10
LTC1530
1530fa
Figure 5b plots the minimum required R
IMAX
resistor (k)
versus the maximum operating load current (I
LMAX
=
I
LOAD
+ I
RIPPLE
/2) as a function of Q1’s R
DS(ON)
. Note that
during an intial power-up sequence (V
OUT
= 0V), the
inductor’s start-up current I
ST
is much higher than the
steady-state condition, I
LMAX
. The difference between I
ST
and I
LMAX
is affected by the input power supply slew rate,
the input and output voltages, the LTC1530 soft-start slew
rate, the maximum duty cycle and the inductor and output
capacitor values.
For a given application, the input and output requirements
are known and determine the main inductor and output
capacitor values. These values establish the transient load
recovery time. In general, a low value inductor combined
with high value output capacitance has a short transient
load recovery time at the expense of higher inductor ripple
and start-up current (I
RIPPLE
and I
ST
). However, if a small
inductor and large value output capacitors are chosen, the
value of R
IMAX
obtained from Figure 5b may be too small
to allow proper regulator start-up.
During start-up, if I
ST
is higher than the current limit
threshold set by the R
IMAX
resistor, the LTC1530 current
limit comparator turns on. This comparator then limits
input charging current by reducing duty cycle. During this
time, if V
OUT
doesn’t increase above one-half of the rated
value, the LTC1530 hard current limit circuit turns on. This
circuit forces the LTC1530 to repeat a soft-start cycle and
the power supply fails to start. If V
OUT
increases above
one-half of the rated value, the power supply output may
start-up properly depending on whether the limited input
current charges the output capacitor and prevents hard
current limit action.
Therefore, select R
IMAX
with the start-up current (I
ST
) in
mind. Choosing R
IMAX
to set the current comparator
threshold above I
ST
ensures proper power supply start-up
as well as recovery from an output fault condition.
Figures 6a and 6b plot the start-up I
ST
vs output capaci-
tance and inductance for unloaded and loaded conditions
with the current limit circuit disabled. Figures 6a and 6b
are provided as examples. Actual I
ST
under start-up con-
ditions must be measured for any application circuit so
that R
IMAX
can be properly chosen.
I
LMAX
(A)
0
MINIMUM REQUIRED R
IMAX
()
5500
4500
3500
2500
1500
500
16 18
1530 F05b
426
810 14
12
20
R
IMAX
500
I
LMAX
= I
LOAD
+ I
RIPPLE
/2
Q1 R
DS(ON)
= 0.05
0.04
0.03
0.02
0.01
Figure 5b. Minimum Required R
IMAX
vs I
LMAX
OUTPUT CAPACITANCE (mF)
0
START-UP I
ST
(A)
25
20
15
10
5
0
2
468
1530 F06a
10 12
T
A
= 25°C
V
IN
= 5V
I
LOAD
= 0A
L = 1.2µH
L = 4.7µH
L = 2.4µH
Figure 6a. Start-Up I
ST
vs Output Capacitance
OUTPUT CAPACITANCE (mF)
0
START-UP I
ST
(A)
30
25
20
15
10
5
0
2
468
1530 F06b
10 12
T
A
= 25°C
V
IN
= 5V
I
LOAD
= 10A
L = 1.2µH
L = 4.7µH
L = 2.4µH
Figure 6b. Start-Up I
ST
vs Output Capacitance
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LTC1530
1530fa
Power MOSFETs
Two N-channel power MOSFETs are required for synchro-
nous LTC1530 circuits. They should be selected based
primarily on threshold voltage and on-resistance consid-
erations. Thermal dissipation is often a secondary con-
cern in high efficiency designs. The required MOSFET
threshold should be determined based on the available
power supply voltages and/or the complexity of the gate
drive charge pump scheme. In 5V input designs where a
12V supply is used to power PV
CC
, standard MOSFETs
with R
DS(ON)
specified at V
GS
= 5V or 6V can be used with
good results. The current drawn from the 12V supply
varies with the MOSFETs used and the LTC1530’s operat-
ing frequency, but is generally less than 50mA.
LTC1530 applications that use a 5V V
IN
voltage and a
doubling charge pump to generate PV
CC
do not provide
enough gate drive voltage to fully enhance standard
power MOSFETs. Under this condition, the effective
MOSFET R
DS(ON)
may be quite high, raising the dissipa-
tion in the FETs and reducing efficiency. In addition,
power supply start-up problems can occur with standard
power MOSFETs. These start-up problems can occur for
two reasons. First, if the MOSFET is not fully enhanced,
the higher effective R
DS(ON)
causes the LTC1530 to acti-
vate current limit at a much lower level than the desired
trip point. Second, standard MOSFETs have higher GATE
threshold voltages than logic level MOSFETs, thereby
increasing the PV
CC
voltage required to turn them on. A
MOSFET whose R
DS(ON)
is rated at V
GS
= 4.5V does not
necessarily have a logic level MOSFET GATE threshold
voltage. Logic level FETs are the recommended choice for
5V-only systems. Logic level FETs can be fully enhanced
with a doubler charge pump and will operate at maximum
efficiency. Note that doubler charge pump designs run-
ning from supplies higher than 6.5V should include a
Zener diode clamp at PV
CC
to prevent transients from
exceeding the absolute maximum rating of the pin.
After the MOSFET threshold voltage is selected, choose
the R
DS(ON)
based on the input voltage, the output voltage,
allowable power dissipation and maximum output cur-
rent. In a typical LTC1530 buck converter circuit, operat-
ing in continuous mode, the average inductor current is
equal to the output load current. This current flows through
+
+
0.22µF
10µF
+
C
O
C
IN
L
O
MBR0530T1 MBR0530T1
OPTIONAL FOR
V
IN
> 6.5V
LTC1530
PV
CC
G1
V
OUT
1530 F07
V
IN
13V
1N5243B
Q1
Q2
G2
In order for the current limit circuit to operate properly and
to obtain a reasonably accurate current limit threshold, the
I
MAX
and I
FB
pins must be Kelvin sensed at Q1’s drain and
source pins. A 0.1µF decoupling capacitor can also be
connected across R
IMAX
to filter switching noise. In addi-
tion, LTC recommends that the voltage drop across the
R
IMAX
resistor be set to 100mV. Otherwise, noise spikes
or ringing at Q1’s source can cause the actual current limit
to be greater than the desired current limit set point.
MOSFET Gate Drive
The PV
CC
supply must be greater than the input supply
voltage, V
IN
, by at least one power MOSFET V
GS(ON)
for
efficient operation. This higher voltage can be supplied
with a separate supply, or it can be generated using a
simple charge pump as shown in Figure 7. The 86%
maximum duty cycle ensures sufficient off-time to refresh
the charge pump during each cycle.
As PV
CC
is powered up from 0V, the LTC1530 undervolt-
age lockout circuit prevents G1 and G2 from pulling high
until PV
CC
reaches about 3.5V. To prevent Q1’s high
R
DS(ON)
from triggering the current limit comparator while
PV
CC
is slewing, the current limit circuit is disabled until
PV
CC
is8V. In addition, on start-up or recovery from
thermal shutdown, the driver logic is designed to hold G2
low until G1 first goes high.
Figure 7. Doubling Charge Pump
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LTC1530
1530fa
Note that while the required R
DS(ON)
values suggest large
MOSFETs, the power dissipation numbers are only 1.39W
per device or lesslarge TO-220 packages and heat
sinks are not necessarily required in high efficiency appli-
cations. Siliconix Si4410DY or International Rectifier
IRF7413 (both in SO-8) or Siliconix SUD50N03 or Motorola
MTD20N03HDL (both in DPAK) are small footprint sur-
face mount devices with R
DS(ON)
values below 0.03 at 5V
of V
GS
that work well in LTC1530 circuits. With higher
output voltages, the R
DS(ON)
of Q1 may need to be signifi-
cantly lower than that for Q2. These conditions can often
be met by paralleling two MOSFETs for Q1 and using a
single device for Q2. Using a higher P
MAX
value in the
R
DS(ON)
calculations generally decreases the MOSFET
cost and the circuit efficiency and increases the MOSFET
heat sink requirements.
In most LTC1530 applications, R
DS(ON)
is used as the
current sensing element. MOSFET R
DS(ON)
has a positive
temperature coefficient. Therefore, the LTC1530 I
MAX
sink
current is designed with a positive 3300ppm/°C tempera-
ture coefficient. The positive tempco of I
MAX
provides first
order correction for current limit vs temperature. There-
fore, current limit does not have to be set to an increased
level at room temperature to guarantee a desired output
current at elevated temperatures.
Table 1 highlights a variety of power MOSFETs that are
suitable for use in LTC1530 applications.
Inductor Selection
The inductor is often the largest component in an LTC1530
design and must be chosen carefully. Choose the inductor
value and type based on output slew rate requirements
and expected peak current. The required output slew rate
primarily controls the inductor value. The maximum rate
of rise of inductor current is set by the inductor’s value, the
input-to-output voltage differential and the LTC1530’s
maximum duty cycle. In a typical 5V input, 2.8V output
application, the maximum rise time will be:
DC
VV
LL
MAX
IN OUT
=
185.
A
sµ
either Q1 or Q2 with the power dissipation split up accord-
ing to the duty cycle:
DC Q
V
V
DC Q
V
V
VV
V
OUT
IN
OUT
IN
IN OUT
IN
()
()
1
21
=
=− =
()
The R
DS(ON)
required for a given conduction loss can now
be calculated by rearranging the relation P = I
2
R.
R
P
DC Q I
VP
V
I
R
P
DC Q I
VP
VV
I
DS ON Q
MAX Q
MAX
IN MAX Q
OUT
MAX
DS ON Q
MAX Q
MAX
IN MAX Q
IN OUT
MAX
()
()
()
()
()
()
()
()
1
1
2
1
2
2
2
2
2
2
1
2
=
[]
()
=
()
[]
()
()
=
[]
()
=
()
[]
()
()
P
MAX
should be calculated based primarily on required
efficiency or allowable thermal dissipation. A high efficiency
buck converter designed for the Pentium
II with 5V input
and a 2.8V, 11.2A output might allow no more than 4%
efficiency loss at full load for each MOSFET. Assuming
roughly 90% efficiency at this current level, this gives a P
MAX
value of:
(2.8)(11.2A/0.9)(0.04) = 1.39W per FET
and a required R
DS(ON)
of:
R
VW
VA
R
VW
VV A
DS ON Q
DS ON Q
()
()
.
..
.
.
..
.
1
2
2
2
5139
2 8 11 2
0 020
5139
528112
0 025
=
()
=
=
()
()
=
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LTC1530IS8-2.8#TRPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators Syn Cntrler w/Current Limit
Lifecycle:
New from this manufacturer.
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