V15N2 - MAY

LINEAR TECHNOLOGY
MAY 2005
IN THIS ISSUE…
COVER ARTICLE
Finally, High Voltage
Current Sensing Made Easy ........... 1
Brendan Whelan, Glen Brisebois,
Albert Lee and Jon Munson
Issue Highlights ............................ 2
Linear Technology in the News… ... 2
DESIGN FEATURES
Versatile Buck-Boost Converter
Offers High Efficiency in a
Wide Variety of Applications ......... 8
Dave Salerno
Low EMI, Output Tracking, High
Efficiency, and Too Many Other
Features to List in a 3mm x 4mm
Synchronous Buck Controller ..... 11
Lin Sheng
Tiny RS232 Transeivers Run
Directly from Alkaline, NiMH
or NiCd Batteries ....................... 14
Kevin Wrenner and Troy Seman
Low Voltage Hot Swap™ Controller
with Inrush Current Control ........ 17
Chew Lye Huat
DESIGN IDEAS
............................................... 20–36
(complete list on page 20)
New Device Cameos...................... 37
Design Tools ................................ 39
Sales Offices................................ 40
VOLUME XV NUMBER 2
Finally, High Voltage
Current Sensing Made Easy
by Brendan Whelan, Glen Brisebois,
Albert Lee and Jon Munson
High Voltage Ability,
Flexibility and Accuracy
The LT6100 and LTC6101 are high
voltage precision high-side current
sense amplifiers. Their simple architectures make them flexible and easy
to use, while careful design has made
them reliable and robust.
Key features include high supply
range, user-configurable gains, low
input current, high PSRR and low
offset voltage. These features make
the LT6100 and LTC6101 perfect for
precision industrial and automotive
sensing applications as well as current-overload protection circuits.
The LT6100 operates to 48V, is
the simpler of the two to use, requiring almost no external components,
draws little power, and is tolerant of
several abnormal conditions such as
split inputs, power off, and reverse
battery.
The LTC6101 is the higher speed of
the two, operates to 70V, and is more
flexible, having external resistors set
the gain. Both parts are available in
a variety of small packages.
How Current Sensing Works
Current sensing is commonly accomplished in one of two ways. One
method is magnetic, where a structure
is created using permeable materials
to couple an m-field to a coil or Halleffect sensor. While non-intrusive to
the measured circuit, a coil type pickup
is intrinsically unable to provide
RSENSE
ILOAD
+ VSENSE –
VSUPPLY
LOAD
VSENSE = ILOAD • RSENSE
Figure 1. Typical high-side
current-sense circuit
any DC information (though exotic
“flux-gate” techniques are possible),
and Hall sensors generally lack the
accuracy and sensitivity for most DC
measurements.
The alternative is the introduction of
a known “sense” resistance in the load
path, thereby creating a small voltage
drop that is directly proportional to
the load current. Generally, the preferred connection for a sense resistor
is in the supply side of the circuit,
so that common grounding practices
can be retained and load faults can
be detected. In the case of positive
supply potentials, this connection is
commonly referred to as a “high-side”
sense configuration, as shown schematically in Figure 1. This means that
the sense voltage is a small difference
on a large common-mode signal from
the perspective of the sense amplifier,
which poses unusual demands on the
implementation to preserve accuracy
and dynamic range.
continued on page 3
, LTC, LT, Burst Mode, OPTI-LOOP, Over-The-Top and PolyPhase are registered trademarks of Linear Technology Corporation. Adaptive Power, C-Load, DirectSense, FilterCAD, Hot Swap, LinearView, Micropower SwitcherCAD, Multimode
Dimming, No Latency ΔΣ, No Latency Delta-Sigma, No RSENSE, Operational Filter, PanelProtect, PowerPath, PowerSOT,
SmartStart, SoftSpan, Stage Shedding, SwitcherCAD, ThinSOT, UltraFast and VLDO are trademarks of Linear Technology
Corporation. Other product names may be trademarks of the companies that manufacture the products.
EDITOR’S PAGE
Issue Highlights
M
onitoring the current on the high
side of a high voltage load is a
traditionally complex problem.
Typical grow-your-own solutions use
operational or instrumentation amplifiers, but these are commonly limited
in operational voltage range and/or
require a number of additional components. Simpler, integrated solutions
often lack versatility and/or precision.
Neither makes for an ideal solution.
Enter the LT6100 and LTC6101,
two high voltage precision high-side
current sense amplifiers. They boast
simple architectures that make them
flexible and easy to use, and careful
design that makes them reliable and
robust.
See our cover article for more about
these breakthrough devices.
Featured Devices
Below is a summary of the other devices featured in this issue.
Compact Power Solutions
The LTC3442 is a 1.2A buck-boost
converter that is ideal for mini disk
drive applications, and certainly for
other buck-boost apps as well. The
LTC3442 extends battery life with 95%
efficiency and fits into tight spaces
with its 3mm × 4mm DFN package.
(Page 8)
The LTC3808 synchronous DC/
DC controller packs many features
required by the latest electronic devices into a low profile (0.8mm tall),
3mm × 4mm leadless DFN package,
or a leaded SSOP-16 package. The
LTC3808 can provide output voltage
as low as 0.6V and output current as
high as 7A from a wide, 2.75V to 9.8V,
input range, making it a good fit for
battery powered and distributed DC
power systems. (Page 11)
RS232 Transceivers
Six new devices comprise a family of
small-footprint RS232 transceivers
that operate at up to 1Mbps over a
supply range of 1.8V to 5.5V. The
wide supply range permits operation
directly from two alkaline, NiCd, or
2
Linear Technology in the News…
Linear Completes Solid Quarter
On April 19, Linear Technology announced revenue for its third fiscal
quarter of $290,734,000, an increase of 39% over the third quarter of
the previous year. Included in the current quarter’s revenue is royalty
revenue of $40,000,000, which represents past royalties receivable under terms of a settlement and license agreement with another company.
Linear Technology expects to earn further royalties, dependent on sales of
licensed products, quarterly from July 2005 through June 2013. Linear
also reported net income for the quarter of $121,633,000 or $0.39 diluted
earnings per share, an increase of 42% over the third quarter last year.
According to Lothar Maier, CEO, “Linear Technology completed a solid
quarter, further enhanced by the settlement and license agreement. The
Company continues to be cash flow positive and profitable, as evidenced
by the 42% return on sales. The license agreement confirms the strength
of our intellectual property. We continue to lead the market with high
performance analog technology and innovative products.”
Products in the News
Linear ADCs Make Waves in Germany… The April issue of the German publication, Elektronik Journal features a cover article on Linear
Technology’s LTC2220 high speed ADC family. The issue included an
in-depth article on the product family, which delivers industry-leading
performance.
Product of the Week… The April 18 issue of EE Times featured Linear
Technology’s LT5527 RF downconverting active mixer as Product of the
Week. The publication highlighted the product’s ability to streamline 3G
basestation design.
Review of the Week… In its April 11 issue, EE Times featured Linear
Technology’s LTC3780 high performance buck-boost switching regulator
controller in its product Review of the Week. EE Times states in the article,
“The major breakthrough is a device that is the only true buck-boost
controller today. That is, it’s one that generates a glitch-free output as
it switches seamlessly from the buck to boost mode and vise versa. The
chip also maintains extremely high system efficiency over a wide inputvoltage range.”
NiMH battery cells, while a separate
VL supply pin eliminates interfacing
problems in mixed-supply systems.
(Page 14)
an adjustable soft-start, important for
the large load capacitors typical in low
voltage applications. (Page 17)
Low Voltage Hot Swap Controller
The LTC4216 is a low voltage Hot
Swap controller that allows a board
to be safely inserted and removed
from a live backplane. The LTC4216
is designed to meet the latest low voltage board supply requirements with
its unique feature of controlling load
voltages from 0V to 6V. It also features
The Design Ideas start on page 29,
including a temperature-to-frequency
converter that runs on two AA batteries. an LDO linear regulator that
betters switchers in efficiency, and
a compact DDR memory solution.
Three New Device Cameos appear on
page 37.
Design Ideas and Cameos
Linear Technology Magazine • May 2005
DESIGN FEATURES
LT6100 and LT6101, continued from page 1
LOAD
Traditional grow-your -own
solutions use operational or instrumentation amplifiers, but these are
commonly limited in the voltage range
of operation and/or require a number
of additional components to perform
the voltage translation function to
create a ground-referenced readout
signal. Far better and simpler solutions
are attainable by using the LT6100 and
LTC6101, which solve most high side
current sensing requirements.
For an index of these and other current sense solutions, see Table 1. For
specific applications where the current
sensing is performed within dedicated
chips or chip sets, see Table 2.
Watch Out for Sources of
Current Sensing Error
As with any sensor design, there are
several potential sources of error to
consider. The accuracy of the circuit
depends largely on how well the value
of the sense resistor is known. The
sense resistor itself has defined tolerances and temperature dependencies
that introduce errors. Stray resistance
in the measurement path or large
dI/dt loops can also add errors. It is
important to properly implement Kelvin connections to the sense resistor
to minimize these effects.1
After sense resistance, the most
significant source of error is the voltage
offset of the sense amplifier, since it
generates a level-independent uncertainty in the measurement. This is
particularly important for preserving
accuracy at current levels that are
substantially below the maximum
design value. In some applications it
is desirable to calibrate out the static
component of this term (in software,
for example), but this may not always
be practical.
An additional error source to
consider is the tolerance of any resistors that may be required for setting
scale factors. This can contribute to
full-scale uncertainty along with the
sense resistor and Kelvin connection
1 This topic is covered in depth in “Using Current
Sensing Resistors with Hot Swap Controllers and
Current Mode Voltage Regulators” in Linear Technology Magazine, September, 2003, pp. 34–35.
Linear Technology Magazine • May 2005
RSENSE
100m
1
VIN
(VCC + 1.4V) TO 48V
8
VS–
RG1
5k
V S+
RG2
5k
+
–
R
25k
A1
VCC
2.7V TO 36V
–
2
VO1
Q1 RE
10k
+
RO
50k
VEE
FIL
A2
3
6
5
R/3
R
4
VOUT
A2
A4
7
Figure 2. LT6100 simplified schematic
tolerances. For the LT6100, scaling
resistors are all provided on-chip, so
the tolerances are well defined and
accounted for in the data sheet specifications. In the case of the LTC6101,
the scaling accuracy is set strictly by
the user’s choice of resistors, thereby
allowing optimization for particular
requirements.
LT6100 Theory of Operation
Figure 2 shows a simplified schematic
of the LT6100 sensing across a 100mΩ
sense resistor. The differential voltage
across the sense resistor is imposed
upon internal resistor RG2 by the
action of the op amp A1 through
Q1’s collector. The resulting current
through RG2 is thus I = VSENSE/RG2,
and this current flows through Q1 and
RO. The voltage which appears across
RO is RO • VSENSE/RG2. But RO is ten
times the value of RG2, so the voltage is
ILOAD
–
VSENSE
RSENSE
simply 10 • VSENSE. This gives rise to the
LT6100’s inherent gain of 10 up to this
point. The next stage involving op amp
A2 gives the designer the flexibility of
selecting further gain by grounding or
floating pins A2 and A4 or connecting
them to the output. Gains of 1, 1.25,
2, 2.5, 4, and 5 can be set here, for
overall gains of 10, 12.5, 20, 25, 40,
and 50. Series resistor RE is provided
between the two stages to allow simple
low pass filtering by adding a capacitor
at the FIL pin.
LTC6101 Theory of Operation
Figure 3 shows a simplified schematic
of the LTC6101 in a basic currentsense circuit. As before, a sense
resistor, RSENSE, is added in series
with the system supply at the positive
(high side) of the supply. The internal
amplifier of the LTC6101 acts as a
voltage follower, driving its inverting
+
VBATTERY
RIN
5
V+
10V
L
O
A
D
3
4
IN –
5k
–
IN +
5k
+
10V
LTC6101
V
–
2
OUT
IOUT
1
VOUT = VSENSE x
ROUT
RIN
ROUT
Figure 3. LTC6101 simplified schematic
3
DESIGN FEATURES
input (IN–) to the same voltage as its
non-inverting input (IN+). This sets a
voltage across RIN that is equal to the
voltage across RSENSE:
VR(IN) = VSENSE
VOUT
=
VSENSE
ROUT
RIN
Substitute:
The current in RIN is therefore:
IIN
and the gain is:
VSENSE = RSENSE • ISENSE
V
= SENSE
RIN
The amplifier inputs are high impedance, so this current does not flow into
the amplifier. It is instead conducted
through an internal MOSFET to the
OUT pin, where it flows through ROUT to
ground. The output voltage is then:
to yield the desired ratio of output
voltage to sense current:
VOUT
I SENSE
=
ROUT •RSENSE
RIN
As with most current-sense solutions, the input and output voltages,
VOUT = IIN • ROUT,
as well as output current, are dictated
by the application. In order to allow
compatibility with most circuits, the
LTC6101 supports input voltages
between 0V and 500mV. This makes
it suitable for most applications that
use a small series sense resistor (or
shunt). The LTC6101’s output may be
required to drive a comparator, ADC, or
other circuitry. The output voltage can
swing from 0V, since it is open-drain,
to 8V. The output current may be set
as high as 1mA, allowing useful speed
and drive capability. The external gain
resistors, RIN and ROUT, allow a wide
range of gains to work in concert with
these circuit constraints.
Table 1. Use this index of publications to find detailed applications information for current sensing solutions.
Publication
Hi Side/Low Side
Uni/Bi
Directional
VOS (CMRR)
Input Voltage/Feature
LT6100 Data Sheet
Hi Side
Uni
300
48V
LT6101 Data Sheet
Hi Side
Uni
300
60V
LT1787 Data Sheet
Hi Side
Bi
75µV
60V, 70µA
LT1990 Data Sheet, pp. 1, 16
Both
Bi
(80dB)
±250V
LT1991 Data Sheet, pp. 1, 19–22
Both
Bi
(80dB)
±60V
LT1995 Data Sheet, p. 20
Both
Bi
LTC2054 Data Sheet, p. 12
Hi Side
Bi
3µV
60V
LTC2054 Data Sheet, p. 1
Low Side
Uni
3µV
–48V
LT1494 Data Sheet, p. 1, 16
Hi Side
Uni, Bi
~1mV
36V
LTC2053 Data Sheet, p. 13
Hi Side (Both possible)
Uni
10µV
5V
LTC6800 Data Sheet, p. 1
Hi Side (Both possible)
Uni
100µV
5V
LTC6943 Data Sheet p. 1
Both
Uni
(120dB)
18V
LT1620 Data Sheet
Both
Uni
5mV
36V, power
LT1366 Data Sheet, p.1
Hi Side
Uni
200µV
36V
LT1797 Data Sheet, p. 1
Low Side
Uni
1mV
–48V, fast
Hi Speed
InfoCard 27
Various circuits
LT1637 Data Sheet, p. 13
Hi Side
Uni
~1mV
44V, Over-The-Top
LT1490A Data Sheet, p. 1
Hi Side
Bi
~1mV
12V, Over-The-Top
Design Note 341
Low Side
Uni
~1µV
–48V, Direct ADC
Linear Technology Magazine
Aug. 2004, p. 33
Low Side
Bi
2.5µV
Direct ADC
Design Note 297
Hi Side
Uni
2.5µV
Direct ADC
LTC1966 Data Sheet, pp. 29, 32
Both (AC)
Application Note 92
Hi Side
4
RMS Current
Uni
various
Avalanche PDs
Linear Technology Magazine • May 2005
DESIGN FEATURES
Features
The LTC6101:
Delivers Accuracy and Speed
in High Voltage Applications
The LTC6101 boasts a fully specified
operating supply range of 4V to 60V,
with a maximum supply voltage of
70V. Applications that require high
operating voltages, such as motor control and telecom supply monitoring,
or temporary high-voltage survival,
such as with automotive load dump
conditions, benefit from this wide supply range. The accuracy is preserved
across this supply range by a high
typical PSRR of 140dB.
The fast response time of the
LTC6101 makes it suitable for
overcurrent-protection circuits. The
typical response time is less than
1µs for the output to rise 2.5V on a
5V output transition. The LTC6101
can detect a load fault and signal
a comparator or microprocessor in
time to open a switch in series with
+
RIN
IN+
IN–
+
L
O
A
D
V
–
–
V
LTC6101
+
OUT
VOUT
ROUT
RIN+ = RIN– – RSENSE
Figure 4. Second input resistor minimizes
error due to input bias current
Both the LT6100 and LTC6101 are very
precise. They boast 300µV maximum
input offset (500µV and 535µV, respectively, over temperature). Neither
part draws supply current from the
input sense pins. The LT6100 draws
5µA from its Over-The-Top® inputs,
while the LTC6101 provides a separate
supply pin (V+) to be connected to the
sensed supply directly and draws only
100nA bias current at its inputs. This
makes the LTC6101 ideal for very
low current monitoring. In addition,
the LTC6101 sense input currents
are well matched so a second input
resistor, RIN+ (Figure 4), may be added
to cancel the effect of input bias. In
this way the LTC6101 effective input
bias error can be reduced to less than
15nA. The LT6100 provides these
matched resistors internally, reducing
its effective input bias current error
to below 1µA.
The LT6100:
Robust and Easy to Use
The LT6100 tolerates a reverse battery on its inputs up to –50V, while
guaranteeing less than 100µA of
resultant fault current. In addition, it
can also be used to sense across fuses
and MOSFETs as shown in Figure 5.
The LT6100 has no problem when
the fuse or MOSFET opens because it
has high voltage pnp’s and a unique
input topology that features full high
impedance differential input swing
Linear Technology Magazine • May 2005
SENSE–
V–
OPEN MOSFET
OR FUSE OK
ISENSE
TO LOAD
FROM SOURCE
VS–
VCC
VEE
OUT
ISENSE
RSENSE
TO LOAD
BATTERY
6.4V TO 48V
VS –
VCC
5V
0V
V S+
VCC
POWER DOWN OK
INPUTS REMAIN
HIGH IMPEDANCE
VEE
LT6100
A2 A4
VOUT
Figure 6. Remove power from the LT6100
with no need to disconnect the battery.
The LT6100 inputs remain high Z.
the load before supply, load or switch
damage occurs.
The architecture of the LTC6101
is the key to its flexibility. The gain
is completely controlled by external
resistors (RIN and ROUT, Figure 3). This
is convenient because most applications specify a small maximum shunt
voltage (to minimize power loss), which
must be matched to either a specific
comparator threshold or a desired ADC
resolution. This requires that gain be
SENSE–
V+
VOUT
LT6100
A2 A4
Figure 5. Sense across a MOSFET or
fuse without worry. LT6100 inputs
can split while remaining high Z.
SENSE+
+ –
VS+
+ –
Input Precision:
A Quick Comparison
capability to ±48V. This allows direct
sensing of fuse or MOSFET voltage
drops, without concern for the fuse or
MOSFET open circuit condition.
Another unique benefit of the
LT6100 is that you can leave it connected to a battery even when it is
unpowered. When the LT6100 loses
power, or is intentionally powered
down, both sense inputs remain high
impedance (see Figure 6). This is
due to the implementation of Linear
Technology’s Over-The-Top input topology at the front end. In fact, when
powered down, the LT6100 inputs
actually draw less current than when
powered up. Powered up or down, it
represents a benign load.
RIN–
+ –
VSUPPLY
V–
SENSE+
+ –
V+
OUT
a.
b.
Figure 7. The LT6101 achieves unparalled versatility in high side current sensing applications
by allowing the user to select the gain via external RIN and ROUT resistors. In most architectures,
some or all of these resistors are internal to the device, as shown here. Fixed gain devices, such
as in (a), limit flexibility. Those with fixed input resistors, as in (b), limit gain and speed.
5
DESIGN FEATURES
VSUPPLY
RSENSE
L
O
A
D
RIN
IN+
IN–
+ –
V–
V+
SERIES FILTER
OUT
LTC6101
LONG WIRE
ROUT
ADC
PARALLEL
FILTER
Figure 8. Open drain output enhances remote sensing accuracy.
VSUPPLY
RSENSE
L
O
A
D
RIN
IN
+
V–
–
+ –
IN
V+
V+
V–
LTC6101
OUT
ADC
ROUT
+
–
V–
Figure 9. Output reference level shifted above V–
carefully set to maintain performance.
In solutions where the gain resistors
are not user-selectable (Figure 7a),
the gain will be fixed, and may not be
set to an appropriate value. Another
approach is to include internal input
resistors (Figure 7b), which allows
user-configured gain, but may force
the use of a very large output resistor in order to get high gain (10-100
or more). A large output resistor will
cause the output to be slower and
Table 2. Linear Technology offers ICs for application-specific current-sensing solutions.
Use this table to find publications that cover specific applications.
6
Publication
Application
LTC4060 Data Sheet
NiMH/NiCd charger
Linear Technology Magazine Mar. 2003, p. 24
Battery chargers
Linear Technology Magazine May 2004, p. 24
Battery gas gauge
Application Note 89
5V, TEC Controller
Application Note 66, Application Note 84
Switch Mode Power
LT Chronicle Jan. 2003, p. 7
Automotive Temp
Design Note 1009
Photo Flash
Design Note 312
VRM9.x
Design Note 347
Bricks
LTC4259, LTC4267 Data Sheet
Power over Ethernet
Design Solution 43
Altera FPGAs
more susceptible to system noise,
and may be too high an impedance
to drive a desired ADC. The LTC6101
avoids these problems by allowing the
application designer to choose both
RIN and ROUT. RIN can be quite small,
its value limited only by the gain error
due to stray board resistance and the
1mA maximum output current specification. Therefore high gain and high
speed can be achieved even with small
VSENSE and ROUT requirements. Gain
accuracy is determined only by the
accuracy of the external resistors.
In addition, the open-drain output
architecture provides an advantage
for remote-sensing applications. If the
LTC6101 output must drive a circuit
that is located remotely, such as an
ADC, then the output resistor can
be placed near the ADC. Since the
open-drain output is a high-impedance current source, the resistive drop
in the output wire will not affect the
result at the converter. System noise
that is coupled onto the long wire can
be easily reduced with a series filter
placed before ROUT, or with a simple
capacitor in parallel with ROUT, with
no loss of DC accuracy (Figure 8). The
output may also be level shifted above
V– by terminating ROUT at a voltage
that is held higher than V– (figure 9),
provided that the maximum difference
between VOUT and V– does not exceed
the maximum specified output of the
LTC6101.
Applications
Micro-Hotplate Current Monitor
Materials science research examines
the properties and interactions of materials at various temperatures. Some
of the more interesting properties can
be excited with localized nano-technology heaters and detected using the
presence of interactive thin films.
While the exact methods of detection are highly complex and relatively
proprietary, the method of creating
localized heat is as old as the light bulb.
Figure 10 shows the schematic of the
heater elements of a Micro-hotplate
from Boston Microsystems (www.bostonmicrosystems.com). The physical
dimensions of the elements are tens
Linear Technology Magazine • May 2005
DESIGN FEATURES
White LED Current Controller
Figure 11 shows the LT6100 used in
conjunction with the LT3436 switch
mode power converter to efficiently
drive a white LED with a constant
current. By closing the switch on pin
A2 of the LT6100, its gain is adjusted
between 40 (open) and 50 (closed).
The FB pin of the LT3436 is a control pin referenced to a 1.2V set point.
When the FB pin is above 1.2V, the
LT3436 stops operation; when below
1.2V, the LT3436 continues operation.
The output voltage (>1.2V) is usually
regulated by applying a resistive divider from the output voltage back to
the FB pin to close the feedback loop.
To achieve a constant output current,
rather than a constant output voltage,
the feedback loop must convert the
load current to a voltage. Enter the
LT6100.
It senses the LED current by measuring the voltage across a 30mΩ
resistor, applies a gain, and feeds the
resulting voltage back to the FB pin.
Linear Technology Magazine • May 2005
VDR+
10
1%
VS–
IHOTPLATE
VS+
+ –
of microns. They are micromachined
out of SiC and heated with simple DC
electrical power, being able to reach
1000°C without damage.
The power introduced to the elements, and thereby their temperature,
is ascertained from the voltage-current
product with the LT6100 measuring
the current and the LT1991 measuring the voltage. The LT6100 senses
the current by measuring the voltage across the 10Ω resistor, applies
a gain of 50, and provides a ground
referenced output. The I to V gain is
therefore 500mV/mA, which makes
sense given the 10mA full scale heater
current and the 5V output swing of the
LT6100. The LT1991’s task is the opposite, applying precision attenuation
instead of gain. The full scale voltage
of the heater is a total of 40V (±20),
beyond which the life of the heater may
be reduced in some atmospheres. The
LT1991 is set up for an attenuation
factor of 10, so that the 40V full scale
differential drive becomes 4V ground
referenced at the LT1991 output. In
both cases, the voltages are easily read
by 0V–5V PC I/O cards and the system
readily software controlled.
5V
VCC
CURRENT
MONITOR
VOUT = 500mV/mA
LT6100
VEE A2 A4
MICRO-HOTPLATE
BOSTON
MICROSYSTEMS
MHP100S-005
5V
5V
M9
M3
M1
LT1991
P1
P3
P9
VOLTAGE
MONITOR
V + – VDR–
VOUT = DR
10
VDR–
www.bostonmicrosystems.com
Figure 10. LT6100 and LT1991 monitor the current and voltage
through a wide range of drive levels applied to a Microhotplate.
The 1.2V set point at the LT3436 can
be referred back across the sense
resistor by dividing by the LT6100
gains of 40 and 50. This gives 30mV
and 24mV respectively. Dividing by the
continued on page 28
D2
LED
L1
3µH
VIN
3.3V TO 4.2V
SINGLE Li-Ion
VIN
D1
B130
0.030
SHDN
FB
V S–
VCC
VOUT
VEE
MMBT2222
0.1µF
8.2k
LT6100
+ –
22µF
16V
CER
1210
124k
VC
GND
VS+
VOUT
VSW
LT3436
LED
ON
4.7µF
6.3V
CER
LED
CURRENT
WARNING! VERY BRIGHT
DO NOT OBSERVE DIRECTLY
A4
A2
OPEN: 1A
CLOSED: 800mA
4.99k
D1: DIODES INC.
D2: LUMILEDS LXML-PW09 WHITE EMITTER
L1: SUMIDA CDRH6D28-3R0
Figure 11. 1Amp/800mA white LED current controller
14V
RIN–
100Ω
VLOGIC
47k
FAULT OUTPUT
OFF ON
LT1910
FAULT
V+
IN
SENSE
TIMER
S4B85N06-05
GATE
GND
1µF
RIN+
100Ω IN+
RSENSE
+
V
10µF
63V
VOUT = 49.9 • ILOAD • RSENSE
FOR RSENSE = 5mΩ:
VOUT = 2.495V AT ILOAD =10A (FULL SCALE)
IN–
+
–
V+
–
LOAD
ILOAD
LTC6101
OUT
VOUT
4.99k
Figure 12. Automotive smart-switch with current readout
7
DESIGN FEATURES
Versatile Buck-Boost Converter
Offers High Efficiency in a Wide
by Dave Salerno
Variety of Applications
Introduction
L1 5µH
Miniature hard disk drives are a popular storage medium for MP3 music files,
digital photographs and other data
stowed in the latest portable electronics. Likewise lithium-ion batteries are
popular for these same devices, which
presents a minor problem in that mini
disk drives typically require a 3.3V
supply, which is right in the middle
of the lithium-ion battery’s operating
range (3.0V-to-4.2V). This requires a
converter that can both step down a
fully-charged Li-Ion battery and step
up the same battery as it discharges
to sub-3.3V levels.
The LTC3442 is a 1.2A buck-boost
converter that is ideal for mini disk
drive applications, and certainly for
other buck-boost appliations as well.
The LTC3442 extends battery life with
95% efficiency and fits into tight spaces
with its 3mm × 4mm DFN package. It
builds upon previous LTC buck-boost
offerings by adding programmable
automatic Burst Mode® operation,
switching frequency and average input
current limiting.
Features
The LTC3442 buck-boost converter
uses the same fixed frequency, fourswitch architecture as the LTC3440
and LTC3441, allowing it to use a
100
VIN
2.7V TO
4.2V
SW1
SW2
VIN
VOUT
1M
Li-Ion
FB
RLIM
VC
0.01µF
RT
64.9k
SGND
50
40
single inductor to regulate the output
voltage with input voltages than can
be greater or less than the output.
This provides an excellent solution
for Li-Ion to 3.3V applications, with
higher efficiency, smaller size and
lower cost than SEPIC designs. Programmable automatic Burst Mode
operation enables the converter to
change operating modes without
external intervention, for the best efficiency in portable applications. The
transition point from fixed frequency
PWM mode to Burst Mode operation
is easily programmed with a single
resistor. In addition, programmable
average input current limit allows
the user to limit the current drawn
from the power source. This feature
is useful in USB applications, where
3.6V
3.6
VIN = 3.6V
3.3V
VOUT
OUT = 3.3V
1
10
100
1k
LOAD CURRENT (mA)
Figure 2. Efficiency vs load
for the converter in Figure 1
8
100mV/DIV
AC COUPLED
1
FIXED FREQUENCY
QUENCY
QUENCY
30
20
0.1
10
AUTOMATIC
OMATIC
AUT
TRANSITION
SITION
TRAN
PO
POINT
POIN
INT
POWER LOSS (mW)
EFFICIENCY (%)
LOSS
POWER LOSS
POWER
0.1
10k
150pF
BURST
PGND
0.01µF
249k
200k
Figure 1. Li-Ion to 3.3V converter delivers 1.2A with automatic Burst Mode operation.
100
60
47µF
10k
L1: COILCRAFT MSS7341-502NXD
1000
70
2.2k
560pF
10µF
Burst Mode
90 OPERATION
80
340k
LTC3442
SHDN/SS
VOUT
3.3V
1.2A
200µs/DIV
Figure 3. Output voltage during the automatic
transition between Burst Mode operation and
Fixed Frequency operation
the allowable current draw is limited
to 500mA maximum. The four internal
100mΩ MOSFET switches provide
high efficiency, even at peak currents
up to 3A. Programmable switching
frequency and soft-start provide flexibility for many different applications.
Output disconnect, which prevents
any unwanted current flow between
VIN and VOUT during normal operation
or shutdown, is an inherent feature of
the 4-switch architecture.
4W, Li-Ion to 3.3V Converter
with Automatic Burst
Mode Operation is Ideal for
Dynamic Load Applications
A typical Li-ion to 3.3V application
circuit is shown in Figure 1. It provides
efficient, well-regulated 3.3V output
power at currents up to 1.2A with
very low ripple, even as the battery
voltage varies from 4.2V down to less
than 3V. The automatic Burst Mode
feature enables it to maintain high
efficiency, even as the load becomes
very light. This is ideal for applications such as miniature disk drives
in portable devices, which require
currents up to an amp during spinup, a few hundred milliamps during
read and write cycles, but much less
current during idle times, or when the
device goes to sleep. Figure 2 shows
Linear Technology Magazine • May 2005
DESIGN FEATURES
L1
3.3µH
MBRM120T3
USB BUS
4.35V TO 5.25V
SW1
VIN
1M
0.1Ω*
680pF
0.01µF
CIN
10µF
182k
43.2k
SW2
LTC3442
VOUT
SHDN/SS
FB
RLIM
VC
RT
BURST
SGND
controlled by the host at any time by
driving the Burst pin above or below
these thresholds.)
Another feature of the LTC3442 is
an adaptive hold circuit that keeps
the VC pin and the compensation
network charged to the correct voltage during Burst Mode operation,
for a smooth transition back to fixed
frequency operation. Figure 3 shows
the output voltage as the converter
switches automatically from Burst
Mode operation to fixed frequency
mode, in response to an increase in
load. If desired, the operating mode
can be forced by driving the Burst pin
high (for fixed frequency operation) or
low (for Burst Mode operation).
MBRM120T3
PGND
*ONLY REQUIRED IF CIN IS A CERAMIC CAP
VOUT
5V
350mA
681k
24.9k
120pF
33pF
COUT
22µF
221k
L1: COILCRAFT LPO4812-332MXC
Figure 4. A 5V converter with average input current limit for USB applications
IIN
200mA/DIV
VOUT
50mV/DIV
AC COUPLED
1MHz USB to 5V
Converter with Average
Input Current Limit
VIN
500mV/DIV
AC COUPLED
1ms/DIV
Figure 5. Step load regulation of the USB converter in Figure 4
100
200
90
175
80
150
70
125
60
100
POWER LOSS
50
40
75
50
100
150 200 250 300
LOAD CURRENT (mA)
350
50
400
Figure 6. Efficiency vs load for
the 5V USB converter in Figure 4
Linear Technology Magazine • May 2005
POWER LOSS (mW)
EFFICIENCY (%)
the converter efficiency, peaking at
95%. Maintaining regulation when
the input voltage drops below 3.3V
allows all the energy in the battery to
be used. It also allows the converter
to maintain regulation during load
transients, when the battery ESR may
cause the input voltage to drop below
3.3V momentarily. In contrast, stepdown designs lose output regulation
when the battery voltage approaches
or dips below 3.3V.
Automatic Burst Mode operation
allows the converter to change operating modes as the load current varies,
maintaining high efficiency, without
any commands required from a host.
By mirroring a small fraction of the
output current and averaging it on
the BURST pin, a voltage is produced
that is proportional to the average load
current. When this voltage exceeds
an internal threshold of 1.12V, the
converter operates in fixed frequency
mode. When the BURST voltage
drops below a threshold of 0.88V,
the converter transitions to Burst
mode operation. Therefore, raising
the value of the resistor on the Burst
pin lowers the load current at which
Burst mode is entered (values above
250K are not recommended). (Note that
the operating mode can be manually
An increasing number of portable
electronic devices and computer peripherals are operated with USB power.
Although this is convenient for the
user, it brings with it some challenges
for the designer of the USB powered device. The voltage regulator tolerance of
the host, combined with voltage drops
in bus-powered hubs and USB cables,
cause the 5V available at the end of
the USB cable to be poorly regulated,
varying from 4.35V to 5.25V (with
transients down to 4.0V). Figure 4
shows a low profile (1.2mm), USB to
5V converter using the LTC3442 for
high-power bus-powered functions.
It accepts the poorly regulated USB
input, and delivers 5V with 2% regulation and less than 20mVP–P ripple.
Figure 5 illustrates the circuit’s ability
to maintain tight regulation during line
IIN
200mA/DIV
VOUT
2V/DIV
IOUT
500mA/DIV
RLIM = 100k
CRLIM = 0.001µF
PULSED OVERLOAD
2ms/DIV
Figure 7. Input current limit overload response of USB converter.
9
DESIGN FEATURES
10
3.3µH
COILCRAFT MOS6020-332MX
R5
4.22k
VIN
2.7V TO
4.2V
SW1
SW2
VIN
VOUT
VOUT
ILED = 300mA/1A
LTC3442
OFF ON
10µF
6.3V
SD/SS
FB
RLIM
VC
2.2nF
RT
R4
1k
64.9k
33.2k
PGND
R3A
169k
2.2nF
R3B
54.9k
LOW HI
10µF
6.3V
R2
200k
BURST
SGND
OPEN LED VOLTAGE LIMIT = (R4+R5) • 0.95/R4
LHXL-PW01
R1
316k
ILED = 24 • (R1+R2+R3)/(R1 • R3) AMPS
2N7002
Figure 8. Constant current white LED driver for Li-Ion-powered applications
eliminating the need for an external
resistor.
High Efficiency, Constant
Current White LED Driver
High current white LEDs are being
used in many new applications, including flashes for cell phone cameras.
These applications demand a small,
high efficiency solution, capable of
supplying a regulated LED current,
which may need to be set anywhere
from a few hundred milliamps to over
1A , while being powered from a Liion battery. With typical white LED
voltages ranging from 3V to 4V, a
buck-boost converter is necessary to
maximize Li-ion battery life.
Most LED drivers must use a current sensing resistor to regulate the
LED current. This approach lowers
efficiency and requires added board
real estate, since the resistor must be
sized to handle the high peak current
in the LED. A unique solution for this
application is shown in Figure 8, where
the LTC3442 is configured as a fixed
frequency constant current source.
By utilizing the output current mirror
at the BURST pin, normally used for
automatic Burst Mode operation, no
current sense resistor is required. In
this application, the feedback loop is
closed on the sensed average output
current, rather than the output voltage. With essentially lossless current
sensing, 94% efficiency is achieved, as
shown in Figure 9. The LED current
can be easily programmed or changed
quickly, as in a pulsed flash, by changing the resistance on the BURST pin.
It can also be turned on and off by
means of the shutdown input. Figure 10 illustrates the response to a
continued on page 24
100
ILED = 300mA
95
EFFICIENCY (%)
and load transients. In this example,
a step load has caused the USB–supplied current to increase by 400mA,
resulting in a 600mV drop in the USB
input voltage, while VOUT exhibits only
a 60mV disturbance.
The converter efficiency is as high
as 92% at 1MHz, as shown in Figure 6.
Note that in this example, the Burst
pin is pulled high for fixed frequency
operation.
One of the restrictions placed on
users of the USB bus is a maximum
allowed current draw of 500mA. To
guarantee that this limit is not exceeded, USB powered solutions often
employ additional current limiting
circuitry, increasing size and cost.
The LTC3442 solves this problem by
including a programmable average
input current limit, which works by
mirroring a small fraction of the input
current and averaging it on the RLIM
pin, using an external RC network.
The RLIM voltage is also connected
to an internal amplifier with a 1V
reference. When the RLIM voltage
reaches 1V, the amplifier clamps the
VC pin, lowering the output voltage as
needed to prevent the input current
from increasing any further. In the
example of Figure 4, the input current is limited to less than 500mA in
the event of an overload. The current
limit response time is set by the filter
capacitor on the RLIM pin. Figure 7
illustrates the circuit’s response to an
overload, with VOUT dropping as IOUT
increases and the USB input current
is clamped to 0.5A.
In this application, Schottky diodes
are required to limit the peak voltage
on the switch nodes and also provide
a small efficiency improvement. Note
that since the diodes are back-to-back,
the output disconnect feature of the
LTC3442 is maintained. The resistor
in series with the input filter capacitor
damps any oscillation or overshoot
resulting from the input capacitor
resonating with the USB cable inductance when the cable is first attached.
This damping resistor is only required
if a ceramic input capacitor is used.
When using a tantalum capacitor, the
ESR of the capacitor provides damping,
1A
90
ILED = 1A
ILED
200mA/
DIV
85
80
300mA
75
70
3
4
3.5
4.5
VIN (V)
Figure 9. Efficiency vs load for the
high current LED driver in Figure 8
2ms/DIV
Figure 10. Step response of the LED
constant current driver in Figure 8
for flash applications
Linear Technology Magazine • May 2005
DESIGN FEATURES
Low EMI, Output Tracking, High
Efficiency, and Too Many Other
Features to List in a 3mm x 4mm
Synchronous Buck Controller by Lin Sheng
Introduction
How It Works
The LTC3808 synchronous DC/
DC controller packs many features
required by the latest electronic devices into a low profile (0.8mm tall),
3mm × 4mm leadless DFN package,
or a leaded SSOP-16 package. The
LTC3808 can provide output voltages
as low as 0.6V and output currents as
high as 7A from a wide, 2.75V to 9.8V,
input range, making it an ideal device
for battery powered and distributed
DC power systems. It also includes
important features for noise-sensitive
applications, including a phase-locked
loop (PLL) for frequency synchronization and spread spectrum frequency
modulation to minimize electromagnetic interference (EMI).
The LTC3808 improves battery
life and saves space by delivering
high efficiency with a low operating
quiescent current. The LTC3808 also
takes advantage of No RSENSETM current mode technology by sensing the
voltage across the main (top) power
MOSFET to improve efficiency and
reduce the size and cost of the solution. Its adjustable high operating
frequency (300kHz–750kHz) allows the
use of small surface mount inductors
and ceramic capacitors for a compact
power supply solution.
The LTC3808 offers flexibility of
start-up control with a fixed internal
start-up time, an adjustable external
soft-start, or the ability to track another voltage source. It also includes
other popular features, such as a
Power Good voltage monitor, current
mode control for excellent AC and DC
line and load regulation, low dropout
(100% duty cycle) for maximum energy extraction from a battery, output
overvoltage protection and short circuit current limit protection.
Figure 1 shows a step-down converter
with an input of 5V and an output
of 2.5V at 5A. Figure 2 shows its
efficiency versus load current. The
LTC3808 uses a constant frequency,
current mode architecture to drive an
external pair of complementary power
MOSFETs. During normal operation,
Linear Technology Magazine • May 2005
The LTC3808 can provide
output voltages as low as
0.6V and output currents
as high as 7A from a
wide, 2.75V to 9.8V, input
range, making it an ideal
device for battery powered
and distributed DC power
systems.
the top P-channel MOSFET is turned
on every oscillator cycle, and is turned
off when the current comparator trips.
The peak inductor current at which
the current comparator trips is determined by the voltage on the ITH pin,
2
1
8
220pF
CITH 15k
RITH
1M 4
6
3
187k
5
59k
SYNC/MODE
VIN
SENSE+
PLLLPF
IPRG
TG
PGOOD
ITH
SENSE–
LTC3808EDE
TRACK/SS
VFB
SW
BG
GND
15
RUN
12
which is driven by the output of the
error amplifier. The VFB pin receives the
output voltage feedback signal from an
external resistor divider. This feedback
signal is compared to the internal 0.6V
reference voltage by the error amplifier.
While the top P-channel MOSFET is
off, the bottom N-channel MOSFET
is turned on until either the inductor
current starts to reverse, as indicated
by a current reversal comparator, or
the beginning of the next cycle.
Selectable Operation Modes
in Light Load Operation
The LTC3808 can be programmed
for three modes of operation via the
SYNC/MODE pin: high efficiency
Burst Mode operation, forced continuous conduction mode or pulse skipping
mode at low load currents. Burst Mode
operation is enabled by connecting the
SYNC/MODE pin to VIN. In this mode,
the peak inductor current is clamped
to about one-fourth of the maximum
value and the ITH pin is monitored
to determine whether the device will
10µF
10Ω
1µF
VIN
2.75V TO 8V
11
10
MP
13
L
1.5µH
14
9
7
VOUT
2.5V
(5A AT VIN = 5V)
MN
Si7540DP
COUT
150µF
100pF
L: VISHAY IHLD-2525CZ-01
Figure 1. A 550kHz, synchronous DC/DC converter with 5V input and 2.5V output at 5A
11
DESIGN FEATURES
Shutdown and
Start-Up Control
The LTC3808 is shut down by pulling
the RUN pin below 1.1V. In shutdown,
all controller functions are disabled
while the external MOSFETs are held
off, and the chip draws less than 9µA.
12
10k
EFFICIENCY
95
VIN = 3.3V
1k
VIN = 5V
VIN = 4.2V
80
100
TYPICAL POWER
LOSS (VIN = 4.2V)
70
10
60
50
1
VOUT = 2.5V
1
10
100
1k
LOAD CURRENT (mA)
VIN = 5V, VOUT = 2.5V
90
0.1
10k
EFFICIENCY (%)
90
100
POWER LOSS (mW)
100
EFFICIENCY (%)
go into a power-saving SLEEP mode.
When the inductor’s average current
is higher than the load requirement,
the voltage at the ITH pin drops as the
output voltage rises slightly. When
the ITH voltage goes below 0.85V, the
device goes into SLEEP mode, turning
off the external MOSFETs and much
of the internal circuitry. The load current is then supported by the output
capacitors, and the LTC3808 draws
only 105µA of quiescent current. As
the output voltage decreases, ITH is
driven higher. When ITH rises above
0.925V, the device resumes normal
operation.
Tying the SYNC/MODE pin to a DC
voltage below 0.4V (e.g., GND) enables
forced continuous mode which allows
the inductor current to reverse at
light loads or under large transient
conditions. In this mode, the P-channel MOSFET is turned on every cycle
(constant frequency) regardless of the
ITH pin voltage so that the efficiency
at light loads is less than in Burst
Mode operation. However it has the
advantages of lower output ripple and
no noise at audible frequencies.
When the SYNC/MODE pin is
clocked by an external clock source
to use the phase-locked loop or is
set to a DC voltage between 0.4V and
several hundred millivolts below VIN
(e.g., VFB), the LTC3808 operates in
PWM pulse skipping mode at light
loads. In this mode, cycle skipping
occurs under light load conditions
because the inductor current is not
allowed to reverse. This mode, like
forced continuous operation, exhibits
low output ripple as well as low audible
noise as compared to Burst Mode
operation. Its low-current efficiency is
better than forced continuous mode,
but not nearly as high as Burst Mode
operation. Figure 3 shows the efficiency versus load current for these
three operation modes.
85
BURST MODE
(SYNC/MODE =
VIN)
80
75
FORCED
CONTINUOUS
(SYNC/MODE = 0V)
70
65
60
PULSE SKIPPING
(SYNC/MODE = 0.6V)
55
50
1
10
100
1k
LOAD CURRENT (mA)
10k
Figure 2. Efficiency and power loss vs load
current of the circuit in Figure 1
Figure 3. Efficiency vs load current in three
operation modes for the circuit in Figure 1
Releasing the RUN pin allows an internal 0.7µA current source to pull
up the RUN pin to VIN. The controller
is enabled when the RUN pin reaches
1.1V. Alternatively, the RUN pin can be
driven directly from a logic output.
The start-up of VOUT is based on
the three different connections on
the TRACK/SS pin. When TRACK/
SS is connected to VIN, the start-up
of VOUT is controlled by the internal
soft-start, which rises smoothly from
0V to its final value in about 1ms. A
second start up mode allows the 1ms
soft-start time to increase or decrease
by connecting an external capacitor
between the TRACK/SS pin and the
ground. When the controller is enabled
by releasing the RUN pin, TRACK/SS
pin is charged up by an internal 1µA
current source and rises linearly from
0V to above 0.6V. The error amplifier
compares the feedback signal VFB to
this ramp instead of the internal softstart ramp, and regulates VFB linearly
from 0V to 0.6V.
In this case, the LTC3808 regulates
the VFB to the voltage at the TRACK/
SS pin. Therefore, in the third mode,
VOUT of LTC3808 can track an external voltage VX during start-up if a
resistor divider from VX is connected
to the TRACK/SS pin. For coincident
tracking during startup, the regulated
final value of VX should be larger than
that of VOUT, and the resistor divider
on VX would have the same values as
the divider on VOUT that is connected
to VFB.
NOISE (dBm)
–10dBm/DIV
NOISE (dBm)
–10dBm/DIV
START FREQ: 400kHz
RBW: 100Hz
STOP FREQ: 700kHz
a. Without SSFM
Selecting an
Operating Frequency
The choice of operating frequency
fOSC is generally a trade-off between
efficiency and component size. Low
frequency operation improves efficiency by reducing MOSFET switching
losses (both gate charge and transition
losses). Nevertheless, lower frequency
operation requires more inductance for
a given amount of ripple current.
START FREQ: 400kHz
RBW: 100Hz
STOP FREQ: 700kHz
b. With SSFM
Figure 4. Spread spectrum modulation of the controller operating frequency
lowers peak EMI as seen in this comparison of the VOUT spectrum without spread
spectrum modulation (a) and with spread spectrum modulation (b).
Linear Technology Magazine • May 2005
DESIGN FEATURES
The internal oscillator for the
LTC3808’s controller runs at a nominal
550kHz frequency when the PLLLPF
pin is left floating and the SYNC/MODE
pin is a DC voltage and not configured
for spread spectrum operation. Pulling the PLLLPF to VIN selects 750kHz
operation; pulling the PLLLPF to GND
selects 300kHz operation.
Alternatively, the LTC3808 can
phase-lock to a clock signal applied to
the SYNC/MODE pin with a frequency
between 250kHz and 750kHz, and a
series RC filter must be connected
between the PLLLPF pin and ground
as the loop filter. In this case, pulseskipping mode is enabled under light
load conditions to reduce noise.
Spread spectrum frequency modulation reduces the amplitude of EMI
by spreading the nominal 550kHz
operating frequency over a range of frequencies between 460kHz and 635kHz
with pseudo random pattern (repeat
frequency of the pattern is about
4kHz). Spread spectrum frequency
modulation is enabled by biasing the
SYNC/MODE pin to a DC voltage above
1.35V and VIN – 0.5V. An internal
2.6µA pull-down current source at
SYNC/MODE can be used to set the
DC voltage at this pin by tying a resistor with an appropriate value between
SYNC/MODE and VIN. A 2.2nF filter
cap between PLLLPF and ground and
a 1000pF cap between SYNC/MODE
and PLLLPF are needed in this mode.
Figure 4 shows the frequency spectral
plots of the output (VOUT) with and
without spread spectrum modulation.
Note the significant reduction in peak
output noise (>20dBm).
Power Good Monitor
and Fault Protection
A window comparator monitors the
feedback voltage and the open-drain
PGOOD output is pulled low when the
feedback voltage is not within 10% of
the reference voltage of 0.6V.
The LTC3808 incorporates protection features such as programmable
current limit, input undervoltage lockout, output overvoltage protection and
10µF
10
2
1
8
1M 4
100pF
22k
10nF
118k
6
3
5
59k
SYNC/MODE
VIN
SENSE+
PLLLPF
IPRG
TG
PGOOD
ITH
SENSE–
LTC3808EDE
SW
TRACK/SS
VFB
BG
GND
RUN
12
VIN
2.75V TO 4.2V
1µF
11
10
13
14
9
MP
Si3447BDV
L
1.5µH
VOUT
1.8V
2A
MN
Si3460DV
COUT
22µF
x2
7
15
100pF
L: VISHAY IHLD-2525CZ-01
Figure 5. A 750kHz, synchronous single cell Li-Ion to 1.8V/2A converter
with external soft-start and a ceramic output capacitor
programmable short circuit current
limit.
Current limit is programmed by the
IPRG pin. The maximum sense voltage across the external top P-channel
MOSFET or a sense resistor is 125mV
when the IPRG pin is floating, 85mV
when IPRG is tied low and 204mV
when IPRG is tied high.
To protect a battery power source
from deep discharge, an internal
undervoltage lockout circuit shuts
down the device when VIN drops below
2.25V to reduce the current consumption to about 3µA. A built-in 200mV
hysteresis ensures reliable operation
with noisy supplies.
During transient overshoots and
other more serious conditions that
may cause the output to rise out of
regulation (>13.33%), an internal
overvoltage comparator will turn
off the top P-channel MOSFET and
turn on the synchronous N-channel
MOSFET until the overvoltage condition is cleared.
In addition, the LTC3808 has a
programmable short circuit current
limit protection comparator to limit the
inductor current and prevent excessive MOSFET and inductor heating.
This comparator senses the voltage
across the bottom N-channel MOSFET
and keeps the P-channel MOSFET off
until the inductor current drops below
the short circuit current limit. The
maximum short-circuit sense voltage
is about 90mV when the IPRG pin is
floating, 60mV when IPRG is tied low
and 150mV when IPRG is tied high.
Single Cell Li-Ion to
1.8V/2A Application
Figure 5 shows a step-down application from 3.3V to 1.8V at 2A. The circuit
operates at a frequency of 750kHz, so
a small inductor (1.5µH) and ceramic
output capacitor (two 22µF caps) can
be used. A 10nF capacitor at TRACK/
SS sets the soft-start time of about
6ms. The RDS(ON) of the P-channel
MOSFET determines the maximum
average load current that the controller can drive. The Si3447BDV in
this case ensures that the output is
capable of supplying 2A with a low
input voltage.
Conclusion
The LTC3808 offers flexibility, high
efficiency, low EMI and many other
popular features in a tiny 3mm ×
4mm DFN package or a small 16-lead
narrow SSOP package. For low voltage
portable or distributed power systems
that require small footprint, high efficiency and low noise, the LTC3808
is an excellent fit.
For more information on parts featured in this issue, see
http://www.linear.com/designtools
Linear Technology Magazine • May 2005
13
DESIGN FEATURES
Tiny RS232 Transeivers Run Directly
from Alkaline, NiMH or NiCd Batteries
by Kevin Wrenner and Troy Seman
Introduction
Six new devices comprise a family of
small-footprint RS-232 transceivers
that operate at up to 1Mbps over a
supply range of 1.8V to 5.5V. The
LTC2801 and LTC2802 are single
transceivers available in 4mm × 3mm
DFN packages, and the LTC2803 and
LTC2804 are dual transceivers available in 5mm × 3mm DFN packages.
The LTC2803-1 and LTC2804-1 are
dual transceivers offered in 16-pin
SSOP packages. The wide supply
range permits operation directly from
two alkaline, NiCd, or NiMH battery
cells, while a separate VL supply pin
eliminates interfacing problems in
mixed-supply systems.
L1
10µH
1.8V TO 5.5V
C4
1µF
2V/DIV
SW
VCC
TIN
CAP
PS
OFF ON
5V/DIV
MODE
TOUT
TIN
TOUT
RIN
ROUT
2V/DIV
ROUT
C1
220nF
LTC2802
VL
150pF
GND
250pF
VEE
VDD
C2
1µF
400ns/DIV
C3
1µF
a.
b.
Figure 1. Operating waveforms at 1.8V and 1Mbps with driver and receiver
fully loaded (a) and transmitter loopback mode test circuit (b)
Achieving the higher signaling
rate—50× the rate provided for in
the original standard—necessitates
slewing the driver faster than the
standard’s 30V/µs limit. The slower
parts, the LTC2801 and LTC2803,
are fully RS232 compliant. Output
levels of all parts are RS232 compliant at their rated data rates even at
1.8V supply.
Figure 2 shows the relationship
of supply current to supply voltage
required to drive 1nF/3kΩ loads at
1Mbps and 250kbps
Data Rate
All of the devices are capable of driving
standard RS232 loads (2.5nF/3kΩ) at
100kbps, and 1nF/3kΩ at 250kbps.
The faster parts, the LTC2802,
LTC2804 and LTC2804-1, can also
drive 250pF/3kΩ at 1Mbps. Waveforms for a single transceiver operating
at 1Mbps and 1.8V in a transmitterloopback configuration are shown in
Figure 1.
various data rates. Figure 3 shows
the supply current sensitivity to data
rate at 1.8V.
More Features
Up to four operating modes are available, depending on the part (Table 1).
The DFN parts have two power-saving
modes. In Shutdown mode, current
draw on each supply is reduced below 1µA. Receiver and driver outputs
are high impedance, eliminating any
problem associated with powering
Table 1. Feature summary
Drivers and Receivers
Package
LTC2801
LTC2802
LTC2803
LTC2803-1
LTC2804
LTC2804-1
1+1
1+1
2+2
2+2
2+2
2+2
12-lead
4mm × 3mm
DFN
12-lead
4mm × 3mm
DFN
16-lead
5mm × 3mm
DFN
16-lead
SSOP
16-lead
5mm × 3mm
DFN
16-lead
SSOP
100kbps for RL=3kΩ, CL=2.5nF
250kbps for RL=3kΩ, CL=1nF
1Mbps for RL=3kΩ, CL=250pF
30V/µs Maximum Slew Rate
Shutdown
Receiver(S) Active
Driver Disable
14
Linear Technology Magazine • May 2005
DESIGN FEATURES
25
125kbps
15
10
20.8kbps
5
0
1
2
50
40
30
125kbps
20
3
4
5
SUPPLY VOLTAGE (V)
6
0
20.8kbps
1nF
2
250pF
40
3
4
5
SUPPLY VOLTAGE (V)
0
6
b.
Each device in the LTC2801 family
drives RS232 compliant output levels over its entire input supply range
using an integrated dual regulator
(Figure 4) that replaces the charge
pump voltage multiplier found in many
RS232 integrated circuits. Excellent
LTC2804
LTC2802
200
0
600
400
DATA RATE (kbps)
800
1000
Figure 3. Supply current vs data rate
(single and dual transceiver)
Figure 2. Supply current vs supply voltage for single (a) and dual (b) transceiver
Dual Regulator
250pF
20
a.
down a part connected to a receiver
output. Receiver(s) Active mode is like
Shutdown except receivers are biased
at low current. With only 15μA current
draw, one or two receivers can listen
for a wake-up signal. Besides the
Normal full-duplex operating mode, a
Driver(s) Disabled mode is available to
support line sharing and half-duplex
operation.
These parts have built-in measures that permit reliable operation
in the sometimes-harsh environment
encountered in RS232 interfaces.
All device pins are protected against
electrostatic discharge (ESD) events
without damage or latch-up. Interface pins have additional protection,
tolerating repeated 10kV human body
model discharges. Both driver and
receiver outputs are current limited.
1nF
60
LTC2804
LTC2803
1
ALL DRIVERS SWITCHING
VCC = VL = 1.8V
RL = 3kΩ
80
250kbps
10
LTC2802
LTC2801
100
ALL DRIVERS SWITCHING
VCC = VL
RL = 3kΩ
CL = 1nF
60
SUPPLY CURRENT (mA)
SUPPLY CURRENT (mA)
30
20
70
ALL DRIVERS SWITCHING
VCC = VL
RL = 3kΩ
250kbps
CL = 1nF
SUPPLY CURRENT (mA)
35
C1
220nF
L1
10µH
1.8V TO 5.5V
C4
1µF
VCC
CAP
SW
VDD
C2
1µF
VL
1.8V TO 5.5V
BOOST
REGULATOR
C5*
220nF
VEE
C3
1µF
*OMIT IF VL IS CONNECTED TO VCC
Figure 4. Dual regulator and recommended biasing
line and load regulation is achieved
with a constant frequency (1.2MHz
typical) boost regulator that generates
a positive supply of 7V and a coupled
inverting charge pump that generates a negative supply of –6.3V. Like
its charge pump voltage multiplier
counterpart, regulator switching varies according to the driver loading. The
regulator operates in a pulse skipping
mode when driver activity/loading is
low. Because all its Schottky diodes
C1
220nF
L1
10µH
2 ALKALINE,
NiCd, OR
NiMH CELLS
+
C4
1µF
–
*
DC-DC
VCC
SW
CAP
1.8V
VL
VCC
*
C5
220nF
µP
PPx
PPy
TXD
PPz
RXD
LTC2804
PS
MODE
T2IN
T2OUT
T1IN
T1OUT
R2OUT
R2IN
R1OUT
R1IN
GND
VDD
CTS
RX
UART
RTS
TX
VEE
C2
1µF
C3
1µF
*ADDITIONAL BYPASS CAP AS NEEDED
Figure 5. Example board layout
with 5mm × 3mm DFN package
Linear Technology Magazine • May 2005
Figure 6. Diagnostic port operating directly off unregulated battery
15
DESIGN FEATURES
1.8V TO 5.5V
2.5V TO 5.5V
L1
10µH
VCC
VL
LTC2802
R T
VCC
C4
2µF
PS
SW
LTC2803
VL
C1
470nF
CAP
VCC
SW
LTC2803
VL
CAP
MODE
TOUT
TIN
3.3k
RIN
ROUT
GND
T2IN
T2OUT
T2IN
T2OUT
T1IN
T1OUT
T1IN
T1OUT
R2OUT
R2IN
R2OUT
R2IN
R1OUT
R1IN
R1OUT
R1IN
VEE
GND
GND
VDD
VDD
VEE
Figure 7. Half-duplex mode on RS232
interface. The logic interface shares a
single wire, too.
are integrated, the regulator requires
only five external components: one
small inductor and four tiny ceramic
capacitors (Figure 5).
Battery-Operated
Microcontroller Interface
The advantage of the VL interface
logic supply feature can be seen in
Figure 6, which shows a battery-operated RS232 interface to a diagnostic
port on a 1.8V microprocessor. For
maximum efficiency, the LTC2804 is
operated directly off the battery voltage. The VL pin is connected to the
microprocessor’s regulated 1.8V supply, setting the RxOUT high level and
the TxIN and control input threshold
voltages, which are automatically
scaled. This configuration can extend
battery life while eliminating the need
for level translators.
Half-Duplex on Shared Line
RS232 transceivers are often used in
configurations outside the scope of the
original standard. Figure 7 shows an
LTC2802 configured to signal half-duplex over a single RS232 interface wire.
The logic interface, too, shares a single
wire between driver and receiver. With
PS kept high, the MODE input serves
as a low-latency driver enable that can
switch between transmit and receive
modes within 2μs. Using a switchable
terminator in the remote device can
help avoid degrading output levels and
increasing power consumption.
C2
2µF
C3
2µF
ANY COMBINATION
LTC2801/LTC2802/LTC2803/LTC2804
Figure 8. Quad transceiver with reduced component count
Quad Transceiver
Adjustable Level Translator
Dual transceivers are commonly used
to provide a bidirectional interface
that includes a data line and a hardware handshaking control signal. If
two such ports are needed, two dual
transceiver devices can share one
device’s regulator (Figure 8). Tie both
device’s CAP pins together, connecting
in parallel the inverting charge pump
Schottky diodes from both devices. The
negative supply level is improved due
to a reduction in the combined diode’s
forward voltage. The second device’s
unused SW pin should be grounded.
This configuration eliminates one set
of external components.
Any RS232 transceiver is a bidirectional level translator. With the regulator
and drivers disabled, the receiver(s)
can provide simple unidirectional level
translation with the output high level
defined by the VL supply (Figure 9).
This makes a useful 3V-to-5V or
5V-to-1.8V inverting translator capable of 1Mbps. A static dual translator
consumes 120μA current. If hysteresis
is not required, the MODE and PS pin
connections can be reversed to obtain
a lower power version (15μA static)
capable of 100kbps.
1.8V TO 5.5V
C5
220nF
VL
LTC2803
3V TO 25V
–25V TO 0V
OFF ON
R2IN
R2OUT
R2IN
R1OUT
PS
MODE
VCC
T2IN
SW
T1IN
GND
VDD
VL
0V
Conclusion
The LTC2801 family’s wide input range
of 1.8V to 5.5V enables these parts to
provide RS232 interfaces with fully
compliant output levels using a broad
range of power sources. The small
footprint required by each part and
its external components (Figure 5),
independent logic interface supply,
and power saving features, make this
family of parts an attractive choice
for designing low cost standardized
signaling interfaces into modern consumer electronics.
VEE
Authors can be contacted
at (408) 432-1900
Figure 9. Inverting level translator
16
Linear Technology Magazine • May 2005
DESIGN FEATURES
Low Voltage Hot Swap Controller
with Inrush Current Control by Chew Lye Huat
Introduction
The LTC4216 is a low voltage Hot Swap
controller that allows a board to be
safely inserted and removed from a live
backplane. The LTC4216 is designed
to meet the latest low voltage board
supply requirements with its unique
feature of controlling load voltages
from 0V to 6V. It also features an adjustable soft-start that provides both
inrush current limiting and current
slew rate control at start-up, important
for the large load capacitors typical in
low-voltage applications.
When a board is plugged into a
backplane, the inrush currents can be
large enough to create a glitch on the
load supply causing other boards on
the bus to malfunction. The LTC4216
provides a low circuit breaker trip
threshold (25mV) with adjustable
response time and analog current
limiting for dual level overcurrent
protection. It also includes a high side
gate drive for an external N-channel
MOSFET. Figure 1 shows a circuit
using the LTC4216 as a Hot Swap
controller for a 1.8V load supply.
pin for powering the device’s internal
circuitry with a minimum of 2.3V. An
RC network shown in Figure 1 can be
connected at the VCC pin to ride out
supply glitches during output-shorts
or adjacent board transients. These
supply glitches can potentially trigger the device into an undervoltage
lockout condition, causing its internal
latches to reset.
Controlling Load Voltages
Down to Zero Volts
Soft-Start Controls
Inrush Current Slew Rate
Output Voltage Monitoring
The output voltage is monitored
through a resistive divider connected
at the feedback (FB) pin, and an FB
comparator with a 0.6V reference.
The FB comparator has a built-in
glitch filter to ride out any unwanted
transients appearing on the FB pin.
When the FB pin voltage exceeds
0.6V, it signals the RESET high after
a power-good delay set by an external
capacitor at the TIMER pin. The delay
is given by:
ms
1.253V • CTIMER
= 0.6265 • CTIMER  
 nF
2µA
The LTC4216 can control load voltages
as low as 0V as it provides two separate
pins: SENSEP pin for controlling the
load voltages from 0V to 6V and VCC
The LTC4216 features a soft-start
function that controls the slew rate of
the inrush current during power-up
(Figure 2). The rate is controlled by an
external capacitor connected from the
soft-start (SS) pin to ground. A built-in
Analog Current Limit (ACL) amplifier
servos the GATE pin to track the rate
of SS ramp-up during power-up. There
are two slopes in the SS ramp-up
profile: a 10µA pull-up for a normal
ramp-rate, and a 1µA pull-up for a
slow ramp rate. The slow SS ramp rate
allows the gate of the external MOSFET
to be turned on with a small inrush
current step. When the load current
starts flowing through the external
sense resistor, SS reverts back to a
normal ramp rate. At the end of the
SS ramp-up, the GATE is servoed to
limit the load current to 40mV across
the sense resistor during startup. If
the voltage across the sense resistor
drops below 40mV due to reduced
load current, the ACL amplifier shuts
off and GATE ramps further with a
20µA pull-up.
Inrush Control
with a GATE Capacitor
Figure 3 shows an alternative approach from the soft-start method to
limit the inrush current during power
up for a large load capacitor. An external capacitor, C4, is connected from
the GATE pin to ground to limit the
inrush current by slewing the GATE
pin voltage. With a GATE pull-up
BACKPLANE PCB EDGE
CONNECTOR CONNECTOR
(FEMALE)
(MALE)
VIN
1.8V
VCC
3.3V
LONG
22Ω
VCC
SENSEP SENSEN GATE
330nF
SHORT
15k
1%
GND
LONG
FB
LTC4216
ON
20k TIMER
1%
10nF
SS
VOUT
1.8V
5A
Si4864DY
0.004Ω
LONG
FILTER
10nF
17.4k
1%
3.3V
10k
1%
10k
+
10k
1000µF
µP
LOGIC
FAULT
FAULT
GND RESET
RESET
18nF
4216 TA01
Figure 1. A 1.8V Hot Swap application
Linear Technology Magazine • May 2005
17
DESIGN FEATURES
current of 20µA, the GATE slew rate
is given by:
dVGATE
20µA
=
dt
C4 + CISS
where CISS is the external MOSFET’s
gate input capacitance. The inrush
current flowing into the load capacitor,
CLOAD, is limited to:
dV
C
IINRUSH =CLOAD • GATE = LOAD • 20µA
dt
C4 + CISS
For the application shown, CLOAD =
470µF, C4 = 22nF and CISS = 3nF,
IINRUSH = 376mA. If CLOAD is very large
and IINRUSH exceeds the analog current
limit, the GATE servos to control the
inrush current to 40mV/RSENSE.
Electronic Circuit Breaker
The load current is sensed by monitoring the voltage across an external sense
resistor, RSENSE, connected between
SENSEP and SENSEN pins in Figure 1.
The Electronic Circuit Breaker (ECB)
trips at 25mV across the sense resistor during an overload condition. The
response time is adjustable through
an external capacitor connected from
the FILTER pin to ground. Whenever
the ECB trip threshold is exceeded, the
FILTER pin charges up the external
capacitor with a 60µA pull-up. Otherwise, it is pulled down by a 2.4µA
current. When the FILTER pin voltage
exceeds 1.253V, the ECB trips and the
GATE pin is pulled down to ground im-
VIN
5V
IOUT
2.5A/DIV
VOUT
1V/DIV
0.5ms/DIV
Figure 2. Power-up with soft-start
for inrush control
mediately to disconnect the board from
the backplane supply. The FAULT pin
is also pulled low whenever the ECB
trips. In order to reconnect the board,
the ON pin must be pulled below 0.4V
for at least 100µs to reset the ECB,
or the VCC pin voltage must be below
2V for more than 200µs.
Analog Current Limiting
Protects Against Severe
Overcurrent Fault
BACKPLANE PCB EDGE
CONNECTOR CONNECTOR
(FEMALE)
(MALE)
LONG
RSENSE
0.01Ω
RX
10Ω
CX
100nF
Figure 4 shows a normal power-up
sequence with a large capacitor load
in Figure 1. When the VCC pin voltage
rises above 2.1V and the ON pin is
greater than 0.8V, the LTC4216 starts
the first timing cycle. A 2µA current
source charges an external capacitor
(C1) connected from the TIMER pin to
ground. When TIMER pin voltage rises
above 1.253V, the TIMER pin is pulled
R5
10k
CY
330nF
M1
Si9426DY
R6
10Ω
RY
22Ω
VCC SENSEP SENSEN GATE
SHORT
SHORT
RESET
LTC4216
R2
10k
LONG
C4
22nF
FB
R4
64.9k
1%
+
VOUT
5V
CLOAD 2A
470µF
R3
10k
1%
ON
FILTER
TIMER
GND
Normal Power-Up Sequence
In addition to an Electronic Circuit
Breaker (ECB), the LTC4216 includes an Analog Current Limit (ACL)
amplifier that does not require an
external compensation capacitor at
the GATE pin. The amplifier’s stability is compensated by the large gate
input capacitance (CISS ≥ 1nF) of the
external MOSFET used. The GATE
Z1
RESET
pin is servoed to limit the load current
to 40mV/RSENSE. The ACL threshold
(40mV) is 1.6 times higher than the
ECB trip threshold (25mV) to provide
dual level current sensing. When the
output is in current limit, it exceeds the
ECB trip threshold causing the FILTER
pin to charge up the external capacitor
with a 60µA pull-up. If the condition
persists long enough for the FILTER
pin voltage to reach its threshold,
the GATE is pulled low and FAULT is
latched low. If the voltage across the
sense resistor exceeds 40mV during an
overload condition, the ACL amplifier
pulls the GATE down in an attempt
to control the load current. For a mild
short terrm overload, the ACL amplifier can immediately control the load
current. However, in the event of a
severe overload, the load current may
overshoot as the MOSFET has large
gate overdrive initially. The GATE is
quickly discharged to ground followed
by the ACL amplifier taking control.
VGATE
5V/DIV
C1
10nF
GND
C3
68nF
Z1: SMAJ6.0A
Figure 3. Application with an external GATE capacitor to enhance inrush control
18
Linear Technology Magazine • May 2005
DESIGN FEATURES
VON
2V/DIV
VON
2V/DIV
VON
2V/DIV
VTIMER
1V/DIV
VTIMER
1V/DIV
VTIMER
1V/DIV
VSS
1V/DIV
VSS
1V/DIV
VGATE
2V/DIV
VGATE
5V/DIV
VGATE
2V/DIV
VFILTER
1V/DIV
VOUT
1V/DIV
VFILTER
1V/DIV
Figure 7. Auto-retry with short at 5V output
VRESET
2V/DIV
VFAULT
5V/DIV
20ms/DIV
discharges through a 2.4µA pull-down
until the device resets.
2ms/DIV
Auto-Retry Application
2ms/DIV
Figure 4. Power-up sequence with load
Figure 6 shows an application that
automatically tries to power up the
board after the Electronic Circuit
Breaker (ECB) has been tripped due
to a shorted load supply output. The
ON pin is shorted to the FAULT pin
and is pulled up by a 200kΩ resistor (RAUTO) to the load supply. A 1µF
capacitor (CAUTO) connected from the
lower end of RAUTO to ground sets the
auto-retry duty cycle. The LTC4216
will retry as long as the short persists.
RAUTO and CAUTO must be selected to
keep the duty cycle low in order to
prevent overheating in the external
N-channel MOSFET.
Figure 7 shows the auto-retry
cycle when the 5V output is shorted
to ground. The ECB is tripped when
the FILTER pin voltage rises above
1.253V after the first timing cycle.
This causes the F
 A
 U
 L
 T
 pin to be pulled
Figure 5. Power-up with short at 1.8V output
low and C1 is discharged. After this,
the Electronic Circuit Breaker (ECB)
is enabled and a GATE ramp-up cycle
begins. GATE is held low initially by
the ACL amplifier until SS switches
from the 10µA pull-up to the 1µA
pull-up for a slower ramp rate. The
slew rate of the inrush current is in
control as GATE ramps up gradually,
tracking the SS ramp rate. SS reverts
back to a normal ramp rate when the
load current starts flowing through
the sense resistor. At the end of the
SS ramp, GATE continues to ramp up
with a 20µA pull-up if the output is
not in current limit. The second timing
cycle starts when the FB pin voltage
exceeds 0.6V. RESET goes high after a
complete timing cycle, indicating that
power is good.
Power-Up into an
Output-Short Sequence
Figure 5 shows power-up with a short
at the output in Figure 1. After the
initial timing cycle, GATE ramps up
and the external MOSFET is turned
on. The load current rises due to the
output short, causing the voltage
across the sense resistor to rise above
25mV. The FILTER pin charges up
the external capacitor with a 60µA
pull-up while the output is in current
limit. The output current is limited to
40mV/RSENSE as the GATE regulates.
When the FILTER pin voltage rises
above 1.253V, the Electronic Circuit
Breaker trips and both GATE and SS
are pulled low. The device latches-off
and FAULT is pulled low, indicating a
fault condition. The FILTER capacitor
continued on page 26
VIN
5V
BACKPLANE PCB EDGE
CONNECTOR CONNECTOR
(FEMALE)
(MALE)
LONG
RESET
Z1
RSENSE
0.004Ω
RAUTO
200k
SHORT
R5
10k
RX
10Ω
CX
100nF
CY
330nF
RY
22Ω
R4
64.9k
1%
VCC SENSEP SENSEN GATE
FB
RESET
LTC4216
FAULT
CAUTO
1µF
GND
M1
Si4864DY
ON
GND
TIMER
C1
100nF
LONG
SS
+
VOUT
5V
CLOAD 5A
470µF
R3
10k
1%
FILTER
C2
4.7nF
C3
22nF
Z1: SMAJ6.0A
Figure 6. Auto-retry application
Linear Technology Magazine • May 2005
19
DESIGN IDEAS
Monolithic Synchronous Step-Down
Regulator Drives 8A Loads with Few
by Joey M. Esteves
External Components
Introduction
I/O SUPPLY
VOLTAGE
2.5V
The LTC3418 is a monolithic synchronous, step-down switching regulator
that is capable of delivering 8A of
output current for microprocessor
and I/O supplies, point of load regulation, and automotive applications.
Internal power MOSFET switches, with
1k
2k
TRACK
VIN
3.3V
PVIN
SVIN
PGOOD
DESIGN IDEAS
Monolithic Synchronous Step-Down
Regulator Drives 8A Loads with
Few External Components ........... 20
Monolithic Step-Down Regulator
Withstands Rigors of Automotive
Environments and Consumes Only
100µA of Quiescent Current ........ 23
David Kim
600mA Switching Converter Reduces
Noise by Automatically Shifting to a
Linear Regulator at Light Loads
.................................................... 29
Kevin Soch
Single Converter Provides
Positive and Negative Supplies .... 30
SGND
ITH
Cheng-Wei Pei
Compact DDR Memory Power ....... 36
Jason Leonard
1k
2k
80
EFFICIENCY (%)
70
60
50
40
30
20
10
0
0.01
VIN = 3.3V
VOUT = 1.2V
f = 2MHz
1
0.10
LOAD CURRENT (A)
10
Figure 2. Efficiency vs Load Current
20
1000pF
2200pF
90
Tom Gross
Temperature-to-Frequency Converter
Runs for Years on Two AA Batteries
.................................................... 34
VFB
4.99k
100
LDO Linear Regulators Rival
Switchers for Efficiency .............. 31
Jon Munson
30.1k
PGND
only 35mΩ on-resistance, allow the
LTC3418 to reduce component count
while achieving high efficiency. Operating at switching frequencies as high
as 4MHz conserves additional space by
permitting the use of smaller inductors
and capacitors. The LTC3418’s ability
to track another voltage supply also
allows it to be used in dual-supply
systems that require power supply
sequencing during start-up.
The LTC3418 employs a constant
frequency, current-mode architecture
Jesus Rosales
Instrumentation Amplifier with
Clock-Tunable Sampling Eliminates
Errors in Acquisition Systems ..... 33
RT
VOUT
1.2V
COUT 8A
100µF
×3
Figure 1. A 1.2V, 8A step-down regulator running at 2MHz,
which allows the use of tiny capacitors and inductors. This
particular configuration operates at a single frequency in
forced continuous mode, which simplifies EMI filtering.
Rich Philpott
900mA Li-Ion Charger in
2mm × 2mm DFN is Thermally
Regulated for Faster Charge Time
.................................................... 27
SYNC/MODE
CIN: AVX 12106D10MAT
L1: COOPER FP3-R20
Michael Nootbaar
SH Lim
SW
47pF
Simple Converter Drives Luxeon
White LEDs from Batteries .......... 21
L1
0.2µH
PGOOD
RUN/SS
CIN
100µF
×4
Joey M. Esteves
Small DFN Electronic
Circuit Breaker
Eliminates Sense Resistor ........... 25
LTC3418
100k
that operates from an input voltage
range of 2.25V to 5.5V and provides an
adjustable output voltage from 0.8V to
5V while delivering up to 8A of output
current. The switching frequency can
be set between 300kHz and 4MHz by
an external resistor. The LTC3418 can
also be synchronized to an external
clock, where each switching cycle
begins at the falling edge of the external clock signal. Since output voltage
ripple is inversely proportional to the
switching frequency and the inductor
value, a designer can take advantage
of the LTC3418’s high switching
frequency to use smaller inductors
without compromising the output
voltage ripple. Lower inductor values
translate directly to smaller case sizes,
reducing the overall size of the system.
OPTI-LOOP® compensation allows the
transient response to be optimized
over a wide range of loads and output capacitors, including ceramics.
For increased thermal handling, the
LTC3418 is offered in a 5mm × 8mm
continued on page 38
Linear Technology Magazine • May 2005
DESIGN IDEAS
Simple Converter Drives Luxeon
White LEDs from Batteries by Michael Nootbaar
Introduction
current drive. Existing boost circuits
generally use voltage feedback switching converters with extra circuitry to
The high output 1W white LEDs from
Luxeon and Nichia provide illumination levels close to 12W incandescent
levels while dissipating only 1W and
lasting for 50,000 hours or more. These
devices promise enormous power savings and reduced maintenance cost
for many lamp applications. However,
these LEDs must be driven with a
constant current to maintain proper
brightness. The forward voltage drop
varies between 2.8V and 4.0V over
process and temperature extremes.
The circuit used to drive the LED must
compensate for this forward voltage
variation while maintaining constant
The LTC3490 provides a
simple solution for boosting
a single or dual cell battery
voltage to the necessary
LED forward voltage and
regulating the current
through the LED load.
sense output current rather than voltage. This results in complex circuits
with poor efficiency.
3
SW
Circuit Description
–
2
P BODY
CONTROL
+
VIN
CAP
GATE
CONTROL
AND
DRIVERS
SENSE
AMP
LIMIT
19.2Ω
0.1Ω
LED
5
250k
–
OVERVOLTAGE
DETECT
6
+
–
PWM
LOGIC
The LTC3490 provides a simple
solution for boosting a single or dual
cell battery voltage to the necessary
LED forward voltage and regulating
the current through the LED load.
The high frequency (1.3MHz) operation
allows small inductor and capacitor
values. The current sensing resistor
and loop compensation components
are internal, reducing the component
count. The LTC3490 is a synchronous
converter eliminating the rectifier diode and its associated efficiency loss.
The only required components are the
boost inductor and an output filter
capacitor. The shutdown and dimming
functions add a few resistors, and an
input capacitor is recommended in
certain conditions.
40k
VREF/2
The LTC3490 is a synchronous boost
converter. Its block diagram is shown
in Figure 1. It will start up with input
voltage as low as 0.9V using a low voltage startup circuit. When the output
voltage exceeds 2.3V, the boost circuits
turn on and the startup circuit shuts
off. The boost converter is a fixed frequency, current mode architecture.
The LED current is sensed with an
internal 0.1Ω resistor on the high side,
which allows the LED cathode to be
grounded. A sense amplifier compares
this voltage to a reference current flowing through a ratiometrically matched
19.2Ω resistor. The sensed voltage dif-
+
OSCILLATOR
100
START-UP
DIMMING
AMP
+
LOBAT
IREF
1
BATTERY
MONITOR
CELLS
GND
4
Figure 1. LTC3490 block diagram
Linear Technology Magazine • May 2005
SHUTDOWN
7
EFFICIENCY (%)
8
CTRL/
SHDN
360
80
320
70
280
EFFICIENCY
60
240
50
200
40
160
30
120
20
80
10
40
0
1
1.5
2
VIN (V)
2.5
3
LED CURRENT (mA)
–
400
LED CURRENT
90
0
Figure 2. LTC3490 efficiency
21
DESIGN IDEAS
ference is integrated and used to set
the PWM controller. The LED current
is therefore constant regardless of the
LED forward voltage.
The LTC3490 is up to 90% efficient
in dual cell applications and over 70%
in single cell applications (Figure 2).
The dual cell and single cell circuits
are shown in Figures 3 and 4, respectively.
L1
3.3µH
ON/OFF
2 NiMH OR
ALKALINE
CELLS
VIN
SW
CAP
+
LTC3490
+
CELLS
1M
LOBAT
LUMILEDS
LUXEON
LXHL-BW02
GND
L1: TYCO DN4835-3R3M
COUT: TDK C2012X5R0J475K
Overvoltage Protection
Output overvoltage protection is required because the current sensing
controller can drive the output voltage
to damaging levels if there is no load.
This occurs if the LED is removed from
the circuit or has failed. As long as the
output current is below 350mA, the
output voltage continues to climb and
would damage the LTC3490 without
overvoltage protection. The overvoltage
detector forces the LTC3490 into
shutdown when the output voltage
is greater than 4.5V. The overvoltage
detector remains on and will restore
normal operation when the output
drops below 4.5V.
COUT
4.7F
CTRL/SHDN LED
Figure 3. Minimum component 2-cell circuit
L1
3.3µH
ON/OFF
1 NiMH OR
ALKALINE
CELL
VIN
SW
CAP
+
LTC3490
COUT
4.7F
CTRL/SHDN LED
CELLS
1M
LOBAT
LUMILEDS
LUXEON
LXHL-BW02
GND
L1: TDK SLF7045T-3R3M2R5
COUT: TDK C2012X5R0J475K
Figure 4. Minimum component 1-cell circuit
Dimming Function
The LTC3490 allows the LED current
to be gradually reduced using the
CTRL/SHDN pin. The CTRL/SHDN
input has three functions: shutdown,
dimming control and constant current
output. The pin is ratiometric to VIN,
which allows simple resistor dividers for setting current values. When
CTRL/SHDN is below 0.2 • VIN, the
part is in shutdown and draws minimal
current. When CTRL/SHDN is greater
than 0.9 • VIN, the part is in constant
350mA mode. When CTRL/SHDN is
between 0.2 • VIN and 0.9 • VIN, the
LED current varies linearly between
0mA and 350mA.
cell operation, respectively. When the
battery voltage drops below the detection level, an open drain output on the
LOBAT pin is pulled low. This output
can be used to drive an indicator or
can be fed back to the CTRL/SHDN
pin to lower the LED current to extend
remaining battery time.
There is also an undervoltage lockout, which shuts down the LTC3490
when the battery voltage drops below
0.8V/cell. This prevents excessive
battery current (single cell) and cell
reversal in unevenly discharged NiMH
cells (dual cell).
Low Battery Detection
Batteries have a phenomenon called
discharge recovery. When a load is
removed from a nearly discharged
battery, the terminal voltage recovers
to surprisingly high voltages. Thus
when a nearly discharged battery trips
the LTC3490 dead battery shutdown,
the reduction in current draw allows
the battery to recover. This turns the
The LTC3490 provides two levels of
low battery detection. These levels
are set by the CELLS pin, indicating
the number of battery cells. The low
battery detection is set at 1.0V when
the CELLS pin is low, and at 2.0V
when the CELLS pin is tied to VIN. This
corresponds to single cell and dual
22
Battery Reality Check
LTC3490 back on, putting the load
back on the battery. The battery voltage
drops, triggering shutdown again. This
phenomenon causes LTC3490 to turn
the LED current on and off rapidly. The
observed effect is that the average LED
current slowly drops as the battery
nears the end of its charge.
Conclusion
The LTC3490 provides a simple solution to driving the high output white
LEDs from alkaline or NiMH batteries.
It offers high efficiency with a low parts
count.
For further information on any
of the devices mentioned in this
issue of Linear Technology, use
the reader service card or call the
LTC literature service number:
1-800-4-LINEAR
Ask for the pertinent data sheets
and Application Notes.
Linear Technology Magazine • May 2005
DESIGN IDEAS
Monolithic Step-Down Regulator
Withstands Rigors of Automotive
Environments and Consumes Only
100µA of Quiescent Current by Rich Philpott
Introduction
Automobile electronic systems place
high demands on today’s DC/DC
converters. They must be able to
precisely regulate an output voltage
in the face of wide temperature and
input voltage ranges—including load
dump transients in excess of 60V, and
cold crank drops to 4V. The converter
must also be able to minimize battery
drain in always-on systems by maintaining high efficiency over a broad
load current range. Similar demands
are made by many 48V nonisolated
telecom applications, 40V FireWire
peripherals, and battery-powered applications with auto plug adaptors. The
LT3437’s best in class performance
meets all of these requirements in
a small thermally enhanced 3mm ×
3mm DFN package.
Features of the LT3437
The LT3437 is a 200kHz fixed frequency, 500mA monolithic buck
switching regulator. Its 3.3V-to-80V
input voltage range makes the LT3437
ideal for harsh automotive environments. Micropower bias current and
Burst Mode operation help to maintain high efficiency over the entire
load range and result in a no load
quiescent current of 100µA for the
VIN
3.3V TO 80V*
2.2µF
100V
CER
VIN
BOOST
SHDN
LT3437
VC
1500pF
330pF
SW
0.1µF
0.1µF
10MQ100N
CSS
VBIAS
165k
27pF
24k
SYNC
100µH BAS21
VOUT
3.3V
250mA
FB
100k
GND
100µF
6.3V
TANT
* FOR INPUT VOLTAGES ABOVE 60V SOME RESTRICTIONS MAY APPLY.
SEE ABSOLUTE MAXIMUM RATINGS IN DATA SHEET.
Figure 1. 14V to 3.3V step-down converter with 100µA no load quiescent current
circuit in Figure 1. The LT3437 has an
undervoltage lockout and a shutdown
pin with an accurate threshold for a
<1µA shutdown mode.
External synchronization can be
implemented by driving the SYNC pin
with a logic-level input. The SYNC pin
also doubles as burst mode defeat for
applications where lower output ripple
is desired over light load efficiency. A
single capacitor provides soft-start
capability which limits inrush current
and output voltage overshoot during
startup and recovery from brown-out
situations. The LT3437 is available in
either a low profile 3mm × 3mm 10-pin
DFN or 16-pin TSSOP package both
with an exposed pad leadframe for low
thermal resistance.
Brutal Input Transients
Figure 2 shows the LT3437’s reaction to the lethal input transients
that are possible in an automotive
environment. Here, the input voltage
rises from a nominal 12V to 72V in a
100ms load dump pulse, then drops to
4V in a 150ms cold crank pulse. The
200kHz fixed frequency and current
mode topology of the LT3437 allow it
to take it all in stride—response to the
input transients are less than 1% of
the regulated voltage. The fuzziness
seen on the output voltage is due
to the ESR of the output capacitor
and the change in inductor current
ripple as the input voltage transitions
between levels. The fuzziness can be
200
180
LOAD DUMP
VIN
20V/DIV
COLD CRANK
0V
140
120
100
80
60
40
20
VOUT
20mV/DIV
AC COUPLED
0
50ms/DIV
Figure 2. Output voltage response to load dump and cold crank input transients
Linear Technology Magazine • May 2005
SUPPLY CURRENT (µA)
160
1
10
20
30 40 50 60
iNPUT VOLTAGE (V)
70
80
Figure 3. Supply current vs input
voltage for circuit in Figure 1
23
DESIGN IDEAS
500
90
450
EFFICIENCY (%)
80
200mA
IOUT
100mA/DIV
0mA
1ms/DIV
eliminated by changing the output
capacitor type from tantalum to a
more costly ceramic.
Low Quiescent Currents
Today’s automotive applications are
migrating to always-on systems,
which require low average quiescent
current to prolong battery life. Loads
are switched off or reduced during
low demand periods, then activated
for short periods. Quiescent current
for the application circuit in Figure 1
is less than 1µA in shutdown mode,
and a mere 100µA (Figure 3) for an
input voltage of 12V under a no load
condition. The LT3437 provides excellent step response from a no-load to
load situation as shown in Figure 4.
Automatic Burst Mode operation ensures efficiency over the entire load
range as seen in Figure 5. Burst Mode
operation can be defeated or enabled
on the fly if lower ripple is desired over
light load efficiency.
Soft-Start Capability
The rising slope of the output voltage
is determined by the output voltage
and a single capacitor. Initially, when
the output voltage is close to zero,
the slope of the output is determined
by the soft-start capacitor. As the
output voltage increases, the slope is
increased to full bandwidth near the
regulated voltage. Since the circuit
is always active, inrush current and
voltage overshoot are minimized for
startup and recovery from overload
(brown-out) conditions. Figure 6 il-
350
60
300
50
250
40
200
POWER LOSS
30
150
20
100
10
50
0
Figure 4. Output voltage response for 0mA-to-200mA load step
400
EFFICIENCY
70
0.1
1
100
10
LOAD CURRENT (mA)
1k
POWER LOSS (mW)
VOUT
50mV/DIV
100
0
Figure 5. Efficiency vs load current
for the circuit in Figure 1
lustrates the effect of several soft-start
capacitor values.
Conclusion
The LT3437’s wide input range, low
quiescent current, robust design, and
available small thermally enhanced
packages make it an ideal solution for
all automotive and wide input voltage,
low quiescent current solutions.
CSS = GND
CSS = 0.1µF
CSS = 0.01µF
VOUT
1V/DIV
COUT = 100µF
ILOAD = 200mA
VIN = 12V
1ms/DIV
Figure 6. Output voltage soft-start
LTC3442, continued from page 10
pulse input for a flash application. The
entire solution is only 2mm high.
This circuit also features overvoltage
protection, preventing excessive output voltage in the event that the
current path to the LED becomes
open-circuited. By connecting the
RLIM pin to a resistive divider on VOUT,
the RLIM input acts as an overvoltage
comparator with a 1.0V reference.
Raising RLIM above 1.0V pulls down
on the VC pin, limiting the output
voltage. By making the value of the
divider resistors relatively small, the
current sourced by the input current
24
mirror to RLIM has a negligible effect
on the overvoltage threshold.
Conclusion
Linear Technology’s LTC3442 synchronous buck-boost converter, with
automatic Burst Mode operation and
programmable input current limit,
simplifies the system power design
in a wide variety of applications. The
buck-boost architecture and 100mΩ
internal switches provide a robust,
high efficiency solution with high
current capability, while the automatic Burst Mode feature maximizes
runtime in portable Li-Ion powered
devices with widely varying load requirements. Programmable soft-start
and switching frequency, as well as
external compensation, make the
LTC3442 a very flexible solution. The
high level of integration in a 3mm ×
4mm DFN package, and the ability to
operate efficiently at over 1MHz using
low profile inductors and all ceramic
capacitors, helps the designer save
precious board real estate and meet
the stringent height requirements of
today’s miniature, portable applications.
Linear Technology Magazine • May 2005
DESIGN IDEAS
Small DFN Electronic Circuit Breaker
by SH Lim
Eliminates Sense Resistor
Introduction
Traditionally, an Electronic Circuit
Breaker (ECB) comprises a MOSFET,
a MOSFET controller and a current
sense resistor. The LTC4213 is a new
electronic circuit breaker that does
away with the sense resistor by instead using the RDS(ON) of the external
MOSFET. The result is a simple, small
solution that offers significant low insertion loss advantage at low operating
load voltage. The LTC4213 features
two circuit breaking responses to
varying over load conditions with three
selectable trip thresholds and a high
side drive for an external N-channel
MOSFET switch.
Overcurrent Protection
The SENSEP and SENSEN pins monitor the load current via the RDS(ON) of
the external MOSFET, and serve as
inputs to two internal comparators—
SLOWCOMP and FASTCOMP—with
trip points at VCB and VCB(FAST), respectively. The circuit breaker trips
when an over-current fault causes a
substantial voltage drop across the
MOSFET. An overload current exceeding VCB/RDS(ON) causes SLOWCOMP to
trip the circuit breaker after a 16µs
delay. In the event of a severe overload
or short circuit current exceeding
VCB(FAST)/RDS(ON), the FASTCOMP trips
the circuit breaker within 1µs, protecting both the MOSFET and the load.
When the circuit breaker trips, the
GATE pin is pulled down immediately
to disconnect the load from the supply.
In order to reset the circuit breaker
fault, either the ON pin must be taken
below 0.4V for at least 80µs or the bias
VCC must be taken below 1.97V for at
least 80µs. Both of the comparators
have a common mode input voltage
range from ground to VCC + 0.2V. This
allows the circuit breaker to operate
even under severe output short circuit
conditions where the load supply voltage collapses.
Q1
SI4864DY
VIN
1.25V
CIN
220µF
+
VBIAS
3.3V
CLOAD
220µF
C1
0.1µF
OFF ON
LTC4213
ON
GND
ISEL
VOUT
1.25V
3.5A
VCC
R4
10k
READY
Figure 1. The LTC4213 in an electronic circuit breaker application
Flexible Overcurrent Setting
The LTC4213 has an ISEL pin to select one of these three over-current
settings:
❑ ISEL at GND, VCB = 25mV and
VCB(FAST) = 100mV
❑ ISEL left open, VCB = 50mV and
VCB(FAST) = 175mV
❑ ISEL at VCC, VCB = 100mV and
VCB(FAST) = 325mV
ISEL can be stepped dynamically.
For example, a higher over-current
threshold can be set at startup and a
lower threshold can be selected after
the supply current has stabilized.
Overvoltage Protection
The LTC4213 can provide load
overvoltage protection (OVP) above
the bias supply. When VSENSEP > VCC +
0.7V for 65µs, an internal OVP circuit
activates with the GATE pin pulling low
and the external MOSFET turning off.
The OVP circuit protects the system
(1)
VON
1V/DIV
(2)
VGATE
5V/DIV
(3)
VREADY
2V/DIV
(4)
VOUT ≈ VIN
1V/DIV
VIN POWERS UP
0.1ms/DIV
Figure 2. Normal power-up sequence
Linear Technology Magazine • May 2005
VCC SENSEP GATE SENSEN
+
from an incorrect plug-in event where
the VIN load supply is much higher than
the VCC bias voltage. The OVP circuit
also cuts off the load from the supply
during any prolonged over voltage
conditions. The 65µs delay prevents
the OVP circuit from triggering due
fast transient noise. Nevertheless, if
fast over voltage spikes are threats to
the system, an external input bypass
capacitor and/or transient suppressor
should be installed.
Typical Electronic Circuit
Breaker (ECB) Application
Figure 1 shows the LTC4213 in a dual
supply ECB application. An input
bypass capacitor is recommended to
prevent transient spikes when the
VIN supply powers-up or the ECB
responds to overcurrent conditions.
Figure 2 shows a normal power-up
sequence. The LTC4213 exits reset
mode once the VCC pin is above the internal under voltage lockout threshold
and the ON pin rises above 0.8V (see
trace 1 in Figure 2). After an internal
60µs de-bounce cycle, the GATE pin
capacitance is charged up from ground
by an internal 100µA current source
(see trace 2). As the GATE pin and
the gate of MOSFET charges up, the
external MOSFET turns on when VGATE
exceeds the MOSFET’s threshold. The
circuit breaker is armed when VGATE
exceeds ΔVGSARM, a voltage at which
the external MOSFET is deemed fully
enhanced, and RDS(ON) minimized.
25
DESIGN IDEAS
VIN
STAGGERED
PCB EDGE
CONNECTOR
VIN
3.3V
SHORT
R3
182k
Zx
SMAJ6.0A
D1
BAT54ALT1
RESET
LONG
ON
R1
68
R2
80.6k
C1
2.2µF
LONG
BACKPLANE GND
R5
330
Q1
IRF7455
SENSEP GATE
C2
1µF
+
CLOAD
100µF
SENSEN
R4
10k
LTC4213
VCC
VOUT
3.3V
3.6A
READY
ISEL
GND
NC
CARD GND
Figure 3. The LTC4213 in a Hot Swap application
Then, 50µs after the circuit breaker is
armed and the READY pin goes high
(see trace 3), the VIN supply starts to
power-up. To prevent power-up failures, the VIN supply should rise with
a ramp-rate that keeps the inrush
current below the ECB trip level. Trace
4 shows the VOUT waveform during the
VIN supply power-up. The gate voltage
finally peaks at ΔVGSMAX + VSENSEN.
The MOSFET gate overdrive voltage
is ΔVGSMAX which is higher than the
ΔVGSARM. This ensures that the external MOSFET is fully enhanced and the
RDSON is further reduced. Choose the
MOSFET with the required RDSON at
VGS approximately equal to ΔVGSMAX.
The LTC4213 monitors the load current when the gate overdrive voltage
exceeds ΔVGSARM.
Typical Hot Swap Application
Figure 3 shows the LTC4213 in a single
supply Hot Swap application where the
LTC4216, continued from page 19
low by an internal N-channel device
and CAUTO is discharged to ground.
The GATE pin is pulled immediately
to ground to disconnect the board.
When the ON pin goes below 0.4V for
more than 100µs, the ECB is reset.
The internal N-channel device at the
FAULT pin is switched off and RAUTO
starts to charge CAUTO slowly towards
the load supply.
When the ON pin rises above 0.8V,
the LTC4216 attempts to reconnect the
board and start the first timing cycle.
26
load can be kept in shutdown mode
until the Hot Swap action is completed.
Large input bypass capacitors should
be avoided in Hot Swap applications
as they cause large inrush currents.
Instead, a transient voltage suppressor
should be employed to clip and protect
against fast transient spikes.
In this application, the backplane
starts with the RESET signal held
low. When the PCB long trace makes
contact the ON pin is held below 0.4V
by the D1 schottky diode. This keeps
the LTC4213 in reset mode. The VIN
supply is connected to the card when
the short trace makes contact. The VCC
pin is biased via the R1-C1 filter and
VOUT is pre-charged by resistor R5. To
power-up successfully, the R5 resistor
should provide sufficient initial start
up current for the shutdown load
circuit and the 280µA sinking current
source at SENSEN pin. On the other
hand, the R5 resistor value should
limit the load surge current during
board insertions and fault conditions.
When RESET signals a high at the
backplane, capacitor C2 at the ON
pin charges up via the R3/R2 resistive
divider. When ON pin voltage exceeds
0.8V, the GATE pin ramps up. The
GATE voltage finally peaks and the
external MOSFET is fully turned on
to reduce the voltage drop between VIN
and VOUT. The LTC4213 monitors the
load current when the gate overdrive
voltage exceeds ΔVGSARM.
With a dead short at the 5V output
in Figure 6, the ECB trips when the
FILTER pin voltage exceeds 1.253V
after the first timing cycle. The entire
cycle is repeated until the short is
removed. The duration of each cycle
is given by the time needed to charge
CAUTO to within 0.8V of the ON pin
voltage, after the FAULT pin is pulled
low and the first timing cycle delay.
With RAUTO = 200kΩ, CAUTO = 1µF and
C1 = 100nF, the cycle time is 85ms.
The external MOSFET is on for about
2ms giving a duty cycle of 2.3%.
Conclusion
Conclusion
The LTC4213 is a small package, No
RSENSE Electronic Circuit Breaker that
is ideally suited for low voltage applications with low MOSFET insertion loss.
It includes selectable dual current level
and dual response time circuit breaker
functions. The circuit breaker has wide
operating input common-mode-range
from ground to VCC.
The LTC4216 Hot Swap controller is
designed to handle very low supply
voltages, down to 0V. Its adjustable
soft-start function controls the inrush
current slew rate at start-up, important with the large load capacitors used
in low voltage systems. The analog
current limit amplifier, the electronic
circuit breaker with low trip threshold of 25mV and adjustable response
time provides dual level overcurrent
protection.
Linear Technology Magazine • May 2005
DESIGN IDEAS
900mA Li-Ion Charger in 2mm × 2mm
DFN is Thermally Regulated for
by David Kim
Faster Charge Time
Introduction
It can be tough to design a high performance linear Li-Ion battery charger
for cell phones, MP3 players and other
portable devices. The overriding design
problem is how to squeeze the charger
onto ever-shrinking boards, while
managing the heat inherently generated by the charge process. The typical
solution is to lower the maximum
charge current to a sub-optimal value
to avoid overheating, thus increasing
charge time.
The LTC4059 is designed to shorten
charge time even while squeezing
the charger into the smallest spaces.
The LTC4059 is a 2mm × 2mm DFN
package constant-current/constant
voltage Li-Ion linear charger with a
built-in 900mA MOSFET, accurate
charge current monitor output and
thermal regulation control. Thermal
regulation in this device is different,
and much better, than the thermal
shutdown found in most chargers.
Thermal feedback control allows a designer to maximize the charge current,
and thus decrease charge time without
the risk of damaging the LTC4059 or
any other components. Figure1 shows
a typical application.
Figure 2 shows a complete 2.5mm
x 2.7mm charging circuit that includes the LTC4059 and two passive
700
4.4
CONSTANT
VOLTAGE
4.2
500
4.0
400
3.8
300
3.6
200
3.4
VCC = 5V
100
RPROG = 2k
TA = 25°C
0
0.5
0
BATTERY VOLTAGE (V)
CHARGE CURRENT (mA)
600
CONSTANT
CURRENT
VDD
VIN
4.5V TO 8V
50k
VCC
LTC4059A
1µF
EN
GND
µP
ACPR
600mA
BAT
PROG
2k
+
4.2V
Li-Ion
BATTERY
Figure 1. Simple and tiny Li-Ion battery
charger offers thermal regulation for
improved charge time.
components. The internal MOSFET
architecture requires no blocking
diode or external sense resistor.
In addition to its miniscule size, the
LTC4059 includes other important
features for the latest cellular phones,
wireless headsets, digital cameras,
wireless PDAs and MP3 players. Supply current in shutdown mode is very
low—10µA from the input supply, and
under 1µA from the battery when the
input supply is removed. It also has the
capability of charging single cell Li-Ion
batteries directly from a USB port.
Constant Current/
Constant Voltage/
Constant Temperature
The LTC4059 uses a unique architecture to charge a battery in a
constant-current, constant-voltage
or constant temperature fashion. In
a typical operation, to charge a single
cell Li-Ion battery, the user must apply
an input voltage of at least 4.5V to the
5V WALL
ADAPTER
850mA ICHG
USB
POWER
500mA ICHG
1.5
2
3.0
2.5
Vcc pin along with a 1% resistor connected from PROG to GND (using the
formula RPROG = 1000 • 1.21V/ICHG)
and EN pin under 0.92V. When all
three conditions are met, the charge
cycle begins in constant-current mode
with the current delivered to the battery equal to 1210V/RPROG.
If the power dissipation of the
LTC4059 and/or high ambient temperature results in the device junction
temperature rising to near 115°C,
the part enters constant temperature
mode and the thermal feedback loop
of the LTC4059 decreases the charge
current to regulate the die temperature
to approximately 115 °C. This feature
allows the user to program a charge
current based on typical operating
conditions and eliminates the need for
the complicated thermal over-design
necessary in other linear chargers.
Typically, the thermal feedback loop
conditions are temporary as the
ICHG
D1
MP1
3.2
1
Figure 2. Chargers do not get smaller
than this (2.5mm x 2.7mm).
1k
BAT
LTC4059
VCC
PROG
MN1 3.4k
+
SYSTEM
LOAD
Li-Ion
BATTERY
2.43k
TIME (HOURS)
Figure 3. Complete charge cycle
(800mAh Battery)
Linear Technology Magazine • May 2005
Figure 4. Charger that combines both wall adapter and USB power inputs
27
DESIGN IDEAS
battery voltage rises with its charge
(resulting in lower power dissipation
across the MOSFET) but it is the worst
case situation that one must account
for when determining the maximum
allowable values for charge current
and IC temperature.
Once the die temperature drops
below 115 °C, the LTC4059 returns to
constant-current mode straight from
constant temperature mode. As the
battery voltage approaches the 4.2V
float voltage, the part enters constantvoltage mode. In constant-voltage
mode LTC4059 begins to decrease the
charge current to maintain a constant
voltage at the BAT pin rather than a
constant current out of the BAT pin
(Figure 3).
Regardless of the mode, the voltage
at the PROG pin is proportional to
the current delivered to the battery.
During the constant current mode,
the PROG pin voltage is always 1.21V
indicating that the programmed charge
current is flowing out of the BAT pin.
In constant temperature mode or
constant voltage mode, the BAT pin
current is reduced. The charge current at any given charge cycle can be
determined by measuring the PROG
pin voltage using the formula ICHRG =
1000 • (1.21V/RPROG).
Using the battery voltage and the
PROG pin voltage information, the user
can determine the proper charge termination current level (typically 10%
of the full-scale programmed charge
current). Once the desired charge
current level is reached, the user can
terminate the charge cycle simply by
pulling up the EN pin above 1.2V.
LT6100, LTC6101, continued from page 7
high-side switch controls an N-channel MOSFET that drives a controlled
load, and uses a sense resistance
to provide overload detection (note
the surge-current of lamp filaments
may cause a protection trip, thus
are not recommended loads with the
LT1910). The sense resistor is shared
by the LT6101 to provide the current
measurement.
The LTC6101 supplies a current
output, rather than a voltage output, in
proportion to the sense resistor voltage
drop. The load resistor for the LTC6101
may be located at the far end of an
arbitrary length connection, thereby
sense resistor of 30mΩ gives set point
currents of 1A and 800mA.
Monitor the Current
of Automotive Load Switches
With its 60V input rating, the LTC6101
is ideally suited for directly monitoring
currents on vehicular power systems,
without need for additional supply
conditioning or surge protection
components.
Figure 12 shows an LT1910-based
intelligent automotive high-side switch
with an LTC6101 providing an analog current indication. The LT1910
28
Board Layout
Properly soldering the exposed metal
on the backside of the LTC4059
package is critical for minimizing the
thermal resistance. Properly soldered
LTC4059 on a 2500mm 2 double
sided 1oz copper board should have
a thermal resistance of approximately
60°C/W. When the LTC4059 is not
properly soldered (or does not have
enough copper), the thermal resistance rises, causing the LTC4059 to
enter constant-temperature mode
more often, thus resulting in longer
charge time. As an example, a correctly
soldered LTC4059 can deliver over
900mA to a battery from a 5V supply
at room temperature. Without a backside thermal connection, this number
could drop to less than 500mA.
Li  CC, ACPR
Two versions of the part are available,
depending on the needs of the battery
chemistry. The LTC4059 has a Li CC
pin, which disables constant-voltage
operation when it is pulled up above
0.92V. In this mode, the LTC4059
turns into a precision current source
capable of charging Nickel chemistry
batteries. In the LTC4059A, the Li CC
pin is replaced by an ACPR pin, which
monitors the status of the input voltage
with an open-drain output. When Vcc
is greater than 3V and 150mV above
the BAT pin voltage, the ACPR pin will
pull to ground; other wise the pin is
forced to a high impedance state.
Combining
Wall Adapter and USB Power
Figure 4 shows an example of combining wall adapter and USB power
inputs. In this circuit, MP1 is used to
prevent back conduction into the USB
port when a wall adapter is present
and D1 is used to prevent USB power
loss through the 1K pull-down resistor. The 2.43k resistor sets the charge
current to 500mA when the USB port
is used as input and the MN1 and
3.4k resistor is used to increase the
charge current to 850mA when the
wall adapter is present.
Conclusion
The LTC4059 is industry’s smallest
single cell Li-Ion battery charger capable of up to 900mA charge current. The
thermal regulation feature of LTC4059
allows the designer to maximize the
charge current and shorten the charge
time without the risk of damaging the
circuit. The small circuit size, thermal
protection, low supply current and
low external component count make
LTC4059 an ideal solution for small
portable and USB devices.
preserving accuracy even in the presence of ground-loop voltages.
Conclusion
The LT6100 and LTC6101 are precise
high side current sensing solutions.
Although very similar in obvious
respects, each has its unique advantages. The LT6100 draws much less
power, can be powered down while
maintaining high Z characteristics,
and has nearly indestructible inputs.
The LTC6101 can withstand up to 70V,
is infinitely gain configurable, and
provides an open drain output.
Linear Technology Magazine • May 2005
DESIGN IDEAS
600mA Switching Converter Reduces
Noise by Automatically Shifting to a
Linear Regulator at Light Loads
by Kevin Soch
Introduction
Figure 1. The LTC3448 regulator occupies
less than 0.1in2 of board space.
current, and enters linear regulator
operation when appropriate. The
crossover between switcher mode
and linear regulator mode can also
be controlled externally by driving the
MODE pin high or low.
The LTC3448 has a 2.5V to 5.5V
input voltage range, perfect for single
VIN
2.5V TO 5.5V
Linear Technology Magazine • May 2005
continued on page 32
SW
VOUT
RUN
LTC3448
MODE
CIN
4.7µF
22pF
VFB
FREQ
SYNC
GND
Features
474k
COUT
4.7µF
VOUT
1.5V
316k
Figure 2. LTC3448 minimum component implementation.
1k
6
90
80
100
70
EFFICIENCY
60
10
50
POWER LOSS
40
30
1
20
VIN = 3.6V
VOUT = 1.5V
10
0
0.1
1
10
100
LOAD CURRENT (mA)
1k
0.1
Figure 3. Overall efficiency and power loss as
a function of load current. Part is operating
in automatic linear regulator mode with VIN =
3.6V and VOUT = 1.5V.
LOAD TRANSITION CURRENT (mA)
100
EFFICIENCY (%)
The LTC3448 automatically shifts
gears to maintain high efficiency and
low noise over a wide range of load
currents. For normal loads, it operates
as a current mode constant frequency
converter, which yields well-defined
ripple frequencies. At moderate load
currents, it transitions into pulse
skipping mode for decreased output
ripple. At load currents below 3mA, it
automatically shifts to linear regulator
operation to maintain <5mVP–P noise
and reduce the quiescent supply current to 32µA.
No external sense resistor is required to detect the load current.
Simply tie the MODE pin to VOUT.
The LTC3448 uses a patent pending
process where it monitors the behavior
of the switcher to determine the load
Li-Ion battery-powered applications,
and is available with an adjustable output voltage. Its 100% duty
cycle provides low dropout operation,
extending battery life in portable systems. Low output voltages are easily
supported with the 0.6V feedback
reference voltage.
Switching frequency is selectable
at either 1.5MHz or 2.25MHz, or can
be synchronized to an external clock
applied to the SYNC pin. The high
switching frequency allows the use
of small surface mount inductors and
capacitors. The LTC3448 also saves
space with an internal synchronous
switch, which eliminates the need
for an external Schottky diode and
increases efficiency.
2.2µH
VIN
POWER LOSS (mW)
High efficiency, low ripple current, and
a small footprint are critical power
supply design requirements for cell
phones, MP3 players and other portable devices. The LTC3448 delivers
excellent performance in each of these
areas. It is a high efficiency, monolithic, synchronous buck regulator
using a constant frequency, current
mode architecture. It achieves very
low ripple by automatically shifting to
linear regulator operation at load currents below 3mA, and pulse skipping
operation at moderate load currents.
This is a critical feature in applications such as cell phones, where low
power supply noise is required while
in standby. Its built-in 0.35Ω switches
provide for up to 96% efficiency. Finally, it fits into 0.1in2 (see Figure 1)
due to its 8-lead 3mm × 3mm DFN or
MSOP package, 1.5MHz or 2.25MHz
switching frequency, internal compensation, and minimum number of
small external components.
5
4
3
2
1
0
VIN = 3.6V
VOUT = 1.5V
0
2
8
4
6
INDUCTOR VALUE (µH)
10
12
Figure 4. Switching-to-linear-regulator
crossover load current depends on
inductor value. VIN = 3.6V, VOUT = 1.5V.
29
DESIGN IDEAS
Single Converter Provides Positive
by Jesus Rosales
and Negative Supplies
VIN
2.7V TO 4.2V
LP
22µH
VOUT1
15V
IOUT(P)*
SWP
VPOS
RFBP
549k
CFBP, 4.7pF
CIN
2.2µF
10V
CNF
1µF
LN1
47µH
VIN
SWN
DN
LT3472
FBP
FBN
SHDN
SHDN
SSP
COUT(P)
4.7µF
16V
GND
SSN
CSSP
0.22µF
*OUTPUT CURRENT
VIN
IOUT(P) IOUT(N)
4.2V
45mA
65mA
3.3V
35mA
50mA
2.7V
25mA
35mA
CIN:
COUT(P):
CNF:
COUT(N):
LP:
LN1, LN2:
RFBN
324k
CFBN
10pF
LN2
47µH
VOUT2
–8V
IOUT(N)*
COUT(N)
2.2µF
16V
CSSN
0.22µF
AVX 0805ZD225KA T2A
TAIYO YUDEN EMK316BJ475ML
TAIYO YUDEN EMK212BJ105
TDK C2012X7R1C225K
MURATA LQH32CN220K53
MURATA LQH32CN470K53
Figure 1. A 1.1MHz, 2.7V–4.2V to 15V, 25mA and –8V, 35mA converter/inverter.
to set its output voltage. The LT3472
works well with input voltages as high
as 16V. The LT3472 also includes an
output sequencing feature which allows the negative supply to ramp up
only after the positive one has reached
88% of its final value, providing for a
controlled turn on as demonstrated in
Figure 2. In situations where inrush
current is a problem, the LT3472 offers a capacitor-programmable soft
start feature that allows the designer
to individually program the ramp rate
of each output. This feature allows the
designer to reduce inrush current to
any arbitrary level. Figure 3 shows the
supply efficiency.
80
VIN = 4.2V
75
EFFICIENCY (%)
Charge coupled device (CCD) imagers,
LCDs, some op amps and many other
circuits require both a positive and
negative power supply. Typically, two
DC/DC converters are used—one for
the positive supply and the other for
the negative—but the additional ICs
and related circuitry add cost and
complexity. There are single converter
topologies that develop plus/minus
supplies, but usually the second
output suffers from poor regulation.
In addition, in order to produce a
second output of different amplitude,
odd transformer turns ratios or post
regulators become necessary, which
also increases cost, complexity and
efficiency losses.
The LT3472 dual DC/DC converter
simplifies the design of dual, positive
and negative, supplies by combining
two switchers that have independent
control loops and ±34V output ranges.
Figure 1 shows a circuit using the
LT3472 that produces two independently regulated power supplies from
a single Lithium-ion cell: a 15V, 25mA
supply, and a –8V, 35mA supply. A
useful application for this could be for
amplifier circuits which need to output
true zero volts with only a single positive supply available. A low current
negative supply and boosted positive
supply rail permits full amplifier output swing from 0V to VBATTERY.
The Schottky rectifying diodes are
integrated into the LT3472, which
shrinks and simplifies the solution.
Each supply requires only one resistor
VIN = 2.7V
70
VIN = 3.3V
65
60
0
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9
OUTPUT POWER (W)
1
Figure 3. Efficiency for both outputs
loaded at 10% load increments
VOUT1
5V/DIV
0V
0V
VOUT2
5V/DIV
5ms/DIV
Figure 2. Start up sequence
30
Figure 4. The compact layout of a
dual output converter/inverter
Linear Technology Magazine • May 2005
DESIGN IDEAS
LDO Linear Regulators
Rival Switchers for Efficiency
Introduction
Thermal Limitations
While efficiency is always quoted as a
benchmark for switching regulators,
power loss is often more important.
Power loss sets the size of the heat sink,
and the size of the heat sink is—more
than any other component—directly
related to the size of the board.
Linear regulators are about simplicity, so their advantages are clearest
in designs where no more than the
multi-layer circuit board is needed
to provide heat sinking. To a first ap-
2.5
that satisfies the requirements of most
industrial applications.
The amount of output current
that the linear regulator can deliver
depends on the input-to-output differential voltage and the power loss
limitations. For instance, in a 2.5Vto-1.5V design, the 1V differential
voltage allows for 1A of load current to
meet the 1W dissipation requirement
(see Figure 1). If the differential voltage is only 0.7V, as in a 2.5V-to-1.8V
regulator, the maximum load current
increases to over 1.4A.
Figure 1 shows that there is a wide
range of power combinations that can
be filled under these circumstances.
In surface mount designs, power loss
correlates directly to board area as
power is usually dissipated through
the metal layers. With this in mind,
Figure 1 covers a range of linear regulator applications that compare well
with switching regulators—which are
very efficient at high input-to-output
differential voltages, but rarely have
better than 75%–80% efficiency at low
input-to-output differential voltages.
For instance, consider a low dropout regulator regulating 1.8V-to-1.2V
at one amp. With an input-to-output
differential of 0.6V, the maximum
amount of output current available
increases to over 1.5A, at one watt
of power dissipation (see Figure 1).
2
VIN – VOUT (V)
Switching power supplies owe much of
their popularity to their efficiency, even
when the distinction is not necessarily deserved. For instance, when low
voltage input supplies are available,
and currents are around an amp or
so, a less complex low dropout linear
regulator can match the efficiency of
a switcher. Furthermore, if the design
is limited to all surface mount applications, with heat sinking provided by the
board, a linear regulator can provide
switcher-like efficiency over a fairly
wide range of input voltages.
For example, a linear regulator
provides excellent efficiency in a
1.8V-to-1.2V application. Even at 2A
of output current, only 1.2W of power
is dissipated. This is sufficiently low
enough for a multi-layer board to
provide adequate heat sinking.
POWER DISSIPATION = 2W
1.5
POWER DISSIPATION = 1W
POWER DISSIPATION = 0.5W
1
0.5
0
0
1
2
3 4 5 6 7
LOAD CURRENT (A)
8
9
by Tom Gross
10
Figure 1. Various power dissipation limits
shown as a function of load current and
input-to-output differential voltage.
proximation, a multi layer board can
dissipate power at 40°C per watt. If we
want to limit the regulator maximum
At low input and output
voltages, linear regulators
offer excellent regulation,
and in many cases, deliver
efficiency rivaling that of
switching regulators. In all
cases a linear regulator
circuit is simpler and less
costly.
temperature to 125°C, 1W of dissipation allows an ambient temperature
of 85°C. An ambient temperature of
85°C is a conservative design number
VBIAS = 5V
1µF
LTC3026
VIN = 1.8V
VIN
1.8V
BST
SW
IN
OUT
SHDN
ADJ
VOUT
1.5V
11k
4.02k
1µF
GND
PG
a.
COUT
10µF
Ceramic
2.2µH
4.7µF
CER
SW
VIN
SWITCHER
22pF
RUN
MODE
VFB
301k
SYNC
10µF
CER
VOUT
1.5V
432k
GND
b.
Figure 2. Two 1.5V output DC/DC converters. The first (a) is a typical linear regulator using the LTC3026 with an external
bias supply. The second (b) is a typical 1.5V switching regulator application. In circuit (a), if an external bias supply is not
present, the LTC3026 can generate its own bias with an internal boost converter and an external inductor (10 µH, 150mA).
Linear Technology Magazine • May 2005
31
DESIGN IDEAS
Compare the two different topologies
in a 1.8-to-1.5 volt application. In
this design, the power dissipation is
low enough that even three amps of
output current do not exceed our 1W
power limitation. Figure 2a shows a
1.5A application using the LTC3026
CMOS linear regulator. A comparable
step-down switching regulator circuit is shown in Figure 2b. Figure 3
compares the efficiencies and power
losses of both circuits. As shown, the
switching converter is more efficient
at low load currents, but the linear
regulator efficiency matches, then
surpasses, the switcher efficiency as
the load current increases. The same
is true for the power losses. The linear
EFFICIENCY (%)
96
SWITCHER
EFFICIENCY
SWITCHER
POWER
LOSS
LDO
92
500
100
400
96
300
POWER
LOSS
200
84
LDO
EFFICIENCY
100
84
0
80
80
0
200
400
600
800
LOAD CURRENT (mA)
1k
Figure 2 shows a typical application
using a minimum number of external
components. The loop compensation
is integrated into the device, and the
optional 22pF feed-forward capacitor improves the transient response.
The switching frequency is 1.5MHz as
shown (FREQ pin to ground) but it can
be set to 2.25MHz by connecting the
FREQ pin to VIN. Figure 3 shows the
efficiency and power loss as a function
of load current.
By connecting the MODE pin to
VOUT, the part automatically transitions from a switching regulator to a
linear regulator at low load currents.
In the circuit of Figure 2, the transition occurs when the load current
drops below approximately 3mA. The
transition load value has an inverse
relationship to the inductor value, as
32
300
VIN = VOUT + VDROPOUT, VOUT = 1.5V
LDO
EFFICIENCY
92
88
SWITCHER
EFFICIENCY
88
240
SWITCHER
POWER
LOSS
180
120
LDO
POWER
LOSS
0
200
400
600
800
LOAD CURRENT (mA)
60
1k
0
Figure 3. Efficiency and power loss of the
LTC3026 linear regulator compare favorably
to that of a switching regulator. The LDO
maintains good efficiency to 1.5A.
Figure 4. At the lowest input-to-output
differential voltage, VIN = VOUT + VDROPOUT and
VOUT = 1.5V, the efficiency and power losses of
the linear regulator fare even better compared
to those of the switching regulator.
regulator fares better as load current
increases.
As the input-to-output differential
voltages decrease, such as occurs in
battery-powered applications, the linear regulator efficiency compares even
more favorably to the switcher (see
Figure 4). For instance, at 500mA of
load current, where the dropout voltage of the LTC3026 is only 60mV, the
linear regulator is over 97% efficient,
whereas the switcher efficiency is
around 85%. In this case, the linear
regulator beats the switcher in all
aspects—efficiency, power loss, size,
simplicity and cost.
LTC3448, continued from page 29
Minimum Component 1.5V
Step-Down Implementation
EFFICIENCY (%)
VIN = 1.8V
VOUT = 1.5V
POWER LOSS (mW)
Comparison of a Switcher
and Linear Regulator in
the Same Application
100
POWER LOSS (mW)
Increasing the maximum power dissipation to 2W, allows well over 3A
of output current. The efficiency of a
switching regulator operating under
these conditions is typically 75%. The
added complexity and cost of a switching regulator makes a linear regulator
look even better.
VOUT
10mV/DIV
A
Conclusion
At low input and output voltages, linear
regulators offer excellent regulation,
and in many cases, deliver efficiency
rivaling that of switching regulators.
In all cases a linear regulator circuit is
simpler and less costly. In applications
where the board can adequately dissipate the power, linear regulators can
handle a reasonable range of inputs
and output voltages.
C
B
D
ILOAD = 20mA
ILOAD
25mA/DIV
ILOAD = 1mA
100µs/DIV
Figure 5. The load transient response of the circuit in Figure 2. The transitions from linear
regulator behavior to switching behavior and back are shown. In the region labeled A, load
current is 1mA and the part is operating as a linear regulator. In the region labeled B, the load
current has increased to 20mA and the switcher has turned on in pulse skipping mode. In the
region labeled C, the load has decreased to 1mA, but the part has not yet transitioned back into
linear regulator operation, thus the lower frequency pulse skipping behavior. In region D, the part
is again operating as a linear regulator, with greatly reduced output noise.
shown in Figure 4, but is independent
of other external component values,
and largely independent of the values
of VIN and VOUT. The device transitions
back into switching regulator mode
when the load current exceeds 10mA,
regardless of inductor value.
Figure 5 shows the load transient
response when the load is increased
from 1mA to 20mA and then back to
1mA. The difference in ripple between
the pulse skipping operation and linear regulator operation can be clearly
seen.
Linear Technology Magazine • May 2005
DESIGN IDEAS
Instrumentation Amplifier with
Clock-Tunable Sampling Eliminates
Errors in Acquisition Systems by Jon Munson
Introduction
The LTC2053 is a highly popular
precision instrumentation amplifier
for differentially acquiring DC or lowfrequency signals—it’s popularity is
mainly due to its offset uncertainty
below 10µV worst case and DC common-mode rejection of 116dB. It owes
its high performance to a switchedcapacitor front-end that drives a
Zero-Drift (ZD) operation amplifier
(shown in Figure 1). The LTC2053
incorporates a fixed-frequency timing
generator to coordinate the switchedcapacitor activity. The nominal input
sampling rate, fS, is 3kHz, which is not
necessarily ideal for all applications.
Enter the LTC2053-SYNC. It offers
all the features of the LTC2053 plus
the ability to set the sampling rate
with an external clock. The sampling
rate is an eighth of the external clock
frequency, and is guaranteed to operate over a 2-octave range above and
below the nominal rate of 24kHz (i.e.
12kHz to 48kHz).
Tuning Input Performance
by External Clocking
The LTC2053 input structure includes
CMOS switches and two 1000pF
capacitors. Since charge transfers
balance the capacitor voltages on each
sampling cycle, the overall behavior is
that of an Infinite-Impulse-Response
(IIR) function that approximates a
first-order lowpass filter (LPF). The
sample rate and corner frequency
of the LPF behavior is related to the
LTC2053-SYNC external clock by the
following relationships:
fS =
fCLK
8
and f3dB ≈
fCLK
72
In the center of the clock frequency
range of the LTC2053-SYNC:
f3dB =
24kHz
= 330Hz
72
Linear Technology Magazine • May 2005
8
+IN
V+
ZERO-DRIFT
OP AMP
+
3
CS
–IN
OUT
CH
–
2
7
÷8
OSC
REF
5
V–
RG
4
6
CLK
1
Figure 1. LTC2053-SYNC instrumentation
amplifier includes an external clock input
for sample rate control.
By varying the clock frequency, the
3dB rolloff characteristic is tunable
over a range of 150Hz–700Hz. This
property can be used to avoid attenuation of a desirable signal component,
improve rejection of an undesired
component, or most importantly, provide frequency placement of Nyquist
input-sampling aliases.
Tuning Output Performance
by External Clocking
The bandwidth of the internal ZD
op-amp is much wider than the first
Nyquist zone established by the
switched capacitor front-end, so the
LTC2053 output naturally reproduces a classical sample-and-hold
“stair-case” waveform, including any
attendant alias frequency energy.
In DC applications of the LTC2053,
the alias energy is negligible, simply
looking like an insignificant spurious “clock noise” (for example, about
1k
5V
V+IN
+
VD
V–IN
–
3
8
+
CLK
2
LTC2053-SYNC
4.7nF
1
–
5
4
7
6 R2
EXTERNAL
CLOCK
0V
5V
VOUT
R1
Figure 2. Recommended clock source coupling
to minimize digitally-induced ground noise.
8µVRMS output at fS with a gain of 250
connection). Sampling theory indicates
that the alias level is proportional to
signal amplitude and increases with
signal frequency. This simply means
that larger sampling steps occur for
more rapidly varying signal waveforms,
such that post-filtering may be needed
to minimize error in the downstream
signal-processing chain.
For acquisition systems with integrating analog-to-digital conversion
(ADC), simply configuring the ZD opamp with heavily capacitive feedback
is ordinarily sufficient to minimize
error. In systems with sample-andhold ADC technology, management of
the Nyquist energy and/or sampling
transients is important. One technique
is to filter the LTC2053 output with
added components, and another is to
synchronize the input sampling with
the ADC sample-and-hold rate (or a
sub-harmonic thereof). The LTC2053SYNC offers improved performance
in either case by allowing the input
sampling rate to be externally controlled. In the filtered case, raising the
sampling rate can help ease the filter
requirements, and thus reduce cost.
In a synchronized mode the need for
special filtering is often completely
eliminated, since LTC2053-SYNC
sampling transients can be arranged
to never coincide with the ADC sampleand-hold aperture.
Using the External
Clock Signal
The external clock input allows for
slaving of the oscillator that generates
the various sampling controls internal to the LTC2053-SYNC. The input
sampling is performed at a rate that
is an eighth of the clock signal due to
the multiphase nature of the internal
sequencing. If the clock pin is left not
continued on page 38
33
DESIGN IDEAS
Temperature-to-Frequency Converter
Runs for Years on Two AA Batteries
by Cheng-Wei Pei
Introduction
There are many advantages in converting temperature to frequency,
including the ability to transmit
encoded temperature readings over
isolated channels. A frequency carrier
allows complete electrical and thermal
isolation of the temperature measurement circuit, because transmission
can occur via capacitive, inductive or
optical coupling. A simple edge counter
on the receiving end is all that is needed
to demodulate the signal for highly
accurate temperature reading.
Figure 1 shows a simple batteryoperated temperature monitor that
outputs a frequency proportional to
temperature. The beauty of the circuit
lies in its simplicity and low power
draw: a mere 27µA typical at room
temperature, and 50µA max over the
industrial temperature range—low
enough to run from a pair of 1800mAH
AA batteries for over four years. The
circuit maintains operation with supply voltages as low as 2.5V.
Circuit Description
Figure 1 contains a current source (using the amplifier section of an LTC1541
micropower op amp, comparator and
reference) driving the SET pin of an
LTC6906 micropower oscillator. A
1.2V reference voltage is attenuated
FREQUENCY (kHz)
200
10M
1.2V
2
3
–
1M
BATT
8
1/3 LTC1541
1
RCURRENT
49.9k
+
4
1M
10M
160
ACTUAL
140
15
35 55 75
TEMP (°C)
95 115 135
Figure 2. A graph of output frequency versus
temperature. The slight bow in the circuit
comes from the 1/(1 – T) dependence of the
frequency, and is repeatable with part-to-part
variations.
1k
SET
DIV
BATT
11.5M
5
6
+
1/3 LTC1541
7
–
10M
Figure 1. The micropower circuit shown draws 50µA max quiescent current (27µA typical at
room temperature) and contains only two components (not counting external resistors). The
circuit runs on supply voltages from 2.5V–5.5V, and can be powered by CMOS logic gates or
microprocessor outputs.
by 10 and forced across the 49.9kΩ
resistor (RCURRENT), which creates a
constant current source regardless
of the voltage at the SET pin. The
temperature monitoring function is
not readily apparent from the schematic, because the LTC6906 clock
output is temperature independent
in common usage. The trick is to take
advantage of the unique architecture
of the LTC6906 with constant current
drive of the SET pin. The output of the
LTC6906 is determined by the following equations:
ISET
VSET • 10pF
 ISET

26mV • ln 
 – 2.3mV(T – 27)
–18
 82 × 10 
THEORETICAL
OUT
LTC6906
ISET
VSET =
180
120
34
1/3
LTC1541
FREQUENCY =
220
100
–45 –25 –5
BATT
VSET depends on temperature, but
only in the 2.3mV term.
In a typical application of the
LTC6906, the temperature dependence of VSET is irrelevant, because
a resistor to ground, RSET, sets the
output frequency. Thus:
ISET =
VSET
RSET
FREQUENCY =
VSET RSET
1
=
VSET • 10pF RSET • 10pF
Here, though, the LTC6906 finds
itself in an atypical application. We
want to bring out the temperature
dependence of VSET, so ISET is held constant in the circuit shown in Figure 1.
The temperature dependence on VSET
causes the frequency to change with
temperature (as shown in Figure 2):
FREQUENCY =
ISET 10pF
 ISET

26mV • ln 
 – 2.3mV(T – 27)
–18
 82 × 10 
The DIV pin and the amount of current sunk by the current source set
the frequency range of the circuit in
Figure 1. This current can be adjusted
by changing the value of RCURRENT, with
the equation:
ISET =
0.12V
RCURRENT
As shown, the current source is
designed to sink 2.4µA from the SET
pin of the LTC6906, and the DIV
Linear Technology Magazine • May 2005
DESIGN IDEAS
pin is left unconnected. This gives
an output range of approximately
110kHz–170kHz over the –40°C to
85°C industrial temperature range.
A larger ISET current would move the
frequency range to higher frequencies,
within the capabilities of the LTC6906.
Higher output frequencies, though,
come at the cost of higher quiescent
current. The output of the LTC6906
should also be buffered or isolated
with a resistor if the LTC6906 is driving more than 50pF of capacitance or
supplying over 1mA of load current.
Heavier loads dissipate more power in
the IC, which causes additional heating of the part and possible skewing
of the ambient temperature measurement results.
The 1kΩ resistor at the SET pin
serves to isolate the sensitive pin from
any stray capacitance, and does not
affect the temperature performance
of the circuit. The use of an isolation resistor along with a guard ring
minimizes errors due to board leakage
currents.
The comparator section of the
LTC1541 is used in Figure 1 as a low
battery monitor. The supply voltage
is divided and compared to the 1.2V
reference, and the output of the comparator goes low if the supply voltage
drops below 2.6V.
Circuit Performance
Figure 2 compares the theoretical temperature versus frequency plot of the
circuit in Figure 1 (with ISET = 2.4µA)
with actual measurements taken from
a circuit in the lab. The graph shows
a monotonic curve that agrees well
with theory, and the architecture of
the LTC6906 ensures that the circuit
performance is repeatable with partto-part variations, thus simplifying
calibration.
The low quiescent current of
the LTC6906, even at high output
frequencies, is low enough that the
dissipated quiescent power does not
affect the temperature reading of the
circuit. At 50µA quiescent current
with a 3V power supply voltage (two
AA batteries in series), the LTC6906
dissipates 150µW, which adds approximately 24.8m°C to the junction
temperature. At room temperature
(27°C), this represents less than 0.1%
error in the temperature-to-frequency
conversion.
The other possible source of error
is the current source, where an input
reference drift over temperature would
change the value of the current, and
thus the frequency. The LTC1541’s
internal reference drift is less than
0.1% over the industrial temperature
range, which ultimately contributes
less than 0.01% of error to the temperature circuit (considering the 0.1
voltage gain of the current source).
Output Transmission
Though the temperature measurement circuit discussed in this article
is extremely low power, the circuit
components necessary to transmit
the output frequency over isolated
channels may not be. There are many
ways to transmit information over
isolated channels, and some of them
require significantly more current
than the 50µA of the temperature
circuit.1 Optical sources (IR diodes,
photo transistors, etc.) and RF power
BATT
3.2V
VDD
TEMPERATURE
MONITORING
CIRCUIT IN
FIGURE 1
1.58k
IR DIODE
Figure 3. CMOS logic shown gating the power supply of the temperature monitoring circuit
and the transmission circuitry (an LED). The circuit may draw milliamps in its “on” state, but
reducing the “on” duty cycle can significantly lower the average dissipated power.
Linear Technology Magazine • May 2005
amplifiers can require many milliamps
of quiescent operating current. One
way to mitigate the significant loss
of these measurement devices is to
gate the power to the system on and
off, which keeps the average power
very low.
If the temperature measurement
function is not needed continuously,
the low power and high supply rejection
of the LTC6906 and LTC1541 allow the
circuit to be powered by a CMOS logic
gate or microprocessor output pin. The
system diagram shown in Figure 3
features CMOS gates that enable and
disable the temperature monitoring
circuit and its buffer/transmission circuitry. Using this method, the average
power consumption of the temperature
monitor circuit alone can be reduced to
nanoamps or picoamps. Even if 10mA
of current is required to drive external
transmission and logic circuitry, if the
system is only active 1% of the time,
the average current will be 100µA. A
circuit with 100µA of average current
will operate on a pair of AA batteries
for over two years.
If more frequent transmission is
necessary, and the 1 millisecond turnon time of the LTC6906 would make
circuit timing too complex, the 50µA
quiescent current of the temperature
monitoring circuit is low enough that
it can always stay on, regardless of
the status of the transmission circuitry. The CMOS logic would then
be designed to enable and disable
only the output buffer/transmission
circuitry.
Conclusion
The LTC6906 micropower oscillator and the LTC1541 combination
amplifier, comparator, and reference
can combine to create a robust,
accurate, and repeatable temperatureto-frequency monitor that runs off of
low-voltage power supplies and can be
electrically and thermally isolated from
other electronic circuits.
Notes
1 Keep in mind that any high current circuit elements dissipate power, and therefore generate
heat. Maintain enough distance between these
components and the LTC6906 to prevent errors in
the ambient temperature measurement.
35
DESIGN IDEAS
Compact DDR Memory Power
by Jason Leonard
Introduction
The LTC3776 is a high efficiency,
2-phase dual DC/DC synchronous
controller that provides a complete
power solution for DDR memory. Its
first output is designed to supply the
I/O power VDDQ, while the second
output, which has symmetric source
and sink load current capability, provides the bus termination power VTT.
The LTC3776 features a No RSENSE
constant frequency current mode
architecture that requires no current
sense resistors or Schottky diodes.
It operates from a wide input supply
from 2.75V to 9.8V, making it ideal
for 3.3VIN and 5VIN applications. The
LTC3776’s two channels operate outof-phase, reducing the required input
capacitance, while its high operating
frequency of up to 850kHz allows the
use of small inductors and capacitors.
The LTC3776 is available in a tiny 4mm
x 4mm QFN package or in a 24-lead
narrow SSOP package.
circuit can source up to 3A of load current on the VDDQ supply and can sink
or source up to 3A on the VTT supply.
The 2.5V regulation point is set by the
R1-R2 resistor divider. The VTT voltage
is internally programmed to regulate
to half the voltage on the VREF pin via
an internal resistor divider. Thus, to
achieve the VTT = VDDQ/2 DDR memory
requirement, the VDDQ output can be
simply tied to the VREF pin, without
requiring any additional external
resistors. The VTT = VDDQ/2 requirement is met even during startup as
illustrated in Figure 2. Figure 3 shows
the efficiency for this circuit. Since
the VDDQ output voltage is adjustable,
the LTC3776 is compatible with all
generations of DDR memory.
Adjustable, Synchronizable
or Spreadable Frequency
The LTC3776 offers three selectable
operating frequencies—300kHz,
550kHz, or 750kHz—or it can be synchronized to an external clock source
between 250kHz and 850kHz using
the LTC3776’s phase-locked loop. This
allows the switching frequency of both
the VDDQ and VTT output to be synchro-
3.3V to 2.5V/1.25V Dual
Step-Down DC/DC Converter
Figure 1 illustrates a design solution
for a 3.3V to 2.5V (VDDQ) and 1.25V
(VTT) step-down DC/DC converter. This
100k
PGOOD
IPRG1
Conclusion
The LTC3776 is a dual step-down
DC/DC controller that provides both
the VDDQ and VTT supplies with a single
IC. It requires few external components
and enables a small, easy-to-use,
highly efficient solution that makes
the LTC3776 the ideal choice for DDR
memory power.
0.5V/DIV
VIN
3.3V
10µF
×2
VIN
nized not only to each other, but also
to a system clock. Alternatively, the
LTC3776 can be programmed to enter
spread spectrum modulation mode,
in which the frequency is randomly
varied between 450kHz and 580kHz
to reduce conducted and radiated electromagnetic interference (EMI) (See
“Dual Switcher with Spread Specturm
Reduces EMI” in Linear Technology
Magazine, December 2004, page 9).
4ms/DIV
Figure 2. Startup waveforms
for the circuit in Figure 1
IPRG2
SENSE1+ SENSE2+
L1
1.5µH
(VDDQ)VOUT1
2.5V
3A
MP1
TG1
TG2
SW1
SW2
MP2
L2
1.5µH
LTC3776
187k
1nF
100µF
59k
BG2
PGND
PGND
VREF
FREQ
VFB1
VFB2
ITH1
ITH2
MN2
2.2nF
SYNC/SSEN
22k
6.2k
SGND
100pF
330pF
L1, L2: VISHAY IHLP-2525CZ-01
MP1/MN1, MP2/MN2: Si7540P COMPLEMENTARY P/N
Figure 1. Complete DDR power solution using the LTC3776
36
90
100µF
VDDQ
80
EFFICIENCY (%)
BG1
MN1
100
VOUT2 (VTT)
1.25V
±3A
70
VTT
60
50
40
30
20
10
0
10
1k
100
LOAD CURRENT (mA)
10k
Figure 3. Efficiency versus load
current for the circuit in Figure 1
Linear Technology Magazine • May 2005
NEW DEVICE CAMEOS
New Device Cameos
Dual Low Dropout, Low Noise,
Micropower Regulators with
Independent Inputs Work
in Tracking Supplies
The LT3027 and LT3028 are dual low
dropout, low noise, micropower regulators with independent inputs. The
LT3027 has two regulators capable
of providing 100mA of output current, whereas the LT3028 combines
a 100mA and a 500mA regulator.
Typical dropout voltage for the 100mA
regulator is 300mVat the rated output
current; the 500mA regulator of the
LT3028 has a typical dropout voltage of 320mV. Each regulator has
its own independent input, allowing
for flexibility in power management.
Quiescent current for each of the
regulators is less than 30µA, ideal for
use in battery-powered systems. Both
regulators also feature an independent
shutdown state, lowering quiescent
current to less than 0.1µA. Quiescent
current is well controlled in dropout.
The LT3027 and LT3028 are capable
of operating with the voltage at the ADJ
pin above the regulated output voltage.
This allows for the regulators to be
used with power supply control devices
that sequence, track, or ratio multiple
supplies, such as the LTC2923. The
LT3027 and LT3028 regulators also
feature low noise operation with the
addition of an external 0.01µF bypass
capacitor. Over the 10Hz to 100kHz
bandwidth, output voltage noise is
reduced to 20µVRMS. The 100mA
regulators can operate with as low as
1µF of capacitance on the output while
the 500mA regulator requires 4.7µF,
though the use of the external bypass
capacitor necessitates larger output
capacitors. Small ceramic capacitors
can be used on these devices without
the need for added series resistance
as is common with other regulators.
Internal protection circuitry on the
regulators includes reverse-battery
protection, current limiting and thermal limiting.
Both regulators are adjustable
with an output voltage range of 1.22V
to 20V. The LT3027 is packaged in
Linear Technology Magazine • May 2005
thermally enhanced 10-lead MSOP
and DFN (3mm × 3mm) packages and
the LT3028 is available in thermally
enhanced 16-lead TSSOP and DFN
(5mm × 3mm) packages.
Synchronous DC/DC
Converter Features Low
EMI and Programmable
Output Tracking
LTC3809 and LTC3809-1 are low
power, synchronous step-down DC/
DC converters that can deliver high
efficiency with a low quiescent current. Each can provide output voltages
as low as 0.6V and output currents
as high as 7A from a wide, 2.75V to
9.8V, input range, making them ideal
devices for single lithium-ion cell, other
multi-cell and distributed DC power
systems. LTC3809 and LTC3809-1
also take advantage of No RSENSETM
current mode technology by sensing the voltage across the main (top)
power MOSFET to improve efficiency
and reduce the size and cost of the
solution. Both include other popular
features, such as current mode control
for excellent AC and DC line and load
regulation, low dropout (100% duty
cycle) for maximum energy extraction
from a battery, output overvoltage
protection and short circuit current
limit protection.
LTC3809’s adjustable high operating frequency (300kHz–750kHz)
allows the use of small surface mount
inductors and ceramic capacitors for
a compact power supply solution. It
also includes important features for
noise-sensitive applications, including
a phase-locked loop (PLL) for frequency
synchronization and spread spectrum
frequency modulation to minimize
electromagnetic interference (EMI).
Spread spectrum modulation minimizes the need for EMI shields and filters
in applications such as navigation
systems, wireless LANs, data acquisition boards and industrial/military
radio devices by spreading the nominal
operating frequency (550kHz) over a
range of frequencies between 460kHz
and 635kHz.
LTC3809-1 operates at a fixed
frequency of 550kHz. It also offers
flexibility of start-up control with a
fixed internal start-up time, an adjustable external soft-start, or the ability
to track another voltage source. This
flexibility of start-up control not only
reduces the inrush current surge and
prevents output voltage overshoot,
but also provides the ability of output
tracking in multiple power supply
systems.
Both LTC3809 and LTC3809-1
are available in a low profile (0.8mm
height), tiny 3mm × 3mm leadless DFN
package or a 10-pin MSOP exposed
pad package.
Dual Synchronous,
400/800mA, 2.25MHz
Step-Down DC/DC Regulators
in a 10-Lead MSOP
The LTC3548 is a dual, constant
frequency, synchronous step-down
DC/DC converter, intended for low
power applications. It operates within
a 2.5V to 5.5V input voltage range
and has a fixed 2.25MHz switching
frequency, making it possible to use capacitors and inductors that are under
1.2mm in height. The LTC3548 is the
latest in the LTC3407 and LTC3407-2
family of dual regulators and features
improved Burst Mode ripple and two
outputs of 400mA and 800mA. It is
available in a small MS10 package,
allowing two DC/DC Regulators to
occupy less than 0.2 square inches
of board real estate.
The outputs of the LTC3548 are
independently adjustable from 0.6V
to 5V. For battery-powered applications that have input voltages above
and below the output voltage, the
LTC3548 can be used in a single
inductor, positive buck-boost converter configuration. Two built-in
0.40Ω switches allows up to 400mA
and 800mA of output current at high
efficiency. Internal compensation
minimizes external components and
board space.
Efficiency is extremely important in
battery-powered applications, and the
LTC3548 keeps efficiency high with an
automatic, power saving Burst Mode
operation, which reduces gate charge
37
NEW DEVICE CAMEOS
losses at low load currents. With no
load, both converters together draw
only draw 40µA, and in shutdown, the
device draws less than 1µA, making it
ideal for low current applications.
The LTC3548 uses a current-mode,
constant frequency architecture that
benefits noise sensitive applications.
Burst Mode operation is an efficient
solution for low current applications,
but sometimes noise suppression
is a higher priority. To reduce noise
problems, a pulse-skipping mode is
available, which decreases the ripple
noise at low currents. Although not
as efficient as Burst Mode operation
at low currents, pulse-skipping mode
still provides high efficiency for moderate loads. In dropout, the internal
P-channel MOSFET switch is turned
on continuously, thereby maximizing
the usable battery life.
A Power-On Reset output is available for microprocessor systems
to insure proper startups. Internal
undervoltage comparators on both
outputs pull the POR output low if the
output voltages are not above –8.5%
of the regulation. The POR output is
delayed by 262,144 clock cycles (about
117ms) after achieving regulation, but
is pulled low immediately when either
ouput is out of regulation.
The small size, efficiency, low external component count, and design
flexibility of the LTC3548 make it an
ideal DC/DC converter for portable
devices.
LTC2053-SYNC, continued from page 33
LTC2053-SYNC, the use of an RC
coupling network at the external clock
input pin is recommended, as shown
in Figure 2.
architecture in those difficult signal
acquisition situations where sampling
artifacts may be otherwise difficult or
impractical to manage. The external
clocking feature allows controlling the
sampling rate over at least a 2-octave
range to optimize performance and
reduce (or eliminate) antialias filter
complexity.
connected, then the internal oscillator
free-runs at approximately 24kHz and
the sampling rate is thus about 3kHz.
When an external clock is applied, the
internal oscillator’s feedback is overdriven and all timing is then based on
the external frequency. To minimize
digital ground-noise transients at the
LTC3418, continued from page 20
QFN package with an exposed pad to
facilitate heat sinking.
The LTC3418 can be configured for
either Burst Mode, pulse skip or forced
continuous operation. Burst Mode
operation provides high efficiency over
the entire load range by reducing gate
charge losses at light loads. In the
LTC3418, the burst clamp is adjusted
by varying the DC voltage at the Sync/
Mode pin within a 0V–1V range. The
voltage at this pin sets the minimum
peak inductor current during each
switching cycle in Burst Mode operation. If the minimum peak inductor
current delivers more energy than is
demanded by the load current, the
internal power switches skip switching
cycles to maintain regulation. Burst
Mode operation provides an efficient
solution for light-load applications,
but sometimes noise suppression
takes priority over efficiency. Forced
continuous operation, though not
as efficient as Burst Mode operation
at light loads, maintains a steady
frequency, making it easier to reduce
noise and RF interference.
Voltage tracking is enabled by applying a ramp voltage to the TRACK
38
Conclusion
The LTC2053-SYNC offers a means to
utilize the exceptional low frequency
precision of the LTC2053 sampling
pin. When the voltage on the TRACK
pin is below 0.8V, the feedback voltage regulates to this tracking voltage.
When the tracking voltage exceeds
0.8V, tracking is disabled and the feedback voltage regulates to the internal
0.8V reference voltage.
A High Efficiency 1.2V/8A
Step-Down Regulator with
All Ceramic Capacitors
Figure 1 shows a 1.2V step-down
switching regulator that can be
used as a core supply voltage for
microprocessors. It uses all ceramic
capacitors and tracks an I/O voltage
of 2.5V. This circuit provides a regulated 1.2V output at up to 8A from a
3.3V input. Efficiency for this circuit
is as high as 87% and is shown in
Figure 2. The switching frequency
for this circuit is set at 2MHz by an
external resistor, ROSC. Operating at a
frequency this high allows the use of
a lower valued and physically smaller
inductor. During start-up, the output
of the LTC3418 coincidentally tracks
the I/O supply voltage. Once the I/O
supply voltage exceeds 1.2V, tracking
is disabled and the LTC3418 regulates
its output voltage to 1.2V.
Ceramic capacitors offer low cost
and low ESR, but many switching
regulators have difficulty operating
with them. The LTC3418, however,
includes OPTI-LOOP compensation,
which allows it to operate properly with
ceramic input and output capacitors.
The problem that many switching
regulators have when using ceramic
capacitors is that their ESR is too low,
which leads to loop instability. That is,
the phase margin of the control loop
can drop to inadequate levels without
the aid of the zero that is normally
generated from the higher ESR of
tantalum capacitors. The LTC3418
allows loop stability to be achieved
over a wide range of loads and output
capacitors with the proper selection of
compensation components at the ITH
and VFB pins.
Conclusion
The LTC3418 is a monolithic, synchronous step-down DC/DC converter that
is well suited to applications requiring
up to 8A of output current. Its high
switching frequency and internal
low RDS(ON) power switches allow the
LTC3418 to provide a small solution
size with high efficiency.
Linear Technology Magazine • May 2005
DESIGN TOOLS
DESIGN TOOLS
Databooks
The 2004 set of eleven Linear databooks is available
and supersedes all previous Linear databooks. Each
databook contains product data sheets, selection
guides, QML/space information, package information,
appendices, and a complete index to the set.
For more information, or to obtain any of the databooks,
contact your local sales office (see the back of this
magazine), or visit www.linear.com.
Amplifiers (Book 1 of 2) —
• Operational Amplifiers
Amplifiers (Book 2 of 2) —
• Operational Amplifiers
• Instrumentation Amplifiers
• Application Specific Amplifiers
References, Filters, Comparators, Special
Functions, RF & Wireless —
• Voltage References • Special Functions
• Monolithic Filters
• RF & Wireless
• Comparators
• Optical Communications
• Oscillators
Monolithic Switching Regulators —
• Micropower Switching Regulators
• Continuous Switching Regulators
Switching Regulator Controllers (Book 1 of 2) —
• DC/DC Controllers
Switching Regulator Controllers (Book 2 of 2) —
• DC/DC Controllers
• Digital Voltage Programmers
• Off-Line AC/DC Controllers
Linear Regulators, Charge Pumps,
Battery Chargers —
• Linear Regulators
• Charge Pump DC/DC Converters
• Battery Charging & Management
Hot Swap Controllers, MOSFET Drivers, Special
Power Functions —
• Hot Swap Controllers
• Power Switching & MOSFET Drivers
• PCMCIA Power Controllers
• CCFL Backlight Converters
• Special Power Functions
Data Converters (Book 1 of 2) —
• Analog-to-Digital Converters
Data Converters (Book 2 of 2) —
• Analog-to-Digital Converters
• Digital-to-Analog Converters
• Switches & Multiplexers
Interface, System Monitoring & Control —
• Interface — RS232/562, RS485,
Mixed Protocol, SMBus/I2C
• System Monitoring & Control — Supervisors,
Margining, Sequencing & Tracking Controllers
Information furnished herein by Linear Technology Corporation is believed to be accurate and reliable. However,
no responsibility is assumed for its use. Linear Technology
Corporation makes no representation that the interconnection of its circuits, as described herein, will not infringe on
existing patent rights.
Linear Technology Magazine • May 2005
www.linear.com
Brochures
Customers can quickly and conveniently find and retrieve
product information and solutions to their applications.
Located at www.linear.com., the site quickly searches our
database of technical documents and displays weighted
results of our data sheets, application notes, design
notes, Linear Technology magazine issues and other
LTC publications. The LTC website simplifies the product selection process by providing convenient search
methods, complete application solutions and design
simulation programs for Power, Filter, Op Amp and Data
Converter applications. Search methods include a text
search for a particular part number, keyword or phrase.
And the most powerful, a parametric search engine. After
selecting a desired product category, engineers can
specify and sort by key parameters and specifications
that satisfy their design requirements.
Power Management & Wireless Solutions for Handheld
Products — The solutions in this product selection guide
solve real-life problems for cell phones, digital cameras,
PDAs and other portable devices. Circuits are shown for
Li-Ion battery chargers, battery managers, USB support,
system power regulation, display drivers, white LED
drivers, photoflash chargers, DC/DC converters, SIM
and smart card interfaces, photoflash chargers, and RF
PA power supply and control. All solutions are designed
to maximize battery run time, save space and reduce
EMI where necessary—important considerations when
designing circuits for handheld devices.
Purchase Products Online
Credit Card Purchases—Purchase online direct from
Linear Technology at www.linear.com using a credit card.
Create a personalized account to check order history,
shipment information and reorder products.
Linear Express Distribution — Get the parts you need.
Fast. Most devices are stocked for immediate delivery.
Credit terms and low minimum orders make it easy to get
you up and running. Place and track orders online. Apply
today at www.linear.com or call (866) 546-3271.
Applications Handbooks
Linear Applications Handbook, Volume I — Almost a
thousand pages of application ideas covered in depth by
40 Application Notes and 33 Design Notes. This catalog
covers a broad range of real world linear circuitry. In
addition to detailed, systems-oriented circuits, this
handbook contains broad tutorial content together with
liberal use of schematics and scope photography. A
special feature in this edition includes a 22-page section
on SPICE macromodels.
Linear Applications Handbook, Volume II — Continues
the stream of real world linear circuitry initiated by Volume
I. Similar in scope to Volume I, this book covers Application Notes 40 through 54 and Design Notes 33 through
69. References and articles from non-LTC publications
that we have found useful are also included.
Linear Applications Handbook, Volume III —
This 976-page handbook includes Application Notes 55
through 69 and Design Notes 70 through 144. Subjects
include switching regulators, measurement and control
circuits, filters, video designs, interface, data converters,
power products, battery chargers and CCFL inverters.
An extensive subject index references circuits in Linear
data sheets, design notes, application notes and Linear
Technology magazines.
CD-ROM
The March 2005 CD-ROM contains product data sheets,
application notes and Design Notes released through
February of 2005. Use your browser to view product
categories and select products from parametric tables
or simply choose products and documents from part
number, application note or design note indexes.
Automotive Electronic Solutions— This selection guide
features recommended Linear Technology solutions for
a wide range of functions commonly used in today’s
automobiles, including telematics and infotainment
systems, body electronics and engine management,
safety systems and GPS/navigation systems.
Linear Technology’s high-performance analog ICs
provide efficient, compact and dependable solutions
to solve many automotive application requirements.
Software
SwitcherCAD™ III/LTC SPICE — LTC SwitcherCAD III is
a fully functional SPICE simulator with enhancements
and models to ease the simulation of switching regulators. This SPICE is a high performance circuit simulator
and integrated waveform viewer, and also includes
schematic capture. Our enhancements to SPICE result
in much faster simulation of switching regulators than is
possible with normal SPICE simulators. SwitcherCAD III
includes SPICE, macromodels for 80% of LTC’s switching
regulators and over 200 op amp models. It also includes
models of resistors, transistors and MOSFETs. With this
SPICE simulator, most switching regulator waveforms
can be viewed in a few minutes on a high performance
PC. Circuits using op amps and transistors can also be
easily simulated. Download at www.linear.com
FilterCAD™ 3.0 — FilterCAD 3.0 is a computer aided design program for creating filters with Linear Technology’s
filter ICs. FilterCAD is designed to help users without
special expertise in filter design to design good filters
with a minimum of effort. It can also help experienced
filter designers achieve better results by playing “what if”
with the configuration and values of various components
and observing the results. With FCAD, you can design
lowpass, highpass, bandpass or notch filters with a
variety of responses, including Butterworth, Bessel,
Chebychev, elliptic and minimum Q elliptic, plus custom
responses. Download at www.linear.com
SPICE Macromodel Library — This library includes LTC
op amp SPICE macromodels. The models can be used
with any version of SPICE for analog circuit simulations.
These models run on SwitcherCAD III/LTC SPICE.
Noise Program — This PC program allows the user to
calculate circuit noise using LTC op amps, determine
the best LTC op amp for a low noise application, display
the noise data for LTC op amps, calculate resistor noise
and calculate noise using specs for any op amp.
39
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© 2005 Linear Technology Corporation/Printed in U.S.A./30K
www.linear.com
Linear Technology Magazine • May 2005