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SIC401DB Datasheet(PDF) 22 Page - Vishay Siliconix

Part # SIC401DB
Description  15 A microBUCK SiC401A/B Integrated Buck Regulator with Programmable LDO
PDF  28 Pages
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Manufacturer  VISHAY [Vishay Siliconix]
Direct Link  http://www.vishay.com
Logo VISHAY - Vishay Siliconix

SIC401DB Datasheet(HTML) 22 Page - Vishay Siliconix

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Document Number: 63835
S12-2109-Rev. C, 03-Sep-12
Vishay Siliconix
SiC401A, SiC401BCD
www.vishay.com
22
Document Number: 63835
S12-2109-Rev. C, 03-Sep-12
This document is subject to change without notice.
THE PRODUCTS DESCRIBED HEREIN AND THIS DOCUMENT ARE SUBJECT TO SPECIFIC DISCLAIMERS, SET FORTH AT www.vishay.com/doc?91000
For technical questions, contact: powerictechsupport@vishay.com
Using Ceramic Output Capacitors
When the system is using high ESR value capacitors, the
feedback voltage ripple lags the phase node voltage by 90°.
Therefore, the converter is easily stabilized. When the
system is using ceramic output capacitors, the ESR value is
normally too small to meet the above ESR criteria. As a
result, the feedback voltage ripple is 180° from the phase
node and behaves in an unstable manner. In this application
it is necessary to add a small virtual ESR network that is
composed of two capacitors and one resistor, as shown in
figure 14.
The ripple voltage at FB is a superposition of two voltage
sources: the voltage across CL and output ripple voltage.
They are defined in the following equations.
Figure 15 shows the magnitude of the ripple contribution due
to CL at the FB pin.
It is shown by the following equation.
Figure 16 shows the magnitude of the ripple contribution due
to the output voltage ripple at the FB pin.
It is shown by the following equation.
The purpose of this network is to couple the inductor current
ripple information into the feedback voltage such that the
feedback voltage has 90° phase lag to the switching node
similar to the case of using standard high ESR capacitors.
This is illustrated in figure 17.
The magnitude of the feedback ripple voltage, which is
dominated by the contribution from CL, is controlled by the
value of R1, R2 and CC. If the corner frequency of (R1//R2) x
CC is too high, the ripple magnitude at the FB pin will be
smaller, which can lead to double-pulsing. Conversely, if the
corner frequency of (R1//R2) x CC is too low, the ripple
magnitude at FB pin will be higher. Since the SiC401A/B
regulates to the valley of the ripple voltage at the FB pin, a
high ripple magnitude is undesirable as it significantly
impacts the output voltage regulation. As a result, it is
desirable to select a corner frequency for (R1//R2) x CC to
achieve enough, but not excessive, ripple magnitude and
phase margin. The component values for R1, R2, and CC
should be calculated using the following procedure.
Select CL (typical 10 nF) and RL to match with L and DCR
time constant using the following equation.
Figure 14 - Virtual ESR Ramp Current
Figure 15 - FB Voltage by CL Voltage
V
CL =
IL x DCR (s x L/DCR + 1)
S x RL x CL + 1
ΔV
OUT =
ΔIL
8C x fSW
VFB
CL = VCL x
(R1//R2) x S x CC
(R1//R2) x S x CC + 1
Figure 16 - FB Voltage by Output Voltage
Figure 17 - FB Voltage in Phasor Diagram
VFB
ΔV
OUT = ΔVOUT x
R2
R1//
+ R2
S x CC
1



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