AN97-002
May 1997
1
Two-Cell, Step-Up Converter Design for
Portable Applications
James Liu
Introduction
In recent years, the markets for portable electrical
devices, such as the electronic dictionary, palmtop
computers, notebook PCs, PDAs and cellular
phones has grown rapidly. All of these devices use
batteries as the source of power. Due to their
limitations of small size and light weight and due to
increasingly stringent environmental requirements
in product development, the use of small numbers,
small size, long-lasting batteries has become a
trend.
The AIC1630/1631/1633 are very suitable for the
application of using 2~4 batteries. This article will
focus on the application of AIC1631-5 for 2
batteries in the following description.
A set of two alkaline, NiMH, or NiCd battery cells
accompanied by a switching converter with 3V,
3.3V, or 5V output voltage is frequently used as
the power supply source for portable electronic
products. Using two battery cells is usually a result
of compromise between size and battery
operating life. Besides the batteries’ own stored
energy, two other factors also influence batteries’
operating life: the product’s power consumption
and conversion efficiency of the converter. In
order to choose the appropriate switching
converter for an electronic product, therefore, 5
key factors need to be considered:
(1) The current capacity and regulation of the
output should meet the product’s demands.
(2) High conversion efficiency.
(3) Low power consumption.
(4) Squeeze out as much of the battery energy
as possible.
(5) Small size and light weight.
The first factor is absolutely necessary, and the
importance of the other four differs in priority
depending on the character of the product. For
products, which operate relatively high current
for extended time periods, conversion efficiency
is paramount. For products operate with low
current for most of the time, the current
consumption of the converter itself must also be
low. With regards to size and weight, an 8-pin IC,
which does not need a heatsink, with a small
inductor, and minimum number of external parts,
would be an ideal choice. In the following, we use
the AIC1631 DC/DC converter as an example for
several different special products using two
battery cells to demonstrate how the AIC1631
can be used to make an ideal power source.
(+5V)
+VOUT
+VIN
1N5819
CGND
LBO
LBI
VOUT
SGND
SW
VIN
ILIM/SD
+
100mF
C3
D1
47mH*
*Sumida RCH-108
+100mF
C1
+
1K
R1
33K
R2
10mF
C2
VIN
AIC1631-5
Fig. 1 A High-Efficiency 2-Cell to 5V Converter
AN97-002
2
Load Current (mA)
90
0 100 200 300 400 500 600
75
80
85
VIN=1.8V
VIN=2V
VIN=2.2V
VIN=2.5V
VIN=3V
VIN=3.3V
Efficiency (%)
Fig. 2 Conversion Efficiency for the 5V
Converter
Conversion Efficiency Considerations
Conversion efficiency is the main consideration for
those devices which consume above 2mA most of
the time. Fig. 1 shows a high efficiency converter
circuit suitable for producing 5V output from two
battery cells. The components shown in Fig. 1 are
easily obtained low cost common parts. If high-
quality parts (such as MMP core inductors) are
used, efficiencies of 90% and above can be
reached. However, if good output power quality is
desired, such as in Fig. 2 or better, at least two
points need to be observed:
(1) A good power plan and a correct layout for
the circuit board is a must. The AIC1631
evaluation boards are available for your
reference.
(2) One must have the correct inductor values.
The equivalent series resistance of the
inductor must be low and the core must not
be saturated under any operation condition.
The above example uses the Sumida RCH-
108 47mH inductor, whose coil resistance
(RDC) is 0.14W.
When converting 2 alkaline battery cells to 5V, an
inductor of 40-150mH is suggested. For NiCd
batteries, a 20-100mH inductor is suggested.
Inductors of less inductance can output a larger
current. However, too low inductance would result
in serious efficiency loss due to inductor core
saturation. The most reliable method, therefore, is
to test for the best conditions using a range of
suggested values. The lower coil resistance (RDC)
be chosen, the better efficiency obtained. For
products consuming about 20mA, the RDC should
be under 1W. For products with current
consumption at or above 50mA, the RDC should be
below 0.5W. The larger the consumption current,
the smaller the RDC required.
Low Power Consumption Products
The quiescent current of the AIC1631-5 in an no
load state is about 200mA. For special energy-
conscious products, some circuit configurations
are presented here to illustrate how the AIC1631
can be used:
(1) If this DC/DC converter is not required to
maintain output voltage, you may simply pull
pin 1 (shutdown pin) to ground by using a
control signal. The AIC1631 will stop
functioning and the power consumption drop
to less than 10mA. Normal operation can be
recovered by pulling pin 1 high. Generally
speaking, this is ideal for systems with
backup lithium batteries. Fig. 3 is an example
circuit. While using the lowest possible
amount of power, the circuit makes it possible
to retain data in memory even when changing
batteries.
AN97-002
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47mH
+
100mF
C2
+
100mF
C3
+10mF
C1
1K
R2
33K
R1
SDN*
VIN
1N5819
D2
(+5V) VOUT
AIC 1631-5
1N5819
D1
VOUT
LBI
LBO
CGND
SGND
SW
VIN
ILIM/SO
** +
* SDN=VIN or VOUT to Operate
SDN=GND to Shutdown
** Backup Lithium Battery
Fig. 3 Step-Up converter with Shutdown Control
(2) If the output voltage requires the AIC1631,
one could add a few external components to
make an oscillator to generate control signals
for the AIC1631 to perform intermittent
operations. This is called “Burst Mode
Operation”, and is shown in Fig. 4(a). If CTL
shown in Fig. 4(a) is connected to VIN or VOUT,
the circuit will function normally with the
characteristics similar to the circuit in Fig.1. If
CTL is connected to GND, the circuit will
enter Burst Mode with an output voltage of 4V,
and the circuit itself consumes very low
power, as shown in Fig. 4(b). To change the
output voltage in the burst mode, simply
change the divider ratio of R3 and R4 in Fig.
4(a). Note that the voltage of normal
operation will never be exceeded.
0.01mF
C1
2N3904
Q1
1M
1N4148
1N4148
1M
R2 R3
1M
R4
150K
1K
47mH
+100mF
C3
+
10mF
VIN
CTL*
VOUT
1N5819
AIC1631-5
VOUT
LBI
LBO
CGND
SGND
SW
VIN
ILIM/SO
R5
D1
D2
C2
D3
* CTL =GND in Burst Mode
CTL=VIN or VOUT in Normal Mode
(a)
Load Current (mA)
Total Supply Current (mA)
0 50 100 150 200 250 300
200
400
600
800
VIN=1.8V
VIN=2.5V
VIN=2V
VIN=3V
VIN=3.3V
(b)
Fig. 4. Low Supply Current, Burst Mode Step-Up
Converter
(a) Application Circuit
(b) Total supply Current vs. Load Current
(3) To get the most out of the batteries‘ energy,
the DC/DC converter must be able to work at
low battery voltage. The circuit shown in Fig.
5 still deliver 30mA at 5V with input voltage at
1.6V. The conversion efficiency, however, is
somewhat lower than circuit in Fig. 1.
These examples shown above use the
AIC1631-5 to produce a 5V output. The
AIC1631 and AIC1631-3 can be used similarly
to produce 3.3V and 3V, respectively.
AN97-002
4
47mH
+10mF
C3
++
1K
(+5V)
+VOUT
+VIN AIC1631-5
1N5819
D1
VOUT
LBI
LBO
CGND
SGND
SW
VIN
ILIM/SO
R1
33K
R2
100mF
C1
100mF
C2
Fig. 5 1 Cell to 5V Step-Up Converter
2~4 Cells to 5V Low Noise Power Supply
The AIC1631-5 can be used to convert 2-4
Alkaline cells to 5 volts. The low dropout linear
regulator is composed of the low battery detector
(LBI and LBO pins), resistors R1, R2, R3, R4, and
a PNP transistor 2SA1244, while the other
components perform the job of a step-up
switching regulator. The 1N4148 raises the output
voltage of the switch regulator by 0.4V, allowing
the linear low dropout regulator to filter out ripple
noise. This results in a 7% loss in conversion
efficiency, a necessary price to pay for a clean
power source. The lower the output voltage, the
higher the conversion efficiency loss due to this
0.4V voltage drop. For 3.3V (the AIC1631) and 3V
(the AIC1631-3) output voltages, it creates a
conversion efficiency loss around 10%.
2SA1244
Q1
1N4148
D2
1N5819 C4
47mF
C3
22mF
47mF
C1
10mF
C2
R1
62K
R220K
R4
1M
R3
1.2K
1K
R5
L1
40mH
100mH
L2
VOUT
(5V)
VIN
SGND CGND
SW LBO
VIN LBI
ILIM/SD VOUT
7
8
6
5
4
3
2
1
++
+
+
D1
AIC1631-5
Fig. 6 2~4 Cells to 5V Low Noise Power Supply
Components Selection
A few guidelines can be followed when using the
LBI and LBO pins of the AIC1631 (also the
AIC1633 and the AIC1630) to form a low dropout
linear regulator. One can see from Fig. 6, that
output voltage is:
V(R R )
R1. 22 VOUT
12
2
=
+
´
The usable range of values for R4 is very large.
Ordinarily, 1MW is a good choice, R3 must match
with the PNP transistor. Since the current gain of
the PNP transistor is usually only between 5 and
30 when VCE=0.4V, the output current capability
will be inadequate if the R3 value is too large. On
the other hand, since the LB loop can adjust
automatically, it will be acceptable if R3 value is a
little smaller. However, if we use the right value for
R3, in addition to its normal function, it can also
AN97-002
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perform current limiting function. Normally, when
output current is below 300mA and the PNP
transistor is selected according to the following
guidelines, the R3 value would be between 1KW
and 5KW.
The first rule in selecting a PNP transistor is that
the rated current should be high enough.
Secondly, current gain b of the PNP must be
maintained at greater than 10 (the greater the
value the better) when VCE=0.4V and IC is equal to
or larger than the required output current. The
transistor 2SA1244 in Fig. 6 is a good example.
Since under some circumstance, the use of a
capacitor with too large capacitance value or too
low ESR value (such as OSCON capacitors) can
easily shifts the dominant pole of the linear
regulator and causes an oscillation situation. An
electrolytic or a tantalum capacitor with
capacitance lower than 100mF is suggested for the
capacitor C3.
Due to the limited bandwidth of the linear regulator
and the ESR effect of C3, high frequency spikes
and noises may pass the linear regulator and
appear at the output terminal. L1 and C4 are
therefore added at the output node to form a p
filter to filter out high frequency noises and obtain
a truly clean power source.
PCB Layout Hints
With a correct PCB layout, the output voltage
noise of the circuit, shown in Fig. 1 should be
below 20mV (Peak to Peak). Under most
circumstances, the noise cannot even be seen.
However, sometimes one can see ringing of about
10MHz on the oscilloscope. This is referred to as
ground noise. Ground noise is conducted by the
PCB ground traces and closely related to the
layout of the ground plane. How do we distinguish
ground noise? Simply connect the ground end of
the oscilloscope probe to different spots of the
ground plane. If the noise‘s magnitude or shape
changes significantly, then it is ground noise. In
practical applications, we only need to apply a
0.1mF ceramic capacitor across the power input
terminals of the analog circuit, as shown in Fig. 7.
ANALOG
CIRCUIT
GND
VDD
VOUT
VIN
GND
+AIC1631
CIRCUIT 0.1mF
Fig. 7 Ground Noise Reduction by Using a
0.1mF Ceramic Capacitor