
conditions.
VOLTAGE RATINGS
VRSM Non-repetitivepeakreversevoltage.Themaximum
allowable instantaneous reverse voltage including
all non-repetitive transients. duration 10 ms.
VRRM Repetitive peak reverse voltage. The maximum
allowable instantaneous reverse voltage including
transients which occur every cycle,
duration 10 ms, duty cycle 0.01.
VRWM Crest working reverse voltage. The maximum
allowable instantaneous reverse voltage including
transients which may be applied every cycle
exludingallrepetitiveandnon-repetitivetransients.
VRContinuous reverse voltage. The maximum
allowable constant reverse voltage. Operation at
rated VRmay be limited to junction temperatures
below Tj max in order to prevent thermal runaway.
CURRENT RATINGS
IF(AV) Average forward current. Specified for either
square or sinusoidal current waveforms at a
maximum mounting base or heatsink temperature.
The maximum average current which may be
passedthroughthedevicewithoutexceedingTj max.
IF(RMS) Root mean square current. The rms value of a
current waveform is the value which causes the
same dissipation as the equivalent d.c. value.
IFRM Repetitive peak forward current. The maximum
allowablepeakforwardcurrent includingtransients
which occur every cycle. The junction temperature
should not exceed Tj max during repetitive current
transients.
IFSM Non-repetitive forward current. The maximum
allowable peak forward current which may be
applied no more than 100 times in the life of the
device. Usually specified with reapplied VRWM
following the surge.
September 1996
Philips Semiconductors
Power Diodes Introduction
IRRM Repetitive peak reverse current. The maximum
allowablepeakreversecurrent includingtransients
which occur every cycle.
IRSM Non-repetitive reverse current. The maximum
allowable peak reverse current which may be
applied no more than 100 times in the life of the
device.
Forward current ratings
Theforwardvoltage/currentcharacteristicof adiode may
be approximated by a piecewise linear model as shown
in fig:1. where RSis the slope of the line which passes
through the rated current and VOis the voltage axis
intercept.Theforward voltageisthenVF = VO + IF.RS,and
theinstantaneousdissipation isPF = VO.IF + IF2.RS.where
IFis the instantaneous forward current.
It can be shown that the average forward dissipation for
any current waveform is: PF(AV) = VO.IF(AV) + IF(RMS)2.RS,
where IF(AV) is the average forward current and IF(RMS) is
the rms value of the forward current. Graphs in the
published data show forward dissipation as a function of
average current for square or sinusoidal waveforms over
a range of duty cycles and form factors.
To ensure reliable operation, the maximum allowable
junction temperature Tj max should not be exceeded
repetitively, either as a result of the average dissipation
in the device or as a result of high peak currents
The average junction temperature rise is the average
dissipation multiplied by the thermal resistance; Rth j-mb or
Rth j-hs. Subtracting the junction temperature rise from the
maximum allowable junction temperature Tj max, gives the
maximum allowable mounting base or heatsink
temperature.
The peak junction temperature rise for a rectangular
current pulse may be found by multiplying the
instantaneouspowerbythethermalimpedance.Analysis
methods for non-rectangular pulses are covered in the
Power Semiconductor Applications handbook.
Fig.1. Piecewise linear approximation to diode
forward characteristic.
Power diode characteristics
A characteristic is an inherent and measurable property
ofadevice.Suchapropertymay beexpressedas avalue
for stated or recognized conditions. A characteristic may
alsobe a set ofrelated values, usuallyshown ingraphical
form.
REVERSE RECOVERY
When a semiconductor rectifier diode has been
conducting in the forward direction sufficiently long to
establish the steady state, there will be a charge due to
minority carriers present. Before the device can block in
the reverse direction this charge must be extracted. This
extraction takes the form of a transient reverse current
and this, together with the reverse bias voltage results in
additional power dissipation which reduces the
rectification efficiency. At sine-wave frequencies up to
about 400Hz these effects can often be ignored, but at
higher frequencies and for square waves the switching
losses must be considered. The parameters of reverse
recovery are defined in fig:2.
Stored charge
The area under the IRversus time curve is known as the
stored charge (Qs) and is normally quoted in
microcoulombs or nanocoulombs. Low stored charge
devices are preferred for fast switching applications.
Reverse recovery time
Another parameter which can be used to determine the
speedofthe rectifieristhereverserecoverytime(trr).This
is measured from the instant the current passes through
zero (from forward to reverse) to the instant the current
recovers to either 10% or 25% of its peak reverse value.
Low reverse recovery times are associated with low
stored charge devices.
The conditions which need to be specified are:
a. Steady-state forward current (IF); high currents
increase recovery time.
0VF / V
50
40
30
20
10
0 0.5 1.51.0
IF / A
slope Rs
Vo
September 1996
Philips Semiconductors
Power Diodes Introduction
b. Reverse bias voltage (VR); low reverse voltage
increases recovery time.
c. Rate of fall of anode current (dIF/dt); high rates of fall
reduce recovery time, but increase stored charge.
d. Junctiontemperature(Tj);hightemperaturesincrease
both recovery time and stored charge.
Fig.2. Definition of t
rr
, Q
s
and I
rrm
Softness of recovery
In many switching circuits it is not just the magnitude but
the shape of the reverse recovery characteristic that is
important. If the positive-going edge of the characteristic
has a fast rise time (as in a so-called ’snap-off’ device)
this edge may cause conducted or radiated radio
frequency interference (rfi), or it may generate high
voltagesacross inductors which maybe in series with the
rectifier. The maximum slope of the reverse recovery
current (dIR/dt) is quoted as a measure of the ’softness’
of the characteristic. Low values are less liable to give rfi
problems.The measurementconditionswhichneed tobe
specified are as above.
Reverse recovery current
The peak value of the reverse recovery current (Irrm)isan
important parameter in many switched mode power
supply circuits. This is because the high transient current
produced by a diode with a high Irrm can be interpreted by
the circuit as a short circuit fault, which may cause the
power supply to shut down or have apparently poor load
regulation. Like the stored charge and reverse recovery
time, Irrm increases with increasing temperature, so the
effects sometimes only become apparent when the
equipment gets hot. Irrm correlates with stored charge Qs.
Thus choosing an Ultrafast diode with low Qsusually
avoids this problem.
SWITCHING LOSSES
The product of the transient reverse current and the
reversevoltageispowerdissipation,mostofwhichoccurs
whilstthereverse recoverycurrentisdecreasingfrom the
peakvalue(Irrm)tozero.Inrepetitiveoperationanaverage
power can be calculated and added to the forward
dissipation to give the total power. The peak value of
transient reverse current is known as Irrm. The origin of
reverse recovery losses is illustrated in fig:3.
The conditions which need to be specified are:
a. Forward current (IF); high currents increase switching
losses.
b. Rate of fall of anode current (dIF/dt); high rates of fall
increaseswitchinglosses.Thisisparticularlyimportant
in square-wave operation. Power losses in sine-wave
operation for a given frequency are considerably less
due to the much lower dIF/dt.
c. Frequency (f); high frequency means high losses.
d. Reverse bias voltage (VR); high reverse bias means
high losses.
e. Junction temperature (Tj); high temperature means
high losses.
Fig.3. Waveforms showing the origin of reverse
switching losses.
FORWARD RECOVERY
At the instant a semiconductor rectifier diode is switched
into forward conduction there are no carriers present at
the junction, hence the forward voltage drop may be
instantaneously of a high value. As the stored charge
builds up, conductivity modulation takes place and the
forwardvoltage rapidly fallstothesteady state value.The
peakvalueofforwardvoltagedropisknownastheforward
recoveryvoltage(Vfr).Thetimefromtheinstantthecurrent
reaches 10% of its steady-state value to the time the
forward voltagedrops below a given value ( usually5V or
2V)isknownastheforwardrecoverytime(tfr).Theforward
recovery parameters are defined in fig:4.
The conditions which need to be specified are:
a. Forward current (IF); high currents give high recovery
voltages.
b. Current pulse rise time (tr); short rise times give high
recovery voltages.
100%
time
dI
dtF
IR
IF
Irrm
trr
25% or 10%
Qs
time
IR
IF
Irrm
trr
VR
VR
VF
-dIF/dt area = Qs
September 1996
Philips Semiconductors
Power Diodes Introduction
c. Junction temperature (Tj); The influence of
temperature is slight.
Fig.4. Definition of V
fr
and t
fr
Breakover diodes
Breakover diodes (BOD’s) are two terminal devices that
operate in either an off (non-conducting) or an on
(conducting) state. A BOD will remain in the off state until
the maximum breakover voltage is applied across its
terminals. A BOD will then conduct with a low on-state
voltage until the current is reduced below the minimum
holding current.
BOD’s are available as Single Symmetric (operation in
1st and 3rd quadrants) in a hermetically sealed axial
leaded SOD84 envelope, and also in a surface mount
SOD106 package. BOD’s are graded according to
breakover voltage.
BREAKOVER DIODE CHARACTERISTICS
Fig.5. Breakover diode symbol and characteristics.
The main characteristics are illustrated in fig:5. These
characteristics are:-
V(BO) Breakover voltage, the maximum voltage
appearing across the BOD before switching to the
on-state.
VDStand-off voltage, maximum normal operating
voltage.
IDOff-state current, normally quoted at VD.
V(BR) Breakdown voltage, below which the BOD will not
go into avalanche breakdown.
I(BR) Breakdown current, with V(BR) applied.
ISSwitching current, the avalanche current required
to switch the BOD to the on-state.
ITOn-state current.
VTOn-state voltage, specified at a given IT.
IHHolding current, the minimum current at which the
BOD will remain in the on-state.
USE OF BREAKOVER DIODES
BOD’s are primarily designed to protect electronic
equipment connected to transmission lines against
transientovervoltages.However,there aremanyusesfor
BOD’s as breakover switches.
In designing BOD circuits the following must be
considered:-
Off-state conditions
VDMust not be exceeded in normal off-state
operation. In the off-state the BOD will not pass
more current than ID.
dVD/dt The rate of rise of voltage must not exceed that
quotedfor the device. Ifthis is exceeded theBOD
may switch to the on-state.
V(BR) To ensure the BOD remains in the off-state, the
voltage must remain below V(BR) min. If this is
exceeded, the BOD will either clip the voltage or
switch to the on-state.
ISIfV(BR) isexceeded butthecurrentlimitedtobelow
ISminimum,the BOD is prevented from switching
to the on-state.
CjThe off-state capacitance across the BOD. In
transmission line protection applications this will
be across the termination of the line.
Switching conditions
V(BO) Atransient voltage greater than V(BO) max is required
to switch the BOD. V(BO) may be greater than the
voltageacrosstheBODwhenitispassingacurrent
of IS max.
ISTo enable the BOD to switch to the on-state a
current greater than ISmaximum is required.
time
time
VF
Vfr
VF
IF
10%
5V / 2V
tfr
VT
IT
IH V(BO)
IS
ID
VD
current
voltage
Symbol
V(BR)
I(BR)
Symmetric BOD
September 1996
Philips Semiconductors
Power Diodes Introduction
On-state conditions
VTThe on-state voltage is quoted for a given IT
IHTo enable the BOD to switch to the off-state the
current must fall below IHminimum.
ITSM ITSM specifies the rate of rise and duration of a
transient peak on-state current. The waveshape is
definedaccording toCCITTRec. K17, illustrated in
Fig:6. The waveform is referred to as 10/700 µs
waveform.
Fig.6. Definition of I
TSM
waveform.
Thermal conditions
Rth For extended on-state operation ( > 0.1 ms) the
steady-state thermal resistance should be
considered. Total thermal resistance to ambient
should be sufficiently low to dissipate the heat
generated by the device.
Zth If the BOD is used only during transient
overvoltagesthenthe transientthermal impedance
to ambient should be considered.
100%
90%
50%
30%
ITSM
10us 700us time
current
0
September 1996
Philips Semiconductors
Power Diodes Introduction
QUALITY
Total Quality Management
Philips Semiconductors is
committed to be a world class,
customer driven, volume supplier
of semiconductors.
To achieve this, we operate a Total
Quality Management (TQM)
system, based on Continuous
Improvement and Quality
Assurance in all our business
activities, and Partnerships with
our customers and suppliers.
The top priority throughout the company is Continuous
Improvement.
To focus on this we will:
- Work closely with key customers, as our partners.
- Monitor progress, using customer-driven data, of
our product and services.
- Benchmark against the best.
Furthermore, all parts of the organisation must always
demonstrate:
- The presence of a strong, management-led
improvement structure.
- Commitment and participation in all areas.
- Measurable progress towards our Quality
Improvement goals.
Organisation
An organisation is in place which ensures that personnel
with the necessary organisational freedom and authority
can identify and solve quality problems, prevent
occurrence of product non-conformity and protect the
customer from non-conforming product.
Design control
A comprehensive design and development procedure is
in place which ensures that the requirements of good
design practice are met.
Particular emphasis is placed on ensuring that the initial
specification is agreed by the Customer and the
Marketing and Development functions.
There are regular formal reviews of design progress to
ensure that the initial specification will be met by the
design.
Detailed measurements are made on initial samples to
ensure that the initial specification has been met.
Process control
All processes which directly affect quality are carried out
under controlled conditions. Documented work
instructionsareavailableforallproductionprocessesand
the appropriate environmental controls are in place to
ensure consistent processing. Monitoring of the product,
processes and the environment takes place during
production.
Approval exercises are run to ensure that new processes
and new equipment perform at an acceptable level.
Written, photographicor visual standards are available at
the appropriate points in the production processes.
Corrective action
Non-conforming product found in process is investigated
and the root causes identified. Changes to product or
process are then introduced to prevent recurrence of the
problem.
Quality assurance
Based on ISO 9000 standards, customer standardssuch
as Ford TQE. Our factories are certified to ISO 9000.
Partnerships with customers
These include: PPM co-operations, design-in
agreements, ship-to-stock, just-in-time, self-qualification
programmes and application support.
Partnerships with suppliers
In addition to ISO9000 audits and close monitoring of
supplier delivery performance, we operate a Supplier
Excellence Award scheme which requires suppliers and
their sub-suppliers to use statistical process control,
perform gauge studies and use failure mode and effect
analysis (FMEA) techniques to identify and correct the
root causes of quality and delivery problems.
Product reliability
With the increasing complexity of Original Equipment
Manufacturer (OEM) equipment, component reliability
must be extremely high. Our research laboratories and
development departments study the failure mechanisms
of semiconductors. Their studies result in design rules
and process optimizations for the highest built-in product
reliability. Highly accelerated tests are applied in order to
evaluate the product reliability. Rejects from reliability
tests and from customer complaints are submitted to
failure analysis and the results applied to improve the
product or process.
Customer responses
Our quality improvement depends on joint action with our
customer. We need our customers inputs and we invite
constructive comment on all aspects of our performance.
Please contact your local sales representative.
Recognition
The high quality of our products and services is
demonstrated by many Quality Awards granted by major
customers and international organisations.
QUALITY IMPROVEMENT
PARTNERSHIPS
QUALITY ASSURANCE SYSTEM
TQM
September 1996