13
LTC1624
100 resistor in series with the SENSE
pin. This offset
cancels the internal offset in current comparator I
2
(refer
to Functional Diagram). This comparator in conjunction
with the voltage on the I
TH
/RUN pin determines when to
enter into Burst Mode operation (refer to Low Current
Operation in Operation section). With the additional exter-
nal offset present, the drive to the topside MOSFET is
always enabled every cycle and constant frequency opera-
tion occurs for I
OUT
> I
OUT(MIN)
.
Step-Down Converter: Design Example
As a design example, assume V
IN
= 12V(nominal),
V
IN
= 22V(max), V
OUT
= 3.3V and I
MAX
= 2A. R
SENSE
can
immediately be calculated:
R
SENSE
= 100mV/2A = 0.05
Assume a 10µH inductor. To check the actual value of the
ripple current the following equation is used:
I
VV
fL
VV
VV
L
IN OUT OUT D
IN D
=
()()
+
+
The highest value of the ripple current occurs at the
maximum input voltage:
I
VV
kHz H
VV
VV
L
=
()
+
+
=
22 3 3
200 10
33 05
22 0 5
158
...
.
.
µ
A
P-P
The power dissipation on the topside MOSFET can be
easily estimated. Choosing a Siliconix Si4412DY results
in: R
DS(ON)
= 0.042, C
RSS
= 100pF. At maximum input
voltage with T(estimated) = 50°C:
P
VV
VV
ACC
V A pF kHz mW
MAIN
=
+
+
()
+
()
°− °
()
[]
()
+
()()( )( )
=
33 05
22 0 5
2 1 0 005 50 25 0 042
2 5 22 2 100 200 62
2
185
..
.
..
.
.
The most stringent requirement for the Schottky diode
occurs when V
OUT
= 0V (i.e. short circuit) at maximum V
IN
.
In this case the worst-case dissipation rises to:
PI V
V
VV
D SC AVG D
IN
IN D
=
()
+
()
APPLICATIONS INFORMATION
WUU
U
With the 0.05 sense resistor I
SC(AVG)
= 2A will result,
increasing the 0.5V Schottky diode dissipation to 0.98W.
C
IN
is chosen for an RMS current rating of at least 1.0A at
temperature. C
OUT
is chosen with an ESR of 0.03 for low
output ripple. The output ripple in continuous mode will be
highest at the maximum input voltage. The output voltage
ripple due to ESR is approximately:
V
ORIPPLE
= R
ESR
(I
L
) = 0.03(1.58A
P-P
) = 47mV
P-P
Step-Down Converter: Duty Cycle Limitations
At high input to output differential voltages the on-time
gets very small. Due to internal gate delays and response
times of the internal circuitry the minimum recommended
on-time is 450ns. Since the LTC1624’s frequency is inter-
nally set to 200kHz a potential duty cycle limitation exists.
When the duty cycle is less than 9%, cycle skipping may
occur which increases the inductor ripple current but does
not cause V
OUT
to lose regulation. Avoiding cycle skipping
imposes a limit on the input voltage for a given output
voltage only when V
OUT
< 2.2V using 30V MOSFETs.
(Remember not to exceed the absolute maximum voltage
of 36V.)
V
IN(MAX)
= 11.1V
OUT
+ 5V For DC > 9%
Boost Converter Applications
The LTC1624 is also well-suited to boost converter appli-
cations. A boost converter steps up the input voltage to a
higher voltage as shown in Figure 6.
Figure 6. Boost Converter
+
C
B
L1
M1
R2
R1
R
SENSE
C
IN
D1
V
IN
1624 F06
V
IN
V
FB
LTC1624
SENSE
BOOST
TG
SW
GND
+
C
OUT
V
OUT
14
LTC1624
Boost Converters: Power MOSFET Selection
One external N-channel power MOSFET must be selected
for use with the LTC1624 for the switch. In boost applica-
tions the source of the power MOSFET is grounded along
with the SW pin. The peak-to-peak gate drive levels are set
by the INTV
CC
voltage. The gate drive voltage is equal to
approximately 5V for V
IN
> 5.6V and a logic level MOSFET
can be used. At V
IN
voltages below 5V the gate drive
voltage is equal to V
IN
– 0.6V and a sublogic level MOSFET
should be used.
Selection criteria for the power MOSFET include the “ON”
resistance R
DS(ON)
, reverse transfer capacitance C
RSS
,
input voltage and maximum output current. When the
LTC1624 is operating in continuous mode the duty cycle
for the MOSFET is given by:
Main Switch Duty Cycle = 1
+
V
VV
IN
OUT D
The MOSFET power dissipation at maximum output cur-
rent is given by:
APPLICATIONS INFORMATION
WUU
U
Boost Converter: Inductor Selection
For most applications the inductor will fall in the range of
10µH to 100µH. Higher values reduce the input ripple
voltage and reduce core loss. Lower inductor values are
chosen to reduce physical size.
The input current of the boost converter is calculated at full
load current. Peak inductor current can be significantly
higher than output current, especially with smaller induc-
tors and lighter loads. The following formula assumes
continuous mode operation and calculates maximum peak
inductor current at minimum V
IN
:
II
V
V
I
L PEAK OUT MAX
OUT
IN MIN
L MAX
() ()
()
()
=
+
2
The ripple current in the inductor (I
L
) is typically 20% to
30% of the peak inductor current occuring at V
IN(MIN)
and
I
OUT(MAX)
.
I
VV V V
kHz L V V
L
IN OUT D IN
OUT D
P-P
()
=
+−
()
()()
+
()
200
with I
L(MAX)
= I
L(P-P)
at V
IN
= V
IN(MIN)
.
Remember boost converters are not short-circuit pro-
tected, and that under output short conditions, inductor
current is limited only by the available current of the input
supply, I
OUT(OVERLOAD)
. Specify the maximum inductor
current to safely handle the greater of I
L(PEAK)
or
I
OUT(OVERLOAD)
. Make sure the inductor’s saturation cur-
rent rating (current when inductance begins to fall)
exceeds the maximum current rating set by R
SENSE
.
Boost Converter: R
SENSE
Selection for Maximum
Output Current
R
SENSE
is chosen based on the required output current.
Remember the LTC1624 current comparator has a maxi-
mum threshold of 160mV/R
SENSE
. The current compara-
tor threshold sets the peak of the inductor current, yielding
a maximum average output current I
OUT(MAX)
equal to
I
L(PEAK)
less half the peak-to-peak ripple current (I
L
),
divided by the output-input voltage ratio (see equation for
I
L(PEAK)
)
.
PI
V
VV
R
k V I C kHz
where I I
VV
V
MAIN IN MAX
IN MIN
OUT D
DS ON
OUT IN MAX RSS
IN MAX OUT MAX
OUT D
IN MIN
=
+
+
()
+
()
()( )
=
+
()
()
()
()
() ()
()
2
185
11
200
δ
.
δ is the temperature dependency of R
DS(ON)
and k is a
constant inversely related to the gate drive current.
MOSFETs have I
2
R losses, plus the P
MAIN
equation
includes an additional term for transition losses that are
highest at high output voltages. For V
OUT
< 20V the high
current efficiency generally improves with larger MOSFETs,
while for V
OUT
> 20V the transition losses rapidly increase
to the point that the use of a higher R
DS(ON)
device with
lower C
RSS
actual provides higher efficiency. For addi-
tional information refer to Step-Down Converter: Power
MOSFET Selection in the Applications Information
section.
15
LTC1624
Allowing a margin for variations in the LTC1624 (without
considering variation in R
SENSE
), assuming 30% ripple
current in the inductor, yields:
R
mV
I
V
VV
SENSE
OUT MAX
IN MIN
OUT D
=
+
()
()
100
Boost Converter: Output Diode
The output diode conducts current only during the switch
off-time. Peak reverse voltage for boost converters is
equal to the regulator output voltage. Average forward
current in normal operation is equal to output current.
Remember boost converters are not short-circuit pro-
tected. Check to be sure the diode’s current rating exceeds
the maximum current set by R
SENSE
. Schottky diodes such
as Motorola MBR130LT3 are recommended.
Boost Converter: Output Capacitors
The output capacitor is normally chosen by its effective
series resistance (ESR), because this is what determines
output ripple voltage.
Since the output capacitor’s ESR affects efficiency, use
low ESR capacitors for best performance. Boost regula-
tors have large RMS ripple current in the output capacitor
that must be rated to handle the current. The output
capacitor ripple current (RMS) is:
CI
VV
V
OUT OUT
OUT IN
IN
I
RIPPLE RMS
()
Output ripple is then simply: V
OUT
= R
ESR
(I
L(RMS)
).
Boost Converter: Input Capacitors
The input capacitor of a boost converter is less critical due
to the fact that the input current waveform is triangular,
and does not contain large square wave currents as found
in the output capacitor. The input voltage source imped-
ance determines the size of the capacitor that is typically
10µF to 100µF. A low ESR is recommended although not
as critical as the output capacitor and can be on the order
of 0.3. Input capacitor ripple current for the LTC1624
used as a boost converter is:
APPLICATIONS INFORMATION
WUU
U
C
VV V
kHz L V
IN
IN OUT IN
OUT
I
RIPPLE
()
()
()()()
03
200
.
The input capacitor can see a very high surge current when
a battery is suddenly connected and solid tantalum capaci-
tors can fail under this condition. Be sure to specify surge
tested capacitors.
Boost Converter: Duty Cycle Limitations
The minimum on-time of 450ns sets a limit on how close
V
IN
can approach V
OUT
without the output voltage over-
shooting and tripping the overvoltage comparator. Unless
very low values of inductances are used, this should never
be a problem. The maximum input voltage in continuous
mode is:
V
IN(MAX)
= 0.91V
OUT
+ 0.5V For DC = 9%
SEPIC Converter Applications
The LTC1624 is also well-suited to SEPIC (Single Ended
Primary Inductance Converter) converter applications.
The SEPIC converter shown in Figure 7 uses two induc-
tors. The advantage of the SEPIC converter is the input
voltage may be higher or lower than the output voltage.
The first inductor L1 together with the main N-channel
MOSFET switch resemble a boost converter. The second
inductor L2 and output diode D1 resemble a flyback or
buck-boost converter. The two inductors L1 and L2 can be
independent but also can be wound on the same core since
Figure 7. SEPIC Converter
+
+
C
B
L1
L2
M1
R2
R1
R
SENSE
C
IN
D1
C1
V
IN
1624 F07
V
IN
V
FB
LTC1624
SENSE
BOOST
TG
SW
GND
+
C
OUT
V
OUT

LTC1624IS8#TRPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators Hi Eff SO-8 N-Ch Sw Reg Cntr
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