LTC4066/LTC4066-1
19
4066fc
APPLICATIONS INFORMATION
Consider, for example, a USB charge condition where
R
CLPROG
= 2k, R
PROG
= 100k and C
TIMER
= 0.1μF. This
corresponds to a three hour charge cycle. However, if the
HPWR input is set to a logic low, then the input current
limit will be reduced from 500mA to 100mA. With no ad-
ditional system load, this means the charge current will
be reduced to 100mA. Therefore, the termination timer
will automatically slow down by a factor of fi ve until the
charger reaches constant voltage mode (i.e., V
BAT
= 4.2V,
4.1V for LTC4066-1) or HPWR is returned to a logic high.
The charge cycle is automatically lengthened to account for
the reduced charge current. The exact time of the charge
cycle will depend on how long the charger remains in
constant current mode and/or how long the HPWR pin
remains a logic low.
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 if it has not already done so.
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. When the charge current drops below a
programmable threshold while in constant-voltage mode,
the pin assumes a high impedance state (but charge current
continues to fl ow until the charge time elapses). If this
state is not reached before the end of the programmable
charge time, the pin will assume a high impedance state
when a time-out occurs.
The current level at which the CHRG pin changes state is
programmed by the I
STAT
pin. As described in Monitoring
Charge Current and Gas Gauge, the I
STAT
pin sources a
current proportional to the BAT pin current. The LTC4066/
LTC4066-1 monitor the voltage on the I
STAT
pin and turns
off the CHRG N-channel pull-down when V
ISTAT
drops
below 100mV while in constant-voltage mode. The CHRG
current detection threshold can be calculated by the fol-
lowing equation:
I
V
R
V
R
DETECT
ISTAT ISTAT
==
01
1000
100.
For example, to program the CHRG pin to change state at
a battery charge current of 100mA, choose:
R
V
mA
k
ISTAT
==
100
100
1
Note: The end-of-charge (EOC) comparator that moni-
tors the I
STAT
pin voltage for 100mV latches its decision.
Therefore, the fi rst time V
ISTAT
drops below 100mV (i.e.,
I
BAT
drops below 100V/R
ISTAT
) while in constant voltage
mode will toggle CHRG to a high impedance state. If, for
some reason, the charge current rises back above the
threshold, the CHRG pin will not resume the strong pull-
down state. The EOC latch can be reset by toggling the
SHDN pin or toggling the input power to the part. The EOC
latch will also be reset if the BAT pin voltage falls below
the recharge threshold.
LTC4066/LTC4066-1
20
4066fc
APPLICATIONS INFORMATION
NTC Thermistor
The battery temperature is measured by placing a negative
temperature coeffi cient (NTC) thermistor close to the bat-
tery pack. The NTC circuitry is shown in Figure 4. 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 LTC4066/LTC4066-1 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 LTC4066/
LTC4066-1 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 can disable the NTC function.
Thermistors
The LTC4066/LTC4066-1 NTC trip points were designed to
work with thermistors whose resistance-temperature char-
acteristics 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).
+
+
R
NOM
10k
R
NTC
10k
NTC
V
NTC
15
0.1V
NTC_ENABLE
4066 F04a
LTC4066
TOO_COLD
TOO_HOT
0.74 • V
NTC
0.29 • V
NTC
+
14
+
+
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
+
14
LTC4066
(4a) (4b)
Figure 4. NTC Circuits
LTC4066/LTC4066-1
21
4066fc
APPLICATIONS INFORMATION
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 2.” Using these directly
in the manor spelled out previously 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
=Ω
2 815
25
3 266
2 815
100 116
.
.
.
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
k k nearest
Rk
k k is nearest
NOM
COLD HOT
==
()
=
()
.–.
•. .
.–.
., %
.
.–.
. –. –.
.,. %
2 815 0 4086
100 3 266 0 3602
2 815 0 4086
120 8 121 1
1 100
0 4086
2 815 0 4086
3 266 0 3602 0 3602
13 3 13 3 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.
Gas Gauge
The extremely low impedance of the ideal diode between
BAT and OUT (typically 50mΩ) allows users to connect
all of their loads to the OUT pin. Such a confi guration puts
the LTC4066/LTC4066-1 in a unique position whereby it
can monitor all of the current that fl ows into and out of the
battery. Two output pins, I
STAT
and POL, are provided to
enable users to monitor and integrate the battery current
for a true gas gauge function.

LTC4066EUF#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Battery Management USB Power Manager and Li-Ion Charger
Lifecycle:
New from this manufacturer.
Delivery:
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