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SC1109 Просмотр технического описания (PDF) - Semtech Corporation

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SC1109 Datasheet PDF : 17 Pages
First Prev 11 12 13 14 15 16 17
SYNCHRONOUS PWM CONTROLLER WITH
DUAL LOW DROPOUT REGULATOR
CONTROLLERS
SC1109
PRELIMINARY - October 16, 2000
COMPONENT SELECTION
fast enough to reduce the voltage dropped across the
ESR at a faster rate than the capacitor sags, hence en-
SWITCHING SECTION
suring a good recovery from transient with no additional
OUTPUT CAPACITORS - Selection begins with the most excursions.
critical component. Because of fast transient load current We must also be concerned with ripple current in the
requirements in modern microprocessor core supplies, output inductor and a general rule of thumb has been to
the output capacitors must supply all transient load cur- allow 10% of maximum output current as ripple current.
rent requirements until the current in the output inductor Note that most of the output voltage ripple is produced
ramps up to the new level. Output capacitor ESR is by the inductor ripple current flowing in the output capac-
therefore one of the most important criteria. The maxi- itor ESR. Ripple current can be calculated from:
mum ESR can be simply calculated from:
RESR
Vt
It
Where
I = LRIPPLE
VIN
4LfOSC
Ripple current allowance will define the minimum permit-
ted inductor value.
Vt = Maximumtransientvoltageexcursion POWER FETS - The FETs are chosen based on several
It = Transientcurrentstep
criteria with probably the most important being power
dissipation and power handling capability.
For example, to meet a 100mV transient limit with a
TOP FET - The power dissipation in the top FET is a
10A load step, the output capacitor ESR must be less combination of conduction losses, switching losses and
than 10m. To meet this kind of ESR level, there are
three available capacitor technologies.
bottom FET body diode recovery losses.
a) Conduction losses are simply calculated as:
Each Capacitor
Total
Technology
Low ESR Tantalum
C ESR Qty. C ESR
(µF) (m) Rqd. (µF) (m)
330
60 6 2000 10
OS-CON
330
25 3 990 8.3
Low ESR Aluminum 1500
44 5 7500 8.8
PCOND = IO2 RDS(on) δ
where
δ = duty cycle VO
VIN
b) Switching losses can be estimated by assuming a
switching time, if we assume 100ns then:
The choice of which to use is simply a cost/perfor-
mance issue, with Low ESR Aluminum being the
cheapest, but taking up the most space.
PSW = IO VIN 10 2
or more generally,
INDUCTOR - Having decided on a suitable type and
value of output capacitor, the maximum allowable value
of inductor can be calculated. Too large an inductor will
produce a slow current ramp rate and will cause the
output capacitor to supply more of the transient load
current for longer - leading to an output voltage sag
below the ESR excursion calculated above.
The maximum inductor value may be calculated from:
( ) L RESR C
It
VIN VO
The calculated maximum inductor value assumes 100%
duty cycle, so some allowance must be made. Choosing
an inductor value of 50 to 75% of the calculated maxi-
mum will guarantee that the inductor current will ramp
PSW
=
IO VIN (tr + t f ) fOSC
4
c) Body diode recovery losses are more difficult to esti-
mate, but to a first approximation, it is reasonable to as-
sume that the stored charge on the bottom FET body
diode will be moved through the top FET as it starts to
turn on. The resulting power dissipation in the top FET
will be:
PRR = QRR VIN fOSC
To a first order approximation, it is convenient to only
consider conduction losses to determine FET suitability.
For a 5V in; 2.8V out at 14.2A requirement, typical FET
losses would be:
© 2000 SEMTECH CORP.
15
TEL:805-498-2111 FAX:805-498-3804 WEB:http://www.semtech.com

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