PRODUCT DATASHEET
AAT2515
SystemPowerTM
Dual 600mA FastTransient High Frequency Buck Converter
The input capacitor RMS ripple current varies with the
input and output voltage and will always be less than or
equal to half of the total DC load current of both convert-
ers combined.
the power leads from the bench power supply, most
applications do not exhibit this problem.
In applications where the input power source lead induc-
tance cannot be reduced to a level that does not affect
converter performance, a high ESR tantalum or alumi-
num electrolytic capacitor should be placed in parallel
with the low ESR, ESL bypass ceramic capacitor. This
dampens the high Q network and stabilizes the system.
IO1(MAX) + IO2(MAX)
IRMS(MAX)
=
2
This equation also makes the worst-case assumption
that both converters are operating at 50% duty cycle
and are synchronized. Since the converters are not syn-
chronized and are not both operating at 50% duty cycle,
the actual RMS current will always be less than this.
Losses associated with the input ceramic capacitor are
typically minimal.
Output Capacitor
The output capacitor limits the output ripple and pro-
vides holdup during large load transitions. A 10μF X5R
or X7R ceramic capacitor typically provides sufficient
bulk capacitance to stabilize the output during large load
transitions and has the ESR and ESL characteristics nec-
essary for low output ripple.
VO
⎛
VO
⎞
⎠
·
1 -
⎝
VIN
VIN
The term
appears in both the input voltage
ripple and input capacitor RMS current equations. It is
a maximum when VO is twice VIN. This is why the input
voltage ripple and the input capacitor RMS current ripple
are a maximum at 50% duty cycle.
The output voltage droop due to a load transient is
dominated by the capacitance of the ceramic output
capacitor. During a step increase in load current the
ceramic output capacitor alone supplies the load current
until the loop responds. As the loop responds, the induc-
tor current increases to match the load current demand.
This typically takes several switching cycles and can be
estimated by:
The input capacitor provides a low impedance loop for the
edges of pulsed current drawn by the AAT2515. Low ESR/
ESL X7R and X5R ceramic capacitors are ideal for this
function. To minimize the stray inductance, the capacitor
should be placed as closely as possible to the IC. This
keeps the high frequency content of the input current
localized, minimizing EMI and input voltage ripple.
3 · ΔILOAD
=
COUT
VDROOP · FS
The proper placement of the input capacitor (C3 and C8)
can be seen in the evaluation board layout in Figure 2.
Since decoupling must be as close to the input pins as
possible, it is necessary to use two decoupling capaci-
tors. C3 provides the bulk capacitance required for both
converters, while C8 is a high frequency bypass capaci-
tor for the second channel (see C3 and C8 placement in
Figure 2).
Once the average inductor current increases to the DC
load level, the output voltage recovers. The above equa-
tion establishes a limit on the minimum value for the
output capacitor with respect to load transients.
The internal voltage loop compensation also limits the
minimum output capacitor value to 10μF. This is due to
its effect on the loop crossover frequency (bandwidth),
phase margin, and gain margin. Increased output capac-
itance will reduce the crossover frequency with greater
phase margin.
A laboratory test set-up typically consists of two long
wires running from the bench power supply to the eval-
uation board input voltage pins. The inductance of these
wires, along with the low ESR ceramic input capacitor,
can create a high Q network that may affect converter
performance.
The maximum output capacitor RMS ripple current is
given by:
This problem often becomes apparent in the form of
excessive ringing in the output voltage during load tran-
sients. Errors in the loop phase and gain measurements
can also result.
1
V
OUT · (VIN(MAX) - VOUT
)
IRMS(MAX)
=
·
L · F · VIN(MAX)
2 · 3
Dissipation due to the RMS current in the ceramic output
capacitor ESR is typically minimal, resulting in less than
a few degrees rise in hot spot temperature.
Since the inductance of a short printed circuit board
trace feeding the input voltage is significantly lower than
w w w . a n a l o g i c t e c h . c o m
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