June 2006 Tiny Buck-Boost Converter for Low Current Applications

L DESIGN IDEAS
Tiny Buck-Boost Converter for
Low Current Applications
by Eddy Wells
Introduction
One common challenge for many battery powered portable applications is
creating a regulated output voltage
above or below the input source. Traditional buck-boost approaches, such
as a dual inductor SEPIC converter or
cascaded regulators, are unacceptable
in most portable devices because of
their large solution size and low efficiency. Smaller footprint, integrated
charge-pump solutions can switch
between buck and boost operation, but
charge-pumps achieve good efficiency
at only a few operating voltages, while
efficiency dips below 50% at others.
Another compact and simple approach
forgoes a portion of the battery capacity and uses a buck (step-down) only
solution, but the advantages are hard
to justify when much of the battery
capacity is not used, as with certain
Li-Ion chemistries and a 3.3V output,
or with two alkaline cells and a 3.0V
or 2.5V output.
two small ceramic capacitors, a miniature inductor, and the ThinSOT IC.
All versions of the part are available
in a thermally enhanced 3mm × 3mm
DFN packages. A photo of the LTC3531
demo-board is shown in Figure 1.
Generating a Clean 5V
from a Noisy USB Cable
Figure 1. Compact 3.3V buck-boost application
The LTC3531 is a single inductor
200mA buck-boost converter that
generates a regulated output voltage
from a wide input voltage between
1.8V and 5.5V while maintaining high
efficiency. It is an excellent fit for low
power applications where a tiny total
solution size is required. The LTC3531
is available with fixed outputs [3.0V
or 3.3V] or with an adjustable output
that can be set between 2.0V and 5.0V.
The fixed output versions require only
IL
200mA/DIV
BOOST
BUCK-BOOST
BOOST
VOUT
0.5V/DIV
VIN
0.5V/DIV
5.5V
5V
4.5V
20µs/DIV
Generating a clean 5V output from
a USB cable or wall adapter can be
a challenge when the combination of
source impedance and load transients
cause noise and voltage droops. USB
cable voltage can vary between 5.25V
and 4.35V, while the maximum allowed decoupling capacitance on the
input is 10µF. The trace labeled “VIN”
in Figure 2 shows what can occur with
a 4.7µF input capacitor and a 100mA
load step from a powered device. The
LTC3531 produces a clean 5V output
(VOUT) with less than 100mV of peakto-peak ripple using a 22µF VOUT
capacitor. VIN and VOUT are DC aligned
at 500mV per division in Figure 2,
showing significant improvement in
noise and voltage droop. Inductor
current is also shown with operation
in both boost (VIN < VOUT) and buckboost (VIN ≅ VOUT) modes.
A complete schematic of the USB
to 5V application is shown in Figure 3 along with efficiency and power
loss curves versus load current. The
Figure 2. Noisy USB cable input to clean 5V output
4.5
95
SW2
VIN
VOUT
LTC3531
4.7µF
R2
1M
22µF
FB
SHDN
ON OFF
GND
VOUT
5V
200mA
R1
324k
EFFICIENCY (%)
SW1
80
POWER LOSS
75
COKE
1
GRAPHITE/
Li-POLYMER
3.5
3
2.5
70
2
65
0.1
Figure 3. USB to 5V application
38
10
85
POWER LOSS (mW)
USB
4.35V TO
5.25V
4
EFFICIENCY
VOLTAGE (V)
90
10µH
100
1
10
100
LOAD CURRENT (mA)
0.1
1000
0
20
40
60
USED CAPACITY (%)
80
100
Figure 4. Typical 1C lithium-ion/polymer
capacity curves
Linear Technology Magazine • June 2006
DESIGN IDEAS L
Li-Ion
+
–
SW1
SW2
VIN
VOUT
LTC3531-3.3
2.2µF
VOUT
3.3V
150mA
10µF
SHDN
GND
350
95
300
90
EFFICIENCY (%)
VIN
2.7V TO
5V
100
BOOST
MODE
85
80
MAXIMUM IOUT (mA)
10µH
BUCK
MODE
4SW
MODE
75
70
3.3VOUT AT 100mA
60
1.5
2
2.5
3 3.5 4 4.5
INPUT VOLTAGE (V)
5
Maximizing Li-Ion
Capacity for 3.3V
When compared to a straight buck
converter, the LTC3531 allows lower
input voltage operation when providing a 3.3V output from a Li-Ion input
source. Typical capacity curves for
100
+
–
LTC3531-3
2.2µF
VOUT
3V
80mA
47µF
SHDN
GND
80
10
2.5VIN
3.2VIN
75
1.8VIN
70
65
ON OFF
60
0.1
1
POWER LOSS AT 3.2VIN
1
10
100
LOAD CURRENT (mA)
Figure 7. Two AA or two AAA to 3.0V application
0.1
1000
POWER LOSS (mW)
2 x AA
ALKALINE
+
–
SW2
VOUT
EFFICIENCY (%)
85
SW1
100
2
2.5
3
3.5
4
4.5
5
5.5
Figure 6. Output current capability
vs input voltage (VOUT = 3.3V)
coke and graphite anode Li-Ion batteries are shown in Figure 4. Coke types
have a lower cut-off voltage at 2.5V,
where graphite types have a flatter
discharge curve and a 3.0V cut-off.
Solid lithium polymer batteries have
discharge curves similar to graphite.
The equivalent series resistance
(ESR) of the Li-Ion battery causes additional voltage drops at the terminal at
higher load currents. To make matters
worse, the battery protector circuit
adds additional series resistance and
the effects of ESR lower system efficiency as the battery is discharged.
90
VIN
150
VIN (V)
10µH
VIN
1.8V TO
3.2V
200
0
1.5
5.5
Figure 5. Lithium Ion to 3.3V schematic and 100mA efficiency curve.
LTC3531 operates in Burst Mode operation, with just 20µA of quiescent
current, providing high efficiency over
several decades of load current. All four
switches have an RDS(ON) of about 0.5Ω
when operating at 5V, providing >90%
efficiency at higher load currents.
250
50
65
ON OFF
L = 10µH
VOUT = 3.3V
To guarantee a 3.3V output, a buck
only design may need to use a cut-off
voltage of 3.5V or 3.6V. This translates
to a capacity loss of approximately
45% for the coke cell and 20% for the
graphite—both significant reductions
in run time. Furthermore, while graphite or polymer cells are more popular
because of their flat discharge curve,
new chemistries with greater capacity
per volume are on the horizon with
expected discharge curves resembling
the coke anode.
The wide input voltage range of the
LTC3531 allows a regulated 3.3V to be
produced from all Li-Ion chemistries,
two or three alkaline cells, or a 5V
source such as USB. The LTC3531
automatically transitions between
buck, 4-switch (buck-boost), and boost
modes based on the voltage difference
between VIN and VOUT. Figure 5 shows
a 3.3V application circuit, along with
efficiency vs input voltage for a 100mA
load. Maximum load current capability
vs input voltage (VOUT = 3.3V) is shown
in Figure 6. As expected, efficiency and
load current capability are reduced
with input voltage.
3.0V Flash Memory
Application from Two
Alkaline Cells
IL
200mA/DIV
VOUT
50mV/DIV
ILOAD
100mA/DIV
VIN = 2.5V
20µs/DIV
VOUT = 3V
COUT = 47µF
LOAD STEP = 10mA TO 100mA
Figure 8. Transient response of the circuit in Figure 7
Linear Technology Magazine • June 2006
Inexpensive MP3 players and other
relatively low capacity, low cost portable devices often replace a hard
disk drive (HDD) with flash memory
and Li-Ion batteries with disposable
alkaline—a good fit for the LTC3531.
A complete schematic for a two cell
alkaline to 3V flash memory supply is
shown in Figure 7. Efficiency is better
continued on page 40
39
L DESIGN IDEAS
Ideal Diodes Combine Battery Stacks
(Minimize Heat and Voltage Loss)
by Mitchell Lee
Introduction
Modifications
Combining multiple battery stacks to
serve a common load is an easy task for
a diode. Each stack delivers whatever
current it can muster to the load, but
back-feeding from a fresh battery to
one mostly discharged is precluded by
the presence of the blocking diode. If
you’re concerned with heat dissipation
in the diode and voltage drop at end
of discharge, diodes may leave you
pining for a better solution.
Operation over a range of 10V to 36V
is practical, and lower voltage operation is feasible by converting to a logic
level MOSFET. Because the forward
regulation point is a function of the
battery voltage, the 10M–10kΩ divider
should be adjusted to keep the drop
across the 10kΩ resistor in the range
of 10mV to 50mV.
In Figure 1 the forward drop exceeds
26.4mV when the product of the load
current and MOSFET RDS(ON) thus
dictate. For the 55mΩ IRF540, this
point is reached at load currents of
500mA.
Given some finite RDS(ON) there is
a practical limit for the load current
in any MOSFET, where RDS(ON) • ILOAD
ceases to provide any advantage over
a diode. In the case of the IRF540 this
point arrives in the 5A-to-10A range.
For higher current applications, substitute a lower RDS(ON) MOSFET. L
Active Diode
V+
than 80% with fresh alkaline cells and
better than 70% with depleted batteries. Note that overall efficiency is
lower in this application (relative to the
Li-Ion application) because of the lower
drive voltage for the switches—switch
RDS(ON) increases with decreasing drive
voltage. The adjustable version of the
part can be used to power lower voltage
flash memories (i.e. 2.5V) with similar
performance results.
Peak current requirements for flash
memory are typically lower than a
HDD, since there is no disk spin-up,
10k
+
26.4mV
–
1M
1M
IRF540
LT1494
BAT54W
+
LTC3531, continued from page 39
10M
26.4V
16 ALKALINE CELLS
–
The circuit in Figure 1 implements
an active, ideal diode using a low resistance MOSFET and a micropower
op amp. The MOSFET functionally
replaces the diode. Placing it in the
negative lead of the battery stack permits use of an N-channel device in a
simple arrangement, driven on by an
op amp if there is a slight forward voltage and off if the voltage reverses.
The forward voltage drop is regulated at 26.4mV, giving freedom from
oscillations and preventing reverse
current flow. Static current drain for
the entire circuit is less than 4µA.
18V
100nF
–VOUT
Figure 1. Battery pack ideal diode
but load transients still occur when
memory is accessed. The LTC3531’s
response to a 10mA–100mA load step
is shown in Figure 8. Burst Mode®
operation provides a rapid transient
response since there is no compensation loop to slew. Peak-to-peak
voltage ripple plus load step is under
50mV with a 47µF output capacitor.
The output voltage ripple stays fairly
constant over input voltage. Half the
output capacitance (22µF) results in
approximately twice the load step plus
voltage ripple (100mV).
Summary
The LTC3531 provides a simple,
compact buck-boost solution for
lower current, portable applications.
A complete solution, 1mm in height,
can fit in a 35mm2 footprint. The
part maintains high efficiency over
a wide range of input voltages and
load currents, extending battery run
time, while providing the flexibility to
address many designs such as 2-cell
alkaline, USB, and present day or
emerging Li-Ion chemistries. L
For more information on parts featured in this issue,
go to http://www.linear.com
40
Linear Technology Magazine • June 2006