LTC1707CS8#PBF Linear Technology, LTC1707CS8#PBF Datasheet - Page 8

• Manufacturer Part Number: LTC1707CS8#PBF
• Description: IC BUCK SYNC ADJ .6A 8SOIC
• Manufacturer: Linear Technology
• Type: Step-Down (Buck)r

Specifications of LTC1707CS8#PBF

• Internal Switch(s): Yes
• Synchronous Rectifier: Yes
• Number Of Outputs: 1
• Voltage - Output: 0.8 ~ 8.5 V
• Current - Output: 600mA
• Frequency - Switching: 35kHz ~ 350kHz
• Voltage - Input: 2.85 ~ 8.5 V
• Operating Temperature: 0°C ~ 70°C
• Mounting Type: Surface Mount
• Package / Case: 8-SOIC (3.9mm Width)
• Primary Input Voltage: 8.5V
• No. Of Outputs: 1
• Output Voltage: 8.5V
• Output Current: 560mA
• No. Of Pins: 8
• Operating Temperature Range: 0°C To +70°C
• Msl: MSL 1 - Unlimited
• Rohs Compliant: Yes
• Lead Free Status / RoHS Status: Lead free / RoHS Compliant
• Power - Output: -

APPLICATIO S I FOR ATIO
LTC1707
with the oscillator synchronized at its minimum frequency,
i.e., to a clock just above the oscillator free-running
frequency. The actual reduction in average current is less
than for peak current.
The basic LTC1707 application circuit is shown in Figure 1a.
External component selection is driven by the load re-
quirement and begins with the selection of L followed by
C
Inductor Value Calculation
The inductor selection will depend on the operating fre-
quency of the LTC1707. The internal preset frequency is
350kHz, but can be externally synchronized up to 550kHz.
The operating frequency and inductor selection are inter-
related in that higher operating frequencies allow the use
of smaller inductor and capacitor values. However, oper-
ating at a higher frequency generally results in lower
efficiency because of increased internal gate charge losses.
The inductor value has a direct effect on ripple current. The
ripple current I
frequency and increases with higher V
Accepting larger values of I
inductances, but results in higher output voltage ripple
and greater core losses. A reasonable starting point for
setting ripple current is I
The inductor value also has an effect on Burst Mode
operation. The transition to low current operation begins
when the inductor current peaks fall to approximately
200mA. Lower inductor values (higher I
to occur at lower load currents, which can cause a dip in
efficiency in the upper range of low current operation. In
Burst Mode operation, lower inductance values will cause
the burst frequency to increase.
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,
Kool M is a registered trademark of Magnetics, Inc.
8
IN
and C
I
L
OUT.
f L
1
V
OUT
L
decreases with higher inductance or
U
1
U
V
L
OUT
V
IN
= 0.4(I
L
allows the use of low
MAX
W
IN
).
L
or V
) will cause this
OUT
U
.
(1)
forcing the use of more expensive ferrite, molypermalloy,
or Kool M
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.
Ferrite designs have very low core losses 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!
Kool M (from Magnetics, Inc.) is a very good, low loss
core material for toroids with a “soft” saturation character-
istic. Molypermalloy is slightly more efficient at high
(>200kHz) switching frequencies but quite a bit more
expensive. Toroids are very space efficient, especially
when you can use several layers of wire, while inductors
wound on bobbins are generally easier to surface mount.
New designs for surface mount are available from
Coiltronics, Coilcraft and Sumida.
C
In continuous mode, the source current of the top MOSFET
is a square wave of duty cycle V
voltage transients, a low ESR input capacitor sized for the
maximum RMS current must be used. The maximum
RMS capacitor current is given by:
This formula has a maximum at V
I
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
RMS
IN
C
and C
IN
= I
required I
OUT
OUT
®
/2. This simple worst-case condition is com-
cores. Actual core loss is independent of core
Selection
RMS
I
MAX
V
OUT
OUT IN
/V
V
IN
IN
. To prevent large
V
= 2V
IN
V
OUT
OUT
, where
1 2