LTC4417
16
4417f
applicaTions inForMaTion
where R
S
and C
S
are component values shown in Figure8.
The selection of R
S
and C
L
involves an iterative process.
Begin by assuming 0.79 R
S
C
S
= 10µs and choosing
C
L
using Equation (14). See the Inrush Current and Input
Voltage Droop section for more details regarding inrush
current limiting circuitry, and for selecting R
S
.
Figure 8. Slew Rate Limiting Gate Drive
C
IN1
68µF
C
S
VS1
LTC4417
G1
V
OUT
V
OUT
4417 F08
R
S
D
S
BAT54
12V WALL
ADAPTER
V1
IRF7324
M1 M2
+
C
L
47µF
+
C
VS1
channel disconnects or 32ms has elapsed. Once soft-start
has terminated, the gate driver quickly turns on and off
external back-to-back P-channel MOSFETs as needed. A
SHDN low to high transition or V
OUT
drooping below 0.7V
reactivates soft-start.
INRUSH CURRENT AND INPUT VOLTAGE DROOP
When switching control of V
OUT
from a lower voltage supply
to a higher voltage supply, the higher voltage supply may
experience significant voltage droop due to high inrush
current during a fast connection to a lower voltage output
bulk capacitor with low ESR. This high inrush current may
be sufficient to trigger an undesirable UV Fault.
To prevent a UV fault when connecting a higher voltage
input to a lower voltage output, without adding any inrush
current limiting, size the input bypass capacitor large
enough to provide the required inrush current, as shown
by Equation (15).
C
V1
C
L
V1 V
OUT(INIT)
V1
DROOP
1
(15)
where V
OUT(INIT)
is the initial output voltage when being
powered from a supply voltage less than V1, C
V1
is the
bypass capacitor connected to V1, C
L
is the output capaci-
tor and V1
DROOP
is the maximum allowed voltage droop
on V1. Make sure C
V1
is a low ESR capacitor to minimize
the voltage step across the ESR.
In situations where input and output capacitances can-
not be chosen to set the desired maximum input voltage
droop, or the peak inrush current violates the maximum
Pulsed Drain Current (I
DM
) of the external P-channel MOS-
FETs, inrush current can be limited by slew rate limiting
the output voltage. The gate driver can be configured to
slew rate limit the output with a resistor, capacitor and
Schottky diode, as shown in Figure 8. The series resistor
R
S
and capacitor, C
S
, slew rate limit the output, while the
Schottky diode, D
S
, provides a fast turn off path when G1
is pulled to VS1.
With a desired input voltage drop, V1
DROOP
, and known
supply resistance R
SRC
, the series resistance, R
S
, can
be calculated with Equation (16), whereV
G(SINK)
is
the LTC4417’s sink clamp voltage, V
GS
is the external
GATE DRIVER
When turning a channel on, the LTC4417 pulls the common
gate connection (G1, G2 and G3) down with a P-channel
source follower and aA current source. VS1, VS2 and
VS3 voltages at or above 5V will produce rising slew rates
of 12Vs and falling slew rates of 4Vs with 10nF between
the VS and G pins. VS1, VS2 and VS3 voltages lower than
5V will result in lower slew rates, see typical curves for
more detail. As G1, G2 and G3 approaches the 6.2V clamp
voltage, the source follower smoothly reduces its current
while theA hold current continues to pull G1, G2 and
G3 to the final clamp voltage, back biasing the source
follower. Clamping the G1, G2 and G3 voltage prevents
any overvoltage stress on the gate to source oxide of the
external back-to-back P-channel MOSFETs. If leakage into
G1, G2 and G3 exceeds theA hold current, the G1, G2
and G3 voltage will rise above the clamp voltage, where
the source follower enhances to sink the excess current.
When turning a channel off, the gate driver
pulls the com-
mon
gate to the common source with a switch having an
on-resistance of 16Ω, to effect a quick turn-off.
To minimize inrush current at start-up, the gate driver soft-
starts the gate drive of the first input to connect to V
OUT
.
The gate pin is regulated to create a constant 5V/ms rise
rate on V
OUT
. Slew rate control is terminated when any
LTC4417
17
4417f
applicaTions inForMaTion
P-channel’s gate to source voltage when driving the load
and inrush current, C
S
is the slew rate capacitor and C
L
is the V
OUT
hold up capacitance. The output load current
I
L
is neglected for simplicity. Choose C
S
to be at least ten
times the external P-channel MOSFET’s C
RSS(MAX)
, and
C
VS
to be ten times C
S
.
R
S
ΔV
G(SINK)
V
GS
( )
C
L
R
SRC
C
S
V1
DROOP
(16)
Use Equation (17) to verify the inrush current limit is lower
than the absolute maximum pulsed drain current, I
DM
.
I
INRUSH
=
V1
DROOP
R
SRC
(17)
If the external P-channel MOSFET’s reverse transfer
capacitance, C
RSS
, is used instead of C
S
, replace C
S
with
C
RSS
in Equation (16), where C
RSS
is taken at the minimum
V
DS
voltage, and calculate for R
S
. Depending on the size
of C
RSS
, R
S
may be large. Care should be used to ensure
gate leakages do not inadvertently turn off the channel over
temperature. This is particularly true of built in Zener gate-
source protected devices. Careful bench characterization
is strongly recommended, as C
RSS
is non-linear.
The preceding analysis assumes a small input inductance
between the input supply voltage and the drain of the ex-
ternal P-channel MOSFET. If the input inductance is large,
choose C
V1
to be much greater than C
L
and replace R
SRC
with the ESR of C
V1
.
When slew rate limiting the output, ensure power dis-
sipation does not exceed the manufacturer’s SOA for the
chosen external P-channel MOSFET. Refer to the Selecting
External P-channel MOSFETs section.
TRANSIENT SUPPLY PROTECTION
The LTC4417’s abrupt switching due to OV or UV faults
can create large transient overvoltage events with inductive
input supplies, such as supplies connected
by a long cable
.
At times the transient overvoltage condition can exceed
twice the nominal voltage. Such events can damage external
devices and the LTC4417. It is imperative that external
back-to-back P-channel MOSFET devices do not exceed
their single pulse avalanche energy specification (EAS) in
unclamped inductive applications and input voltages to the
LTC4417 never exceed the Absolute Maximum Ratings.
To minimize inductive voltage spikes, use wider and/or
heavier trace plating. Adding a snubber circuit will dampen
input voltage spikes as discussed in Linear Application
Note 88, and a transient surge suppressor at the input will
clamp the voltage. Transient voltage suppressors (TVS)
should be placed on any input supply pin, V1, V2 and V3,
where input shorts, or reverse voltage connection can be
made. If short-circuit of input sources powering V
OUT
are
possible, transient voltage suppressors should also be
placed on V
OUT
, as shown in Figure 9.
When selecting transient voltage suppressors, ensure the
reverse standoff voltage (V
R
) is equal to or greater than
the application operating voltage, the peak pulse current
(I
PP
) is higher than the peak transient voltage divided by
the source impedance, the maximum clamping voltage
(V
CLAMP
) at the rated I
PP
is less than the absolute maxi-
mum ratings of the LTC4417 and BV
DSS
of all the external
back-to-back P-channel MOSFETs.
In applications below 20V, transient voltage suppressors
may not be required if the voltage spikes are lower than the
BV
DSS
of the external P-channel MOSFETs and the LTC4417
Figure 9. Transient Voltage Suppression
FDD4685 FDD4685
M1 M2
24V WALL
ADAPTER
VS1 G1
V
OUT
LTC4417
INPUT
PARASITIC
INDUCTANCE
OUTPUT
PARASITIC
INDUCTANCE
C
V1
0.1µF
C
SN
R
SN
C
OUT
10µF
C
L
330µF
V
OUT
OR
4417 F09
D2
SMBJ26A
D1
SMBJ26CA
OR
+
SNUBBER
LTC4417
18
4417f
Absolute Maximum Ratings. If the BV
DSS
of the external
P-channel MOSFET is momentarily exceeded, ensure the
avalanche energy absorbed by the MOSFETs do not exceed
the single pulse avalanche energy specification (EAS).
Voltage spikes can be dampened further with a snubber.
INPUT SUPPLY AND V
OUT
SHORTS
Input shorts can cause high current slew rates. Coupled
with series parasitic inductances in the input and output
paths, potentially destructive transients may appear at the
input and output pins. If the short occurs on an input that
is not powering V
OUT
, the impact to the system is benign.
Back-to-back P-channel MOSFETs with their common gates
connected to their common sources naturally prevent any
current flow regardless of the applied voltages on either
side of the drain connections, as long as the BV
DSS
is not
exceeded.
If the short occurs on an input that is powering V
OUT
, the
issue is compounded by high conduction current and low
impedance connection to the output via the back-to-back
P-channel MOSFETs. Once the LTC4417 blocks the high
input short current, V1, V2 and V3 may experience large
negative voltage spikes while the output may experience
large positive voltage
spikes.
To prevent damage to the LTC4417 and associated de-
vices in the event of an input or output short, it may be
necessary to protect the input pins and output pins as
shown in Figure 9. Protect the input pins, V1, V2 and V3,
with either unidirectional or bidirectional TVS and V
OUT
with a unidirectional TVS. An input and output capacitor
between 0.1µF and 10µF with intentional or parasitic series
resistance will aid in dampening voltage spikes; see Linear
Technology’s Application Note 88 for general consideration.
Due to the low impedance connection from V1, V2 and V3
to V
OUT
, shorts to the output will result in an input supply
UV fault. If the UV threshold is high enough and the short
resistive enough, the LTC4417 will disconnect the input.
The fast change in current may force the output below
GND, while the input will increase in voltage.
If UV thresholds are set close to the minimum operating
voltage of the LTC4417, it may not disconnect the input
Figure 10. R-C Filter to Ride Through Input Shorts
C
F
10nF
R
F
100Ω
VS3
LTC4417
G3VS2 G2
V
OUT
V
OUT
OUTPUT
4417 F10
IRF7324
M5 M6
IRF7324
M3 M4
C
L
I
L
+
applicaTions inForMaTion
from the output before the output is dragged below the
operating voltage of the LTC4417. The event would cause
the LTC4417’s internal V
LDO
supply voltage to collapse. A
100Ω and 10nF R-C filter on V
OUT
will allow the LTC4417
to ride through such shorts to the input and output, as
shown in Figure 10. Because V
OUT
is also a sense pin
for the REV comparator, care should be taken to ensure
the voltage drop across the resistor is low enough to not
affect the reverse comparator’s threshold. If thes R-C
time constant does not address the issue, increase the
capacitance to lengthen the time constant.
The initial lag due to the R-C filter on the LTC4417’s V
OUT
sense and supply pin will cause additional delay in sensing
when a reverse condition has cleared, resulting in addi-
tional droop when transitioning from a higher voltage to
a lower voltage. If the reverse voltage duration is longer
than the R-C delay, the voltage differential between the
output and the filtered V
OUT
, ∆V, can be calculated with
Equation (18). I
L
is the output load current during the
reverse voltage condition and I
VOUT
is current into V
OUT
,
specified in the electrical table.
ΔV =
I
L
C
L
C
F
I
VOUT
R
F
(18)
I
CC
PAT H SELECTION
Tw o separate internal power rails ensure the LTC4417 is
functional when one or more input supplies are present
and above 2.4V as well as limit current draw from lower

LTC4417HUF#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Power Management Specialized - PMIC 2.5V to 36V Prioritized Triple PowerPath Controller
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