7
LTC1149
LTC1149-3.3/LTC1149-5
TEST CIRCUIT
APPLICATIO S I FOR ATIO
WUU U
Typical Application Circuit
The basic LTC1149 series application circuit is shown in
Figure 1. External component selection is driven by the
input voltage and output load requirement, and begins
with the selection of R
SENSE
. Once R
SENSE
is known, C
T
and L can be chosen. Next, the power MOSFETs and D1
are selected. Finally, C
IN
and C
OUT
are selected and the
loop is compensated. The circuit shown in Figure 1 can be
configured for operation up to an input voltage of 48V. If
the application does not require greater than 15V opera-
tion, then the LTC1148 should be used.
R
SENSE
Selection for Output Current
R
SENSE
is chosen based on the required output current.
The LTC1149 series current comparator has a threshold
range which extends from a minimum of 25mV/R
SENSE
to
a maximum of 150mV/R
SENSE
. The current comparator
threshold sets the peak of the inductor ripple current,
yielding a maximum output current I
MAX
equal to the peak
value less half the peak-to-peak ripple current.
For proper
Burst Mode
operation, I
RIPPLE(P-P)
must be less than or
equal to the minimum current comparator threshold.
Since efficiency generally increases with ripple current,
the maximum allowable ripple current is assumed, i.e.,
I
RIPPLE(P-P)
= 25mV/R
SENSE
(see C
T
and L Selection for
Operating Frequency). Solving for R
SENSE
and allowing a
margin for variations in the LTC1149 series and external
component values yields:
R
SENSE
=
100mV
I
MAX
A graph for selecting R
SENSE
versus maximum output
current is given in Figure 2. The LTC1149 series works well
with values of R
SENSE
from 0.02 to 0.2.
The load current below which Burst Mode
operation
commences, I
BURST
, and the peak short-circuit current,
I
SC(PK)
, both track I
MAX
. Once R
SENSE
has been chosen,
I
BURST
and I
SC(PK)
can be predicted from the following
equations:
I
BURST
15mV
R
SENSE
I
SC(PK)
=
150mV
R
SENSE
+
PGATE
V
IN
V
CC
PDRIVE
V
CC
C
T
I
TH
SENSE
CAP
SHDN2
RGND
NGATE
PGND
SGND
SENSE
+
1
2
3
4
5
6
7
8
16
15
14
13
12
11
10
9
LTC1149
0.047µF
1µF
0.068µF
V
IN
0.1µF
+
V
8
3300pF390pF
1000pF
+
V
9
– V
8
25k
75k
220µF
0.05
+
V
10
V
OUT
+
V
15
50µH
IRF9Z34
220µF
100V
IRFZ34
MBR380
1149 TC
V
FB
/
SHDN1
1k
+
+
+
8
LTC1149
LTC1149-3.3/LTC1149-5
APPLICATIO S I FOR ATIO
WUU U
Figure 3. Timing Capacitor Selection
L and C
T
Selection for Operating Frequency
The LTC1149 series uses a constant off-time architecture
with t
OFF
determined by an external timing capacitor C
T
.
Each time the P-channel MOSFET switch turns on, the
voltage on C
T
is reset to approximately 3.3V. During the
off-time, C
T
is discharged by a current which is propor-
tional to V
OUT
. The voltage on C
T
is analogous to the
current in inductor L, which likewise decays at a rate
proportional to V
OUT
. Thus the inductor value must track
the timing capacitor value.
The value of C
T
is calculated from the desired continuous
mode operating frequency, f:
C
T
=
(7.8)(10
–5
)
f
)
)
1 –
V
OUT
V
IN
A graph for selecting C
T
versus frequency including the
effects of input voltage is given in Figure 3.
As the operating frequency is increased the gate charge
losses will be higher, reducing efficiency (see Efficiency
Considerations). The complete expression for operating
frequency is given by:
f =
1
t
OFF
)
)
1 –
V
OUT
V
IN
where:
t
OFF
= (1.3)(10
4
)(C
T
)
)
)
V
REG
V
OUT
V
REG
is the desired output voltage (i.e., 5V, 3.3V), while
V
OUT
is the actual output voltage. Thus V
REG
/V
OUT
= 1
when in regulation.
Note that as V
IN
decreases, the frequency decreases.
When the input to output voltage differential drops below
1.5V, the LTC1149 series reduces t
OFF
by increasing the
discharge current in C
T
. This prevents audible operation
prior to dropout.
Once the frequency has been set by C
T
, the inductor L must
be chosen to provide no more than 25mV/R
SENSE
of peak-
to-peak inductor ripple current. This results in a minimum
required inductor value of:
L
MIN
=( 5.1)(10
5
)(R
SENSE
)(C
T
)(V
REG
)
As the inductor value is increased from the minimum
value, the ESR requirements for the output capacitor are
eased at the expense of efficiency. If too small an inductor
is used, the inductor current will decrease past zero and
change polarity. A consequence of this is that the LTC1149
series may not enter Burst Mode
operation and efficiency
will be severely degraded at low currents.
FREQUENCY (kHz)
0
0
C
T
CAPACITANCE (pF)
200
400
600
1400
1000
50
100
1200
800
150
200
250
V
OUT
= 5V
V
IN
= 48V
V
IN
= 12V
V
IN
= 24V
1149 F03
The LTC1149 series automatically extends t
OFF
during a
short circuit to allow sufficient time for the inductor
current to decay between switch cycles. The resulting
ripple current causes the average short-circuit current
I
SC(AVG)
to be reduced to approximately I
MAX
.
Figure 2. R
SENSE
vs Maximum Output Current
MAXIMUM OUTPUT CURRENT (A)
0
R
SENSE
()
0.12
0.16
0.20
4
1149 F02
0.08
0.04
0
1
2
3
5
0.10
0.14
0.18
0.06
0.02
9
LTC1149
LTC1149-3.3/LTC1149-5
APPLICATIO S I FOR ATIO
WUU U
Inductor Core Selection
Once the minimum value for L is known, the type of
inductor must be selected. High efficiency converters
generally cannot afford the core loss found in low cost
powdered iron cores, forcing the use of more expensive
ferrite, molypermalloy, or Kool Mµ
®
cores. Actual core
loss is independent of core size for a fixed inductor value,
but it is very dependent on inductance selected. As induc-
tance increases, core losses go down. Unfortunately,
increased inductance requires more turns of wire and
therefore copper losses increase.
Ferrite designs have very low core loss, so design goals
can concentrate on copper loss and preventing saturation.
Ferrite core material saturates “hard,” which means that
inductance collapses abruptly when the peak design cur-
rent is exceeded. This results in an abrupt increase in
inductor ripple current and consequent output voltage
ripple which can cause Burst Mode
operation to be falsely
triggered in the LTC1149 series. Do not allow the core to
saturate!
Molypermalloy (from Magnetics, Inc.) is a very good, low
loss core material for toroids, but it is more expensive than
ferrite. A reasonable compromise from the same manu-
facturer is Kool Mµ. Toroids are very space efficient,
especially when you can use several layers of wire.
Because they generally lack a bobbin, mounting is more
difficult. However, new surface mount designs available
from Coiltronics do not increase the height significantly.
P-Channel MOSFET Selection
Two external power MOSFETs must be selected for use
with the LTC1149 series: a P-channel MOSFET for the
main switch, and an N-channel MOSFET for the synchro-
nous switch.
The minimum input voltage determines whether standard
threshold or logic-level threshold MOSFETs must be used.
For V
IN
> 8V, standard threshold MOSFETs (V
GS(TH)
< 4V)
may be used. If V
IN
is expected to drop below 8V, logic-
level threshold MOSFETs (V
GS(TH)
< 2.5V) are strongly
recommended. When logic-level MOSFETs are used, the
absolute maximum V
GS
rating for the MOSFETs must be
greater than the LTC1149 series internal regulator
voltage V
CC
.
Selection criteria for the P-channel MOSFET include the
on-resistance R
DS(ON)
, reverse transfer capacitance C
RSS
,
input voltage and maximum output current. When the
LTC1149 is operating in continuous mode, the duty cycle
for the P-channel MOSFET is given by:
P-Ch Duty Cycle =
V
OUT
V
IN
The P-channel MOSFET dissipation at maximum output
current is given by:
P-Ch P
D
=
V
OUT
V
IN
+ K(V
IN
)
2
(I
MAX
)(C
RSS
)(f)
(I
MAX
)
2
(1 +
P
) R
DS(ON)
where is the temperature dependency of R
DS(ON)
and K
is a constant related to the gate drive current. Note the two
distinct terms in the equation. The first gives the I
2
R
losses, which are highest at low input voltages, while the
second gives the transition losses, which are highest at
high input voltages. For V
IN
< 24V, the high current
efficiency generally improves with larger MOSFETs
(although gate charge losses begin eating into the gains.
See Efficiency Considerations). For V
IN
> 24V, the transi-
tion losses rapidly increase to the point that the use of a
higher R
DS(ON)
device with lower C
RSS
actually provides
higher efficiency. This is illustrated in the Design Example
section.
The term (1 + ) is generally given for a MOSFET in the
form of a normalized R
DS(ON)
vs temperature curve, but
= 0.007/°C can be used as an approximation for low
voltage MOSFETs. C
RSS
is usually specified in the MOSFET
electrical characteristics. The constant K is much harder to
pin down, but K = 5 can be used for the LTC1149 series to
estimate the relative contributions of the two terms in the
P-channel dissipation equation.
N-Channel MOSFET and D1 Selection
The same input voltage constraints apply to the N-channel
MOSFET as to the P-channel with regard to when logic-
level devices are required. However, the dissipation calcu-
lation is quite different. The duty cycle and dissipation for
Kool Mµ
is a registered trademark of Magnetics, Inc.

LTC1149CS#TRPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 5V High Eff Syn Stepdn Sw Reg
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