22
LTC1709-8/LTC1709-9
estimated using the percentage of overshoot seen at this
pin. The bandwidth can also be estimated by examining
the rise time at the pin. The I
TH
external components
shown in the Figure 1 circuit will provide an adequate
starting point for most applications.
The I
TH
series R
C
-C
C
filter sets the dominant pole-zero
loop compensation. The values can be modified slightly
(from 0.2 to 5 times their suggested values) to optimize
transient response once the final PC layout is done and the
particular output capacitor type and value have been
determined. The output capacitors need to be decided
upon because the various types and values determine the
loop gain and phase. An output current pulse of 20% to
80% of full-load current having a rise time of <2µs will
produce output voltage and I
TH
pin waveforms that will
give a sense of the overall loop stability without breaking
the feedback loop. The initial output voltage step resulting
from the step change in output current may not be within
the bandwidth of the feedback loop, so this signal cannot
be used to determine phase margin. This is why it is
better to look at the Ith pin signal which is in the feedback
loop and is the filtered and compensated control loop
response. The gain of the loop will be increased by
increasing R
C
and the bandwidth of the loop will be
increased by decreasing C
C
. If R
C
is increased by the
same factor that C
C
is decreased, the zero frequency will
be kept the same, thereby keeping the phase the same in
the most critical frequency range of the feedback loop.
The output voltage settling behavior is related to the
stability of the closed-loop system and will demonstrate
the actual overall supply performance.
Automotive Considerations: Plugging into the
Cigarette Lighter
As battery-powered devices go mobile, there is a natural
interest in plugging into the cigarette lighter in order to
conserve or even recharge battery packs during opera-
tion. But before you connect, be advised: you are plugging
into the supply from hell. The main battery line in an
automobile is the source of a number of nasty potential
transients, including load-dump, reverse-battery, and
double-battery.
Load-dump is the result of a loose battery cable. When the
cable breaks connection, the field collapse in the alternator
can cause a positive spike as high as 60V which takes
several hundred milliseconds to decay. Reverse-battery is
just what it says, while double-battery is a consequence of
tow truck operators finding that a 24V jump start cranks
cold engines faster than 12V.
The network shown in Figure 9 is the most straightfor-
ward approach to protect a DC/DC converter from the
ravages of an automotive power line. The series diode
prevents current from flowing during reverse-battery,
while the transient suppressor clamps the input voltage
during load-dump. Note that the transient suppressor
should not conduct during double-battery operation, but
must still clamp the input voltage below breakdown of the
converter. Although the LT1709 has a maximum input
voltage of 36V, most applications will be limited to 30V by
the MOSFET BV
DSS
.
APPLICATIO S I FOR ATIO
WUU
U
Figure 9. Automotive Application Protection
V
IN
170989 F09
12V
50A I
PK
RATING
TRANSIENT VOLTAGE
SUPPRESSOR
GENERAL INSTRUMENT
1.5KA24A
LTC1709
23
LTC1709-8/LTC1709-9
Design Example
As a design example, assume V
IN
= 5V (nominal), V
IN
=␣ 5.5V
(max), V
OUT
= 1.8V, I
MAX
= 20A, T
A
= 70°C and f␣ =␣ 300kHz.
The inductance value is chosen first based on a 30% ripple
current assumption. The highest value of ripple current
occurs at the maximum input voltage. Tie the PLLFLTR pin
to the INTV
CC
pin for 300kHz operation. The minimum
inductance for 30% ripple current is:
L
V
fI
V
V
V
kHz
A
V
V
H
OUT OUT
IN
()
()()
≥µ
1
18
300 30
20
2
1
18
55
135
.
%
.
.
.
A 1.5µH inductor will produce 27% ripple current. The
peak inductor current will be the maximum DC value plus
one half the ripple current, or 11.4A. The minimum on-
time occurs at maximum V
IN
:
t
V
Vf
V
V kHz
s
ON MIN
OUT
IN
()
==
()( )
18
5 5 300
11
.
.
.
The R
SENSE
resistors value can be calculated by using the
maximum current sense voltage specification with some
accomodation for tolerances:
R
mV
A
SENSE
=≈
50
11 4
0 004
.
.
The power dissipation on the topside MOSFET can be
easily estimated. Using a Siliconix Si4420DY for example;
R
DS(ON)
= 0.013, C
RSS
= 300pF. At maximum input
voltage with T
J
(estimated) = 110°C at an elevated ambient
temperature:
P
V
V
CC
V
A
pF
kHz W
MAIN
=
()
+
()
°− °
()
[]
+
()
()
()
=
18
55
10 1 0 005 110 25
0013 1755
20
2
300
300 0 65
2
2
.
.
.
...
.
The worst-case power disipated by the synchronous
MOSFET under normal operating conditions at elevated
ambient temperature and estimated 50°C junction tem-
perature rise is:
P
VV
V
A
W
SYNC
=
()
()
=
55 18
55
20
2
1 48 0 013
129
2
..
.
..
.
A short-circuit to ground will result in a folded back current
of about:
I
mV
ns V
H
A
SC
=
+
()
µ
=
25
0 004
1
2
200 5 5
15
66
.
.
.
.
The worst-case power disipated by the synchronous
MOSFET under short-circuit conditions at elevated ambi-
ent temperature and estimated 50°C junction temperature
rise is:
P
VV
V
A
mW
SYNC
=
()()
()
=
55 18
55
66 148 0013
564
2
..
.
...
which is less than half of the normal, full-load dissipation.
Incidentally, since the load no longer dissipates power in
the shorted condition, total system power dissipation is
decreased by over 99%.
The duty factor for this application is:
DF
V
V
V
V
O
IN
== =
18
5
036
.
.
APPLICATIO S I FOR ATIO
WUU
U
24
LTC1709-8/LTC1709-9
APPLICATIO S I FOR ATIO
WUU
U
Using Figure 4, the RMS ripple current will be:
I
INRMS
= (20A)(0.23) = 4.6A
RMS
An input capacitor(s) with a 4.6A
RMS
ripple current rating
is required.
The output capacitor ripple current is calculated by using
the inductor ripple already calculated for each inductor
and multiplying by the factor obtained from Figure␣ 3
along with the calculated duty factor. The output ripple in
con
tinuous mode will be highest at the maximum input
voltage since the duty factor is <50%. The maximum
output current ripple is:
I
V
fL
at DF
I
V
kHz H
A
VmAmV
COUT
OUT
COUTMAX
RMS
OUTRIPPLE RMS RMS
=
()
=
()
µ
()
=
=Ω
()
=
03 33
18
300 1 5
03
12
20 1 2 24
.%
.
.
.
.
.
PC Board Layout Checklist
When laying out the printed circuit board, the following
checklist should be used to ensure proper operation of the
LTC1709. These items are also illustrated graphically in
the layout diagram of Figure␣ 10. Check the following in
your layout:
1) Are the signal and power grounds segregated? The
LTC1709 signal ground pin should return to the (–) plate
of C
OUT
separately. The power ground returns to the
sources of the bottom N-channel MOSFETs, anodes of the
Schottky diodes, and (–) plates of C
IN
, which should have
as short lead lengths as possible.
2) Does the LTC1709 V
OS
+
pin connect to the point of
load? Does the LTC1709 V
OS
pin connect to the load
return?
3) Are the SENSE
and SENSE
+
leads routed together with
minimum PC trace spacing? The filter capacitors between
SENSE
+
and SENSE
pin pairs should be as close as
possible to the LTC1709. Ensure accurate current sensing
with Kelvin connections at the current sense resistor.
4) Does the (+) plate of C
IN
connect to the drains of the
topside MOSFETs as closely as possible? This capacitor
provides the AC current to the MOSFETs. Keep the input
current path formed by the input capacitor, top and bottom
MOSFETs, and the Schottky diode on the same side of the
PC board in a tight loop to minimize conducted and
radiated EMI.
5) Is the INTV
CC
1µF ceramic decoupling capacitor con-
nected closely between
INTV
CC
and the power ground pin?
This capacitor carries the MOSFET driver peak currents. A
small value is recommended to allow placement immedi-
ately adjacent to the IC.
6) Keep the switching nodes, SW1 (SW2), away from
sensitive small-signal nodes. Ideally the switch nodes
should be placed at the furthest point from the LTC1709.
7) Use a low impedance source such as a logic gate to drive
the PLLIN pin and keep the lead as short as possible.
The diagram in Figure 10 illustrates all branch currents in
a 2-phase switching regulator. It becomes very clear after
studying the current waveforms why it is critical to keep
the high-switching-current paths to a small physical size.
High electric and magnetic fields will radiate from these
“loops” just as radio stations transmit signals. The output
capacitor ground should return to the negative terminal of
the input capacitor and not share a common ground path
with any switched current paths. The left half of the circuit
gives rise to the “noise” generated by a switching regula-
tor. The ground terminations of the sychronous MOSFETs
and Schottky diodes should return to the negative plate(s)
of the input capacitor(s) with a short isolated PC trace
since very high switched currents are present. A separate
isolated path from the negative plate(s) of the input
capacitor(s) should be used to tie in the IC power ground
pin (PGND) and the signal ground pin (SGND). This
technique keeps inherent signals generated by high cur-
rent pulses from taking alternate current paths that have
finite impedances during the total period of the switching
regulator. External OPTI-LOOP compensation allows over-
compensation for PC layouts which are not optimized but
this is not the recommended design procedure.

LTC1709EG-8#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators Hi Pwr PolyPhase DC/DC Controllers
Lifecycle:
New from this manufacturer.
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