The ML4790 is a high efficiency, PFM (Pulse Frequency
Modulation), boost switching regulator connected in
series with an integrated LDO (Low Dropout Regulator)
that incorporates “Silent Switcher™” technology. This
technique incorporates a patented tracking scheme to
minimize the voltage drop across the LDO and increase
the total efficiency of the regulator beyond that which can
be obtained by using a discrete external LDO regulator.
The ML4790 is designed to convert single or multiple cell
battery inputs to regulated output voltages for integrated
circuits and is ideal for portable communications
equipment that cannot tolerate the output voltage ripple
FEATURES
■ Incorporates “Silent Switcher™” technology to deliver
very low output voltage ripple (typically 5mV)
■ Guaranteed full load start-up and operation at 1.0V
input and low operating quiescent current (<100µA)
for extended battery life
■Pulse Frequency Modulation and internal synchronous
rectification for high efficiency
■ Minimum external components
■ Low ON resistance internal switching MOSFETs
■ Adjustable output voltage (2.5V to 5.5V)
normally associated with switching regulators.
An integrated synchronous rectifier eliminates the need for
an external Schottky diode and provides a lower forward
voltage drop, resulting in higher conversion efficiency. (* Indicates Part is End Of Life as Of July 1, 2000)
BLOCK DIAGRAM
Patent Pending
*Optional
1
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ML4790
PIN CONNECTION
ML4790
8-Pin SOIC (S08N)
PIN DESCRIPTION
V
GND
SENSE
V
OUT
IN
1
2
3
4
TOP VIEW
8
7
6
5
PWR GND
SHDN
V
L
V
BOOST
PIN
NO.NAMEFUNCTION
1V
IN
Battery input voltage
2GNDAnalog signal ground
3SENSEProgramming pin for setting the
output voltage
4V
OUT
LDO linear regulator output
PIN
NO.NAMEFUNCTION
5V
BOOST
Boost regulator output for connection
of an output filter capacitor
6V
L
Boost inductor connection
7SHDNPulling this pin high shuts down the
regulator, isolating the load from the
input
8PWR GND Return for the NMOS boost transistor
2
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ML4790
ABSOLUTE MAXIMUM RATINGS
Storage Temperature Range .................... –65°C to +150°C
Lead Temperature (Soldering 10s).......................... +260°C
Absolute maximum ratings are those values beyond which
the device could be permanently damaged. Absolute
maximum ratings are stress ratings only and functional
device operation is not implied.
V
Voltage on Any Other Pin ...GND –0.3V to V
Peak Switch Current (I
Average Switch Current (I
ML4790CS-X ............................................ 0°C to +70°C
ML4790ES-X......................................... –20°C to +70°C
V
Range
IN
ML4790CS-X ................................................ 1.0V to 6V
ML4790ES-X................................................. 1.1V to 6V
V
Range .................................................. 2.5V to 5.5V
OUT
)
JA
ELECTRICAL CHARACTERISTICS
Unless otherwise specified, V
PARAMETERCONDITIONSMINTYP.MAXUNITS
Supply
VIN CurrentVIN = 6V6075µA
V
Quiescent CurrentV
OUT
VL Quiescent Current1µA
= Operating Voltage Range, TA = Operating Temperature Range. (Note 1)
IN
SHDN = high1525µA
BOOST
= V
+ 0.5V810µA
OUT
PFM Regulator
Pulse Width (TON)4.555.5µs
LDO
SENSE Comparator Threshold Voltage194200206mV
Load RegulationSee Figure 1
= 1.2V, I
V
IN
VIN = 2.4V, I
< 10mA4.855.05.15V
OUT
< 75mA4.855.05.15V
OUT
Dropout VoltageSee Figure 1
= 1.2V, I
V
IN
VIN = 2.4V, I
Output Ripple5mV
< 10mA300mV
OUT
< 75mA500mV
OUT
P-P
Shutdown
SHDN Threshold0.50.81.0V
SHDN Bias Current–100100nA
Note 1: Limits are guaranteed by 100% testing, sampling, or correlation with worst case test conditions.
22µH
(Sumida CD54)
ML4790
V
IN
100µF
1nF
931kΩ
39.2kΩ
V
IN
GND
SENSE
V
OUT
PWR GND
SHDN
V
BOOST
100µF
V
L
33µF
I
OUT
V
OUT
Figure 1. Application Test Circuit
3
Page 4
ML4790
FUNCTIONAL DESCRIPTION
The ML4790 combines Pulse Frequency Modulation
(PFM) and synchronous rectification to create a boost
converter that is followed by a low dropout linear
regulator (LDO). This combination creates a low output
ripple boost converter that is both highly efficient and
simple to use.
The PFM regulator charges a single inductor for a fixed
period of time and then completely discharges before
another cycle begins, simplifying the design by
eliminating the need for conventional current limiting
circuitry. Synchronous rectification is accomplished by
replacing an external Schottky diode with an on-chip
PMOS device, reducing switching losses and external
component count.
The integrated LDO reduces the output ripple voltage to
less than 5mV peak-to-peak. Integrating the LDO along
with the PFM regulator allows the circuit to be optimized
for very high efficiency using a patented feedback
technique. It also allows the LDO to provide the
maximum ripple rejection over the operating frequency
range of the regulator.
A block diagram of the ML4790 is shown in Figure 2. The
PFM stage is comprised of Q1, Q2, A1, A2, the one shot,
the flip-flop, and externals L1 and C2. The LDO stage is
comprised of Q3, A3, the offset voltage control, and
external components R1, R2 and C
actually controls the operation of the PFM regulator, the
operation of the LDO stage will be covered first.
. Since the LDO
OUT
LDO OPERATION
The LDO stage operates as a linear regulator. A3 is the
error amplifier, which compares the output voltage
through the divider R1 and R2 to the reference, and Q3 is
the pass device. When the output voltage is lower than
desired, the output of A3 increases the gate drive of Q3,
which reduces the voltage drop across it and brings the
output back into regulation. Similarly, if the output voltage
is higher than desired, A3 adjusts the gate drive of Q3 for
more drop and the output is brought back into regulation.
450
400
350
(mV)
300
OS
V
250
200
150
100
0
10 20 30 40 50 60 70 80 90 100
I
(mA)
OUT
Figure 3. LDO VOS versus output current.
Also included in the LDO stage is an offset voltage
control. This circuit monitors the output current and
adjusts the offset voltage according the general
characteristic shown in Figure 3. The offset control
ensures that the PFM stage provides just enough
“overhead” voltage for the LDO stage to operate properly.
L1
6
Q2
+
A2
–
R
S
5µs
ONE SHOT
Q1
–
A1
+–
V
C2
5
+
OS
= f (I
LOAD
)
Q3
A3
I
LOAD
+
–
4
3
V
REF
R1
R2
C
FB
C
OUT
Figure 2. PFM Regulator and LDO Block Diagram
4
Page 5
ML4790
Note, that at lower output voltages there is less voltage
required at the PFM stage, and therefore less gate drive
available for the pass device Q3. This results in Q3 being
more resistive and unable to deliver as much output
current as a ML4790 set for a higher output voltage. This
characteristic is shown in Figure 4.
200
180
160
140
120
(mA)
100
OUT
I
80
60
40
20
0
2.5V3.5V4.5V5.5V
Figure 4. ML4790 I
VIN = V
OUT
(V)
V
OUT
MAX
OUT
– 0.5V, L = 22µH
PFM REGULATOR OPERATION
When the output of the PFM stage, V
above the dropout voltage, V
+ VOS, the output of A1
OUT
stays low and the circuit remains idle. When V
(pin 5), is at or
BOOST
BOOST
falls
below the required dropout voltage, the output of A1 goes
high, signaling the regulator to deliver charge to the
capacitor C2. Since the output of A2 is normally high, the
output of the flip-flop becomes SET. This triggers the one
shot to turn Q1 on and begins charging L1 for 5µs. When
the one shot times out, Q1 turns off, allowing L1 to
flyback and momentarily charge C2 through the body
diode of Q2. But, as the source voltage of Q2 rises above
the drain, the current sensing amplifier A2 drives the gate
of Q2 low, causing Q2 to short out the body diode. The
inductor then discharges into C2 through Q2. The output
of A2 going low also serves to RESET the flip-flop in
preparation for the next charging cycle. When the
inductor current in Q2 falls to zero, the output of A2 goes
high, releasing Q2‘s gate, allowing the flip-flop to be SET
again. If the voltage at V
is still low, A1 will initiate
BOOST
another pulse. Typical inductor current and voltage
waveforms are shown in Figure 5.
SHUTDOWN
The SHDN pin should be held low for normal operation.
Raising the voltage on SHDN above the threshold level
will release the gate of Q3, which effectively becomes an
open circuit. This also prevents the one shot from
triggering, which keeps switching from occurring.
DESIGN CONSIDERATIONS
INDUCTOR
Selecting the proper inductor for a specific application
usually involves a trade-off between efficiency and
maximum output current. Choosing too high a value will
keep the regulator from delivering the required output
current under worst case conditions. Choosing too low a
value causes efficiency to suffer. It is necessary to know
the maximum required output current and the input
voltage range to select the proper inductor value. The
maximum inductor value can be estimated using the
following formula:
2
××
()()
IN MINON MIN
()
VVI
OUTOSOUT MAX
L
MAX
VT
=
2
×+×
where η is the efficiency, typically between 0.75 and
0.85, and VOS is the dropout voltage at I
from Figure 3. Note that this is the value of inductance
that just barely delivers the required output current under
worst case conditions. A lower value may be required to
cover inductor tolerance, the effect of lower peak inductor
currents caused by resistive losses, and minimum dead
time between pulses.
Another method of determining the appropriate inductor
value is to make an estimate based on the typical
performance curves given in Figures 6 and 7. Figure 6
shows maximum output current as a function of input
voltage for several inductor values. These are typical
performance curves and leave no margin for inductance
and ON-time variations. To accommodate worst case
conditions, it is necessary to derate these curves by at
least 10% in addition to inductor tolerance.
For example, a two cell to 5.5V application requires
40mA of output current while using an inductor with 15%
tolerance. The output current should be derated by 25%
to 50mA to cover the combined inductor and ON-time
tolerances. Assuming that 2V is the end of life voltage of a
two cell input, Figure 6 shows that with a 2V input, the
ML4790 delivers 52mA with a 22µH inductor.
η
()
OUT(MAX)
(1)
taken
INDUCTOR
CURRENT
Q(ONE SHOT)
Q1 ONQ1 ON
Q1 & Q2 OFF
Q2
ON
Figure 5. PFM Inductor Current
Waveforms and Timing.
Q2
ON
5
Page 6
ML4790
Figure 7 shows efficiency under the conditions used to
create Figure 6. It can be seen that efficiency is mostly
independent of input voltage and is closely related to
inductor value. This illustrates the need to keep the
inductor value as high as possible to attain peak system
efficiency. As the inductor value goes down to 10µH, the
efficiency drops to between 70% and 75%. With 47µH,
the efficiency reaches approximately 90% and there is
little room for improvement. At values greater than 47µH,
the operation of the synchronous rectifier becomes
unreliable at low input voltages because the inductor
current is so small that it is difficult for the control circuitry
to detect as shown for the 5.5V output.
V
200
180
160
140
120
100
MAX (mA)
80
OUT
I
60
40
20
0
1.02.0
OUT =
L = 10µH
5.5V
L = 22µH
L = 47µH
3.04.05.0
(V)
V
IN
After the appropriate inductor value is chosen, it is
necessary to find the minimum inductor current rating
required. Peak inductor current is determined from the
following formula:
I
L PEAK
()
TV
ON MAXIN MAX
=
×
() ()
L
MIN
(2)
It is important to note that for reliable operation, make
sure that I
does not exceed the 1A maximum switch
L(PEAK)
current rating. In the two cell application previously
described, a maximum input voltage of 3V would give a
peak current of 880mA. When comparing various
inductors, it is important to keep in mind that suppliers
use different criteria to determine their ratings. Many use a
conservative current level, where inductance has dropped
to 90% of its normal level. In any case, it is a good idea to
try inductors of various current ratings with the ML4790 to
determine which inductor is the best choice. Check
V
OUT =
180
160
140
120
100
MAX (mA)
80
OUT
I
60
40
20
0
1.01.52.02.53.03.54.0
4.5V
L = 10µH
L = 22µH
L = 47µH
VIN (V)
V
140
120
100
80
MAX (mA)
60
OUT
I
40
20
0
1.01.5
OUT =
3.5V
L = 10µH
L = 22µH
L = 47µH
2.02.53.0
(V)
V
IN
V
35
30
25
20
MAX (mA)
15
OUT
I
10
5
0
1.01.21.41.61.82.0
OUT =
L = 10µH
2.5V
L = 22µH
L = 47µH
VIN (V)
Figure 6. Output Current versus Input Voltage.
6
Page 7
ML4790
efficiency and maximum output current, and if a current
probe is available, look at the inductor current to see if it
looks like the waveform shown in Figure 5.
The DC resistance of the inductor should be kept to a
minimum to reduce losses. A good rule of thumb is to
allow 5 to 10mΩ of resistance for each µH of inductance.
Also, be aware that the DC resistance of an inductor
usually isn‘t specified tightly, so an inductor with a
maximum DC resistance spec of 150mΩ may actually
have 100mΩ of resistance.
Suitable inductors can be purchased from the following
suppliers:
The boost capacitor (C2) supplies current to the load
during the ON-time of Q1 and will limit the ripple the
LDO stage has to contend with. The ripple on C2 is
influenced by three capacitor parameters: capacitance,
ESL, and ESR. The contribution due to capacitance can be
determined by looking at the change in the capacitor
voltage required to store the energy delivered by the
inductor in a single charge-discharge cycle, as given by
the following formula:
22
TV
×
C
2
≥
LVVV
2
×××∆(–)
ONIN
BOOSTOUTIN
inFarads
()
(3)
For example, a 2.4V input, a 5V output, a 22µH inductor,
and an allowance of 100mV of ripple on the boost
capacitor results in a minimum C2 value of 15µF.
V
100
95
90
85
80
75
70
EFFICIENCY (%)
65
60
55
50
1.01.52.02.53.03.54.0
OUT =
L = 47µH
4.5V
L = 10µH
L = 22µH
VIN (V)
V
OUT =
100
95
L = 47µH
90
85
80
75
L = 10µH
70
EFFICIENCY (%)
65
60
55
50
1.01.5
3.5V
L = 22µH
2.02.53.0
(V)
V
IN
V
100
95
90
L = 47µH
85
80
L = 22µH
75
70
EFFICIENCY (%)
L = 10µH
65
60
55
50
1.01.21.41.61.82.0
OUT =
2.5V
VIN (V)
Figure 7. Typical Efficiency at maximum output current as a Function of VIN.
7
Page 8
ML4790
V
RR
R
OUT
=×
+
02
12
2
.
()
RR
V
OUT
12
02
1=×−
.
The boost capacitor‘s Equivalent Series Resistance (ESR)
and Equivalent Series Inductance (ESL), also contribute to
the ripple due to the inductor discharge current waveform.
Just after the NMOS transistor turns off, the output current
ramps quickly to match the peak inductor current. This
fast change in current through the boost capacitor‘s ESL
causes a high frequency (5ns) spike that can be over 1V in
magnitude. After the ESL spike settles, the boost voltage
still has a ripple component equal to the inductor
discharge current times the ESR. This component will have
a sawtooth waveshape and can be calculated using the
following formula:
V
∆
ESR
BOOST
≤Ω
I
()
L PEAK
in
()
(4)
For example, a 2.4V input, a 22µH inductor, and an
allowance of 100mV of ripple on the boost capacitor
results in a maximum ESR of 200mΩ. Therefore, a boost
capacitor with a capacitance of 22µF or 33µF, an ESR of
less than 200mΩ, and an ESL of less than 5nH is a good
choice. Tantalum capacitors which meet these
requirements can be obtained from the following
suppliers:
AVX(207) 282-5111
Sprague(207) 324-4140
OUTPUT CAPACITOR
The LDO stage output capacitor (C1) is required for
stability and to provide a high frequency filter. An output
capacitor with a capacitance of 100µF, an ESR of less than
100mΩ, and an ESL of less than 5nH is a good general
purpose choice.
SETTING THE OUTPUT VOLTAGE
The adjustable output can be set to any voltage between
2.5V and 5.5V by connecting a resistor divider to the
SENSE pin as shown in the block diagram. The resistor
values R1 and R2 can be calculated using the following
equation:
(5)
The value of R
should be 40kΩ or less to minimize bias
2
current errors. R1 is then found by rearranging the
equation:
(6)
It is important to note that the accuracy of these resistors
directly affects the accuracy of the output voltage. The
SENSE pin threshold variation is ±3%, and the tolerances
of R1 and R2 will add to this to determine the total output
variation.
Input noise may cause output ripple to become excessive
due to “pulse grouping,” where the charge-discharge
pulses are not evenly spaced in time. In such cases it may
be necessary to add a small 500pF to 1000pF ceramic
feedback capacitor (CFB) from the V
pin to the SENSE
OUT
pin.
INPUT CAPACITOR
Unless the input source is a very low impedance battery, it
will be necessary to decouple the input with a capacitor
with a value of between 47µF and 100µF. This filtering
prevents the input ripple from affecting the ML4790
control circuitry, and it also improves efficiency by
reducing I-squared R losses during the charge and
discharge cycles of the inductor. Again, a low ESR
capacitor (such as tantalum) is recommended.
8
Page 9
LAYOUT
Good PC board layout practices will ensure the proper
operation of the ML4790. Important layout considerations
include:
• Use adequate ground and power traces or planes
• Keep components as close as possible to the ML4790
• Use short trace lengths from the inductor to the VL pin
and from the output capacitor to the V
• Use a single point ground for the ML4790 ground pins,
and the input and output capacitors
A sample PC board layout is shown in Figure 8.
BOOST
pin.
ML4790
Figure 8. Sample PC Board Layout.
9
Page 10
ML4790
PHYSICAL DIMENSIONS inches (millimeters)
0.189 - 0.199
(4.80 - 5.06)
8
Package: S08
8-Pin SOIC
0.017 - 0.027
(0.43 - 0.69)
(4 PLACES)
0.055 - 0.061
(1.40 - 1.55)
PIN 1 ID
1
0.050 BSC
(1.27 BSC)
0.012 - 0.020
(0.30 - 0.51)
SEATING PLANE
0.148 - 0.158
(3.76 - 4.01)
0.059 - 0.069
(1.49 - 1.75)
0.228 - 0.244
(5.79 - 6.20)
0.004 - 0.010
(0.10 - 0.26)
0º - 8º
0.015 - 0.035
(0.38 - 0.89)
0.006 - 0.010
(0.15 - 0.26)
ORDERING INFORMATION
PART NUMBERTEMPERATURE RANGEPACKAGE
ML4790CS0°C to +70°C8-Pin SOIC (S08) (End Of Life)
ML4790ES–20°C to +70°C8-Pin SOIC (S08) (End Of Life)
Micro Linear reserves the right to make changes to any product herein to improve reliability, function or design.
Micro Linear does not assume any liability arising out of the application or use of any product described herein,
neither does it convey any license under its patent right nor the rights of others. The circuits contained in this
data sheet are offered as possible applications only. Micro Linear makes no warranties or representations as to
whether the illustrated circuits infringe any intellectual property rights of others, and will accept no responsibility
or liability for use of any application herein. The customer is urged to consult with appropriate legal counsel
before deciding on a particular application. DS4790-01
2092 Concourse Drive
San Jose, CA 95131
Tel: 408/433-5200
Fax: 408/432-0295
04/28/97 Printed in U.S.A.
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