LTC4055/LTC4055-1
16
4055fb
OPERATION
where V
PROG
is the PROG pin voltage and R
PROG
is the
total resistance from the PROG pin to ground.
For example, if typical 485mA charge current is required,
calculate:
R
V
mA
k
PROG
==
1
485
48 500 100•,
For best stability over temperature and time, 1% metal
lm resistors are recommended. Under trickle-charge
conditions, this current is reduced to 10% of the full-
scale value.
THE CHARGE TIMER
The programmable charge timer is used to terminate the
charge cycle. The timer duration is programmed by an
external capacitor at the TIMER pin and is also a function
of the resistance on PROG. Typically the charge time is:
t Hours
C R Hours
Fk
TIMER
TIMER PROG
()
••
.•
=
μ
3
0 1 100
The timer starts when an input voltage greater than the
undervoltage lockout threshold level is applied, or when
leaving shutdown and the voltage on the battery is less than
the recharge threshold. At power-up or exiting shutdown
with the battery voltage less than the recharge threshold,
the charge time is a full cycle. If the battery is greater than
the recharge threshold, the timer will not start and charging
is prevented. If after power-up the battery voltage drops
below the recharge threshold, or if after a charge cycle
the battery voltage is still below the recharge threshold,
the charge time is set to one half of a full cycle.
The LTC4055/LTC4055-1 have a feature that extends
charge time automatically. Charge time is extended if
the charge current in constant-current mode is reduced
due to load current, undervoltage charge current limit-
ing or thermal regulation. This change in charge time is
inversely proportional to the change in charge current. As
the LTC4055/LTC4055-1 approach constant-voltage mode
the charge current begins to drop. This change in charge
current is part of the normal charging operation of the
part and should not affect the timer duration. Therefore,
the LTC4055/LTC4055-1 detect that the change in charge
current is due to voltage mode, and increase the timer
period back to its programmed operating period.
Once a time-out occurs and the voltage on the battery is
greater than the recharge threshold, the charge current
stops, and the CHRG output assumes a high impedance
state to indicate that the charging has stopped.
Connecting the TIMER pin to ground disables the battery
charger.
CHRG STATUS OUTPUT PIN
When the charge cycle starts, the CHRG pin is pulled
to ground by an internal N-channel MOSFET capable of
driving an LED. After a time-out occurs, the pin assumes
a high impedance state.
NTC Thermistor
The battery temperature is measured by placing a negative
temperature coeffi cient (NTC) thermistor close to the
battery pack. The NTC circuitry is shown in Figure 3. To use
this feature, connect the NTC thermistor, R
NTC
, between
the NTC pin and ground and a resistor, R
NOM
, from the
NTC pin to V
NTC
. R
NOM
should be a 1% resistor with a
value equal to the value of the chosen NTC thermistor at
25°C (this value is 10k for a Vishay NTHS0603N02N1002J
thermistor). The LTC4055/LTC4055-1 go into hold mode
when the resistance, R
HOT
, of the NTC thermistor drops
to 0.41 times the value of R
NOM
or approximately 4.1k,
which should be at 50°C. The hold mode freezes the timer
and stops the charge cycle until the thermistor indicates a
return to a valid temperature. As the temperature drops,
the resistance of the NTC thermistor rises. The LTC4055/
LTC4055-1 are designed to go into hold mode when the
value of the NTC thermistor increases to 2.82 times the
value of R
NOM
. This resistance is R
COLD
. For a Vishay
NTHS0603N02N1002J thermistor, this value is 28.2k
which corresponds to approximately 0°C. The hot and cold
comparators each have approximately 3°C of hysteresis
to prevent oscillation about the trip point. Grounding the
NTC pin disables the NTC function.
LTC4055/LTC4055-1
17
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OPERATION
THERMISTORS
The LTC4055/LTC4055-1 NTC trip points were designed
to work with thermistors whose resistance-temperature
characteristics follow Vishay Dale’s “R-T Curve 2.” The
Vishay NTHS0603N02N1002J is an example of such a
thermistor. However, Vishay Dale has many thermistor
products that follow the “R-T Curve 2” characteristic in
a variety of sizes. Furthermore, any thermistor whose
ratio of R
COLD
to R
HOT
is about 7.0 will also work
(Vishay Dale R-T Curve 2 shows a ratio of R
COLD
to R
HOT
of 2.815/0.4086 = 6.89).
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 these as indicated
in the NTC Thermistor section will give temperature trip
points of approximately 3°C and 47°C, a delta of 44°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 lower temperatures.
Likewise a decrease in R
NOM
with respect to R
NTC
will
move the trip points to higher temperatures. To calculate
R
NOM
for a shift to lower temperature for example, use
the following equation:
R
R
RatC
NOM
COLD
NTC
2 815
25
.
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
R
RatC
NOM
HOT
NTC
0 4086
25
.
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 1 thermistor
from Vishay Dale. The difference between the trip points
is 44°C, from before, and we want the cold trip point to
be 0°C, which would put the hot trip point at 44°C. The
R
NOM
needed is calculated as follows:
R
R
RatC
kk
NOM
COLD
NTC
==
2 815
25
3 266
2 815
100 116
.
.
.
+
+
R
NOM
100k
R
NTC
100k
NTC
V
NTC
15
0.1V
NTC_ENABLE
4055 F03a
LTC4055/LTC4055-1
NTC BLOCK
TOO_COLD
TOO_HOT
0.74 • V
NTC
0.29 • V
NTC
+
16
+
+
R
NOM
121k
R
NTC
100k
R1
13.3k
NTC
V
NTC
15
0.1V
NTC_ENABLE
4055 F03b
TOO_COLD
TOO_HOT
0.74 • V
NTC
0.29 • V
NTC
+
16
LTC4055/LTC4055-1
NTC BLOCK
(3a) (3b)
Figure 3. NTC Circuits
LTC4055/LTC4055-1
18
4055fb
OPERATION
The nearest 1% value for R
NOM
is 115k. This is the value
used to bias the NTC thermistor to get cold and hot trip
points of approximately 0°C and 44°C respectively. To
extend the delta between the cold and hot trip points a
resistor, R1, can be added in series with R
NTC
(see Figure 3b).
The values of the resistors are calculated as follows:
R
RR
RRRR
NOM
COLD HOT
COLD HOT HOT
=
=
()
.–.
.
.–.
•–
2 815 0 4086
1
0 4086
2 815 0 4086
where R
NOM
is the value of the bias resistor, R
HOT
and
R
COLD
are the values of R
NTC
at the desired temperature
trip points. Continuing the example from before with a
desired hot trip point of 50°C:
R
RR
k
Rk
NOM
COLD HOT
==
()
=
=
()
=
.–.
•. .
.–.
.
.–.
. –. –.
2 815 0 4086
100 3 266 0 3602
2 815 0 4086
1 100
0 4086
2 815 0 4086
3 266 0 3602 0 3602
120.8k, 121k is nearest 1%
13.3k, 13.3k is nearest 1%
The fi nal solution is as shown if Figure 3b where R
NOM
=
121k, R1 = 13.3k and R
NTC
= 100k at 25°C.
CURRENT LIMIT UNDERVOLTAGE LOCKOUT
An internal undervoltage lockout circuit monitors the input
voltage and keeps the current limit circuits of the part in
shutdown mode until V
IN
rises above the undervoltage
lockout threshold. The current limit UVLO circuit has a
built-in hysteresis of 125mV. Furthermore, to protect
against reverse current in the power MOSFET, the current
limit UVLO circuit keeps the current limit shutdown if
V
OUT
exceeds V
IN
. If the current limit UVLO comparator
is tripped, the current limit circuits will not come out of
shutdown until V
OUT
falls 50mV below the V
IN
voltage.
CHARGER UNDERVOLTAGE LOCKOUT
Internal undervoltage lockout circuits monitor the V
IN
and
V
OUT
voltages and keep the charger circuits of the part
shut down until V
IN
or V
OUT
rises above the undervoltage
lockout threshold. The charger UVLO circuit has a built-
in hysteresis of 125mV. Furthermore, to protect against
reverse current in the power MOSFET, the charger UVLO
circuit keeps the charger shutdown if V
BAT
exceeds V
OUT
.
If the charger UVLO comparator is tripped, the charger
circuits will not come out of shutdown until V
OUT
exceeds
V
BAT
by 50mV.
SHUTDOWN
The LTC4055/LTC4055-1 can be shut down by forcing the
SHDN pin greater than 1V. In shutdown, the currents on
IN1/IN2, OUT and BAT are decreased to less than 2.5μA
and the internal battery charge timer is reset. All power
paths are put in a Hi-Z state.
SUSPEND
The LTC4055/LTC4055-1 can be put in suspend mode by
forcing the SUSP pin greater than 1V. In suspend mode
the ideal diode function from BAT to OUT and the output
charger are kept alive. The rest of the part is shut down
to conserve current and the battery charge timer is reset
if V
OUT
becomes less than V
BAT
.
V
IN
and Wall Adapter Bypass Capacitor
Many types of capacitors can be used for input bypassing.
However, caution must be exercised when using multilayer
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 charger input to a hot
power source. For more information, refer to Application
Note 88.

LTC4055EUF#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Battery Management USB Pwr Cntr & Li-Ion Lin Chr
Lifecycle:
New from this manufacturer.
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