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LTC1143 View Datasheet(PDF) - Linear Technology

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LTC1143 Datasheet PDF : 20 Pages
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LTC1143/LTC1143L
LTC1143L-ADJ
APPLICATIONS INFORMATION
drawn from VIN, the resulting loss increases with
input voltage. For VIN = 10V the DC bias losses are
generally less than 1% for load currents over 30mA.
However at very low load currents the DC bias current
accounts for nearly all of the loss.
2) MOSFET gate charge current results from switching
the gate capacitance of the power MOSFET. Each time
a MOSFET gate is switched from low to high to low again,
a packet of charge dQ moves from VIN to ground. The
resulting dQ/dt is a current out of VIN that is typically
much larger than the DC supply current. In continuous
mode, IGATECHG = ƒ(QP). The typical gate charge for
a 0.05P-channel power MOSFET is 40nC. This
results in IGATECHG = 4mA in 100kHz continuous opera-
tion, for a 2% to 3% typical midcurrent loss with
VIN = 10V.
Note that the gate charge loss increases directly with
both input voltage and operating frequency. This is the
principal reason why the highest efficiency circuits
operate at moderate frequencies. Furthermore, it
argues against using a larger MOSFET than necessary
to control I2R losses, since overkill can cost efficiency
as well as money!
3) I2R losses are easily predicted from the DC resistances
of the MOSFET, inductor and current shunt. In continuous
mode the average output current flows through L and
RSENSE, but is “chopped” between the P-channel
MOSFET and Schottky diode. The MOSFET RDS(ON) multi-
plied by the P-channel duty cycle can be summed with
the resistances of L and RSENSE to obtain I2R losses.
For example, if the RDS(ON) = 0.1, RL = 0.15, and
RSENSE = 0.05, then the total resistance is 0.3. This
results in losses ranging from 3% to 10% as the output
current increases from 0.5A to 2A. I2R losses cause the
efficiency to roll off at high output currents.
4) The Schottky diode is a major source of power loss at
high currents and gets worse at high input voltages.
The diode loss is calculated by multiplying the forward
voltage drop times the Schottky diode duty cycle
multiplied by the load current. For example, assuming
a duty cycle of 50% with a Schottky diode forward
voltage drop of 0.4V, the loss increases from 0.5% to
8% as the load current increases from 0.5A to 2A. If
Schotky diode losses routinely exceed 5% consider
using the synchronously switched LTC1142 series.
Figure 5 shows how the efficiency losses in one section of
a typical LTC1143 series regulator end up being appor-
tioned. The gate charge loss is responsible for the majority
of the efficiency lost in the midcurrent region. If Burst
Mode operation was not employed at low currents, the
gate charge loss alone would cause efficiency to drop to
unacceptable levels. With Burst Mode operation, the DC
supply current represents the lone (and unavoidable) loss
component, which continues to become a higher percent-
age as output current is reduced. As expected, the I2R
losses and Schottky diode loss dominate at high load
currents.
Other losses including CIN and COUT ESR dissipative
losses, MOSFET switching losses and inductor core losses,
generally account for less than 2% total additional loss.
100
GATE CHARGE
95
12 LTC1143 IQ
90
I2R
SCHOTTKY
DIODE
85
80
0.01
0.03 0.1 0.3
1
3
OUTPUT CURRENT (A)
LTC1143 • F05
Figure 5. Efficiency Loss
Shutdown Considerations
Pins 2 and 10 on the LTC1143 and LTC1143L shut down
their respective sections when pulled high. They require
CMOS logic level signals with tr, tf < 1µs and must never
be floated. The LTC1143L-ADJ gives up the pin-controlled
shutdown function in order to gain feedback pins for
programming the output voltages.
13

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