7
LTC1433/LTC1434
OPERATION
U
(Refer to Functional Diagram)
Having only the small MOSFET on with low load current
reduces switching and gate charge losses, hence boosting
efficiency. For the device to go into low current mode, two
conditions must be satisfied: the peak current of the
inductor should not exceed 260mA and the voltage at the
I
TH
pin should not exceed 0.6V. When either one of the
conditions is exceeded, the big MOSFET will be turned on
at the next clock cycle.
Dropout Operation
When the input supply voltage decreases toward the
output voltage, the rate of change of inductor current
during the on cycle decreases. This reduction means that
the P-channel MOSFETs will remain on for more than one
oscillator cycle since the I
COMP
is not tripped. Further
reduction in input supply voltage will eventually cause the
P-channel MOSFET to be turned on 100%, i.e., DC. The
output voltage will then be determined by the input voltage
minus the voltage drop across the MOSFETs. Typically
under dropout, both the power MOSFETs are on since the
voltage on the I
TH
pin is greater than 0.6V.
Frequency Synchronization
A phase-locked loop (PLL) is available on the LTC1434 to
allow the oscillator to be synchronized to an external
source connected to the PLLIN pin. The output of the
phase detector at the PLL LPF pin is also the control input
of the oscillator, which operates over a 0V to 2.4V range
corresponding to – 30% to +30% in the oscillator’s center
frequency. When locked, the PLL aligns the turn-on of the
MOSFETs to the rising edge of the synchronizing signal.
When the PLLIN is left open, PLL LPF goes low, forcing the
oscillator to minimum frequency.
Power-On Reset
The POR pin is an open-drain output which pulls low when
the regulator is out of regulation. When the output voltage
rises to within 5% of regulation, a timer is started which
releases POR after 2
16
(65536) oscillator cycles. In shut-
down the POR output is pulled low.
Short-Circuit Protection
When the output is shorted to ground, the frequency of the
oscillator will be reduced to about 1/4.5 of its designed
rate. This low frequency allows the inductor current to
discharge, thereby preventing runaway. The oscillator’s
frequency will gradually increase to its designed rate when
the output voltage increases above 0.65V.
APPLICATIONS INFORMATION
WUU
U
The basic LTC1434 application circuit is shown in
Figure 1. External component selection is driven by the
load requirement and begins with the selection of C
OSC
and L. Next, the Schottky diode D1 is selected followed by
C
IN
and C
OUT
.
C
OSC
Selection for Operating Frequency
The LTC1433/LTC1434 use a constant frequency archi-
tecture with the frequency determined by an external
oscillator capacitor C
OSC
. During the on-time, C
OSC
is
charged by a fixed current plus an additional current
which is proportional to the output voltage of the phase
detector (V
PLL LPF
on LTC1434). When the voltage on the
C
OSC
capacitor reaches 1.19V, it is reset to ground. The
process then repeats.
The value of C
OSC
is calculated from the desired operating
frequency. Assume the phase-locked loop has no external
oscillator input, i.e. V
PLL LPF
= 0V.
A graph for selecting C
OSC
vs Frequency is given in Figure
2. For the LTC1433, the expression above is also appli-
cable since its oscillator is internally set up to run at a
condition equal to V
PLL LPF
= 0V. Therefore when using the
graph for determining the capacitance value for the oscil-
lator frequency, the V
PLL LPF
= 0V curve should be used for
LTC1433.
8
LTC1433/LTC1434
LTC1433/LTC1434 are used at 100% duty cycle with low
input voltages.
Inductor Value Calculation
The operating frequency and inductor selection are inter-
related in that higher operating frequencies permit the use
of a smaller inductor for the same amount of inductor
ripple current. However, this is at the expense of efficiency
due to an increase in MOSFET gate charge losses.
The inductor value has a direct effect on ripple current. The
ripple current I
L
decreases with higher inductance or
frequency and increases with higher V
IN
or V
OUT
:
I
fL
V
V
V
L OUT
OUT
IN
=
()()
1
1–
Core losses are dependent on the peak-to-peak ripple
current and core material. Hence, by choosing a larger
inductance the peak-to-peak inductor ripple current will
decrease, therefore decreasing core loss. To further re-
duce losses, low core loss material such as molypermalloy
or Kool Mµ
®
can be chosen as the inductor core material.
An indirect way that the inductor affects efficiency is
through the usage of the big P-channel at low load
currents. Lower inductance values will result in high peak
inductor current. Because one of the conditions that
determines the turning on of the large P-channel is peak
current, this will result in the usage of the large P-channel
even though the load current is low. Hence, efficiency at
low load current will be affected. See Efficiency Consider-
ations.
Inductor Core Selection
Once the 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 inductance
increases, core losses go down. Unfortunately, increased
inductance requires more turns of wire and therefore
copper losses will increase.
APPLICATIONS INFORMATION
WUU
U
Figure 2. Selecting C
OSC
for Oscillator Frequency
Kool Mµ is a registered trademark of Magnetics, Inc.
CAPACITANCE ON C
OSC
PIN (pF)
0
FREQUENCY (kHz)
400
500
600
150
1433/34 F02
300
200
50 100 200
100
0
700
V
PLLLPF
= 1.19V
V
PLLLPF
= 2.5V
V
PLLLPF
= 0V
Another important point to note is that at a low supply
voltages, the R
DS(ON)
of the P-channel switch increases
(see Typical Performance Characteristics). Therefore, the
user should calculate the power dissipation when the
As the operating frequency is increased the gate charge
losses will be higher, reducing efficiency. The maximum
recommended switching frequency is 700kHz. When us-
ing Figure 2 for synchronizable applications, the value of
C
OSC
is selected corresponding to a frequency 30% below
your center frequency (see Phase-Locked Loop and Fre-
quency Synchronization).
Low Supply Operation
The LTC1433/LTC1434 can function down to 3V and the
maximum allowable output current is also reduced at low
input voltages. Figure 3 shows the amount of change as
the supply is reduced down to 2.5V. The minimum guar-
anteed input supply is 3V.
SUPPLY VOLTAGE (V)
4.0
MAXIMUM OUTPUT CURRENT (%)
70
80
1433/34 F03
60
50
3.5
3.0
2.5
100
90
NOT RECOMMENDED
Figure 3. Maximum Allowable Output Current vs Supply Voltage
9
LTC1433/LTC1434
Ferrite designs have very low core loss and are preferred
at high switching frequencies, so design goals can con-
centrate on copper loss and preventing saturation. Ferrite
core material saturates “hard,” which means that induc-
tance collapses abruptly when the peak design current is
exceeded. This results in an abrupt increase in inductor
ripple current and consequent output voltage ripple. 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. Be-
cause they generally lack a bobbin, mounting is more
difficult. However, designs for surface mount are available
which do not increase the height significantly.
Catch Diode Selection
The catch diode carries load current during the off-time.
The average diode current is therefore dependent on the
P-channel switch duty cycle. At high input voltages the
diode conducts most of the time. As V
IN
approaches V
OUT
the diode conducts only a small fraction of the time. The
most stressful condition for the diode is when the output
is short circuited. Under this condition the diode must
safely handle I
PEAK
at close to 100% duty cycle. A fast
switching diode must also be used to optimize efficiency.
Schottky diodes are a good choice for low forward drop
and fast switching times. Most LTC1433/LTC1434 circuits
will be well served by either a 1N5818, an MBRS130LT3 or
an MBRM5819 Schottky diode.
C
IN
and C
OUT
Selection
In continuous mode, the source current of the P-channel
MOSFET is a square wave of duty cycle V
OUT
/V
IN
. To
prevent large voltage transients, a low ESR input capacitor
sized for the maximum RMS current must be used. The
maximum RMS capacitor current is given by:
C required
IN
II
VVV
V
RMS MAX
OUT IN OUT
IN
()
[]
12/
This formula has a maximum at V
IN
= 2V
OUT
, where
I
RMS
= I
OUT
/2. This simple worst-case condition is com-
monly used for design because even significant deviations
do not offer much relief. Note that capacitor manufacturer’s
ripple current ratings are often based on 2000 hours of life.
This makes it advisable to further derate the capacitor, or
choose a capacitor rated at a higher temperature than
required. Several capacitors may also be paralleled to
meet size or height requirements in the design. Always
consult the manufacturer if there is any question.
The selection of C
OUT
is driven by the required effective
series resistance (ESR). Typically once the ESR require-
ment is satisfied the capacitance is adequate for filtering.
The output ripple (V
OUT
) is determined by:
∆∆V I ESR
fC
OUT L
OUT
≈+
1
4
where f = operating frequency, C
OUT
= output capacitance
and I
L
= ripple current in the inductor. The output ripple
is highest at maximum input voltage since I
L
increases
with input voltage. For the LTC1433/LTC1434, the general
rule for proper operation is:
C
OUT
required ESR < 0.25
Manufacturers such as Nichicon, United Chemicon and
Sanyo should be considered for high performance
through-hole capacitors. The OS-CON semiconductor
dielectric capacitor available from Sanyo has the lowest
ESR/size ratio of any aluminum electrolytic at a some-
what higher price. Once the ESR requirement for C
OUT
has been met, the RMS current rating generally far
exceeds the I
RIPPLE(P-P)
requirement.
In surface mount applications multiple capacitors may
have to be paralleled to meet the ESR or RMS current
handling requirements of the application. Aluminum elec-
trolytic and dry tantalum capacitors are both available in
surface mount configurations. In the case of tantalum, it is
critical that the capacitors are surge tested for use in
switching power supplies. An excellent choice is the AVX
TPS series of surface mount tantalums, available in case
heights ranging from 2mm to 4mm. Other capacitor types
include Sanyo OS-CON, Nichicon PL series and Panasonic
SP series. Consult the manufacturer for other specific
recommendations.
APPLICATIONS INFORMATION
WUU
U

LTC1433CGN#TRPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators 450mA, L N C Mode Buck DC/DC Conv
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
Payment:
T/T Paypal Visa MoneyGram Western Union