LTC4081
16
4081fa
For more information www.linear.com/LTC4081
BATTERY CHARGER
Programming Charge Current
The battery charge current is programmed using a single
resistor from the PROG pin to ground. The charge current
is 400 times the current out of the PROG pin. The program
resistor and the charge current are calculated using the
following equations:
R
PROG
= 400
1V
I
BAT
, I
BAT
= 400
1V
R
PROG
The charge current out of the BAT pin can be determined
at any time by monitoring the PROG pin voltage and using
the following equation:
I
BAT
=
V
PROG
R
PROG
400
Stability Considerations
The LTC4081 battery charger contains two control loops:
constant-voltage and constant-current. The constant-
voltage loop is stable without any compensation when a
battery is connected with low impedance leads. Excessive
lead length, however, may add enough series inductance
to require a bypass capacitor of at least 1
µ
F from BAT to
GND. Furthermore, a 4.7µF capacitor with a 0.2W to 1W
series resistor from BAT to GND is required to keep ripple
voltage low when the battery is disconnected.
In constant-current mode, the PROG pin voltage is in
the feedback loop, not the battery voltage. Because of
the additional pole created by PROG pin capacitance,
capacitance on this pin must be kept to a minimum. With
no additional capacitance on the PROG pin, the battery
charger is stable with program resistor values as high
as 25k. However, additional capacitance on this node
reduces the maximum allowed program resistor. The pole
frequency at the PROG pin should be kept above 100kHz.
Therefore, if the PROG pin is loaded with a capacitance,
C
PROG
, the following equation should be used to calculate
the maximum resistance value for R
PROG
:
R
PROG
1
2π 100kHz C
PROG
Figure 2. Isolating Capacitive Load
on PROG Pin and Filtering
4081 F02
C
FILTER
CHARGE
CURRENT
MONITOR
CIRCUITRY
R
PROG
LTC4081
PROG
GND
10k
Average, rather than instantaneous, battery current may be
of interest to the user. For example, when the switching
regulator operating in low current mode is connected in
parallel with the battery, the average current being pulled
out of the BAT pin is typically of more interest than the
instantaneous current pulses. In such a case, a simple RC
filter can be used on the PROG pin to measure the average
battery current as shown in Figure 2. A 10k resistor has
been added between the PROG pin and the filter capacitor
to ensure stability.
Undervoltage Charge Current Limiting (UVCL)
USB powered systems tend to have highly variable source
impedances (due primarily to cable quality and length). A
transient load combined with such impedance can easily
trip the UVLO threshold and turn the battery charger off un-
less undervoltage charge current limiting is implemented.
Consider a situation where the LTC4081 is operating under
normal conditions and the input supply voltage begins to
sag (e.g. an external load drags the input supply down).
If the input voltage reaches V
UVCL
(approximately 300mV
above the battery voltage, DV
UVCL
), undervoltage charge
current limiting will begin to reduce the charge current in
an attempt to maintain DV
UVCL
between V
CC
and BAT. The
LTC4081 will continue to operate at the reduced charge
current until the input supply voltage is increased or volt-
age mode reduces the charge current further.
Operation from Current Limited Wall Adapter
By using a current limited wall adapter as the input sup-
ply, the LTC4081 can dissipate significantly less power
when programmed for a current higher than the limit of
the wall adapter.
APPLICATIONS INFORMATION
LTC4081
17
4081fa
For more information www.linear.com/LTC4081
V
CC
MP1
MN1
1k
4k
1k
1
I
CHG
2
D1
4
Li-Ion
BATTERY
SYSTEM
LOAD
4081 F03
LTC4081
BAT
USB
POWER
(100mA)
5V WALL
ADAPTER
(500mA)
PROG
+
Figure 3. Combining Wall Adapter and USB Power
Consider a situation where an application requires a 200mA
charge current for a discharged 800mAh Li-Ion battery.
If a typical 5V (non-current limited) input supply is avail-
able then the peak power dissipation inside the part can
exceed 300mW.
Now consider the same scenario, but with a 5V input sup-
ply with a 200mA current limit. To take advantage of the
supply, it is necessary to program the LTC4081 to charge
at a current greater than 200mA. Assume that the LTC4081
charger is programmed for 300mA (i.e., R
PROG
= 1.33kW)
to ensure that part tolerances maintain a programmed
current higher than 200mA. Since the battery charger will
demand a charge current higher than the current limit of
the input supply, the supply voltage will collapse to the
battery voltage plus 200mA times the on-resistance of the
internal PFET. The on-resistance of the battery charger
power device is approximately 0.7W with a 5V supply.
The actual on-resistance will be slightly higher due to the
fact that the input supply will have collapsed to less than
5V. The power dissipated during this phase of charging
is approximately 30mW. That is a ten times improvement
over the non-current limited supply power dissipation.
USB and Wall Adapter Power
Although the LTC4081 allows charging from a USB port,
a wall adapter can also be used to charge Li-Ion batter-
ies. Figure 3 shows an example of how to combine wall
adapter and USB power inputs. A P-channel MOSFET,
MP1,
is used to prevent back conducting into the USB
port when a wall adapter is present and Schottky diode,
D1, is used to prevent USB power loss through the 1k
pull-down resistor.
Typically a wall adapter can supply significantly more
current than the current-limited USB port. Therefore, an
N-channel MOSFET, MN1, and an extra program resistor
can be used to increase the charge current when the wall
adapter is present.
Power Dissipation
The conditions that cause the LTC4081 battery charger to
reduce charge current through thermal feedback can be
approximated by considering the total power dissipated
in the IC. For high charge currents, the LTC4081 power
dissipation is approximately:
P
D
= V
CC
V
BAT
( )
I
BAT
+P
D _BUCK
Where P
D
is the total power dissipated within the IC, V
CC
is the input supply voltage, V
BAT
is the battery voltage, I
BAT
is the charge current and P
D_BUCK
is the power dissipation
due to the regulator. P
D_BUCK
can be calculated as:
P
D
_BUCK
=V
OUT
I
OUT
1
η
1
Where V
OUT
is the regulated output of the switching
regulator, I
OUT
is the regulator load and
η
is the regulator
efficiency at that particular load.
It is not necessary to perform worst-case power dissipa-
tion scenarios because the LTC4081 will automatically
reduce the charge current to maintain the die temperature
at approximately 115°C. However, the approximate ambi-
ent temperature at which the thermal feedback begins to
protect the IC is:
T
A
= 115°C – P
D
θ
JA
T
A
= 115°C – (V
CC
– V
BAT
) • I
BAT
θ
JA
if the regulator
is off.
Example: Consider the extreme case when an LTC4081 is
operating from a 6V supply providing 250mA to a 3V Li-Ion
battery and the regulator is off. The ambient temperature
above which the LTC4081 will begin to reduce the 250mA
charge current is approximately:
T
A
= 115°C – (6V – 3V) • (250mA) • 43°C/W
T
A
= 115°C – 0.75W • 43°C/W = 115°C – 32.25°C
T
A
= 82.75°C
APPLICATIONS INFORMATION
LTC4081
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4081fa
For more information www.linear.com/LTC4081
If there is more power dissipation due to the regulator,
the thermal regulation will begin at a somewhat lower
temperature. In the above circumstances, the LTC4081
can be used above 82.75°C, but the charge current will
be reduced from 250mA. The approximate current at a
given ambient temperature can be calculated:
I
BAT
=
115°C T
A
V
CC
V
BAT
( )
θ
JA
Using the previous example with an ambient temperature of
85°C, the charge current will be reduced to approximately:
I
BAT
=
115°C85°C
6V3V
( )
43°C/W
=
30°C
129°C/A
=232.6mA
Furthermore, the voltage at the PROG pin will change
proportionally with the charge current as discussed in
the Programming Charge Current section.
V
CC
Bypass Capacitor
Many types of capacitors can be used for input bypassing;
however, caution must be exercised when using multi-layer
ceramic capacitors. Because of the self-resonant and high
Q characteristics of some types of ceramic capacitors, high
voltage transients can be generated under some start-up
conditions, such as connecting the battery charger input to
a live power source. Adding a 1
W
series resistor in series
with an X5R ceramic capacitor will minimize start-up voltage
transients. For more information, refer to Application Note 88.
Thermistors
The LTC4081 NTC trip points are designed to work with therm-
istors whose resistance-temperature characteristics follow
Vishay Dales R-T Curve 1.” The Vishay NTHS0603NO1N1002J
is an example of such a thermistor. However, Vishay Dale
has many thermistor products that follow the R-T Curve 1”
characteristic in a variety of sizes. Furthermore, any thermis-
tor whose ratio of R
COLD
to R
HOT
is about 5 will also work
(Vishay Dale R-T Curve 1 shows a ratio of R
COLD
to R
HOT
of
3.266/0.5325 = 6.13).
Power conscious designs may want to use thermistors whose
room temperature value is greater than 10k. Vishay Dale has a
number of values of thermistor from 10k to 100k that follow
the R-T Curve 1.” Using different R-T curves, such as Vishay
Dale R-T Curve 2”, is also possible. This curve, combined with
LTC4081 internal thresholds, gives temperature trip points of
approximately 0°C (falling)
and 40°C (rising), a delta of 40°C.
This delta in temperature can be moved in either direction by
changing the value of R
NOM
with respect to R
NTC
. Increasing
R
NOM
will move both trip points to higher temperatures. To
calculate R
NOM
for a shift to lower temperature for example,
use the following equation:
R
NOM
=
R
COLD
3.266
R
NTC
at 25°C
where R
COLD
is the resistance ratio of R
NTC
at the desired cold
temperature trip point. If you want to shift the trip points to
higher temperatures use the following equation:
R
NOM
=
R
HOT
0.5325
R
NTC
at 25°C
where R
HOT
is the resistance ratio of R
NTC
at the desired hot
temperature trip point.
Here is an example using a 100k R-T Curve 2 thermistor
from Vishay Dale. The difference between the trip points is
40°C, from before, and we want the cold trip point to be 0°C,
which would put the hot trip point at 40°C. The R
NOM
needed
is calculated as follows:
R
NOM
=
R
COLD
3.266
R
NTC
at 25°C
=
2.816
3.266
• 10k =8.62k
The nearest 1% value for R
NOM
is 8.66k. This is the value used
to bias the NTC thermistor to get cold and hot trip points of
approximately C and 40°C respectively. To extend the delta
APPLICATIONS INFORMATION

LTC4081EDD#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Battery Management Low Power Battery Charger w/ NTC + Buck DC/DC
Lifecycle:
New from this manufacturer.
Delivery:
DHL FedEx Ups TNT EMS
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