10
LT1510/LT1510-5
where R
PROG
is the total resistance from PROG pin to
ground.
For example, 1A charging current is needed.
R
V
A
k
PROG
=
()()
=
2 465 2000
1
493
.
.
Charging current can also be programmed by pulse width
modulating I
PROG
with a switch Q1 to R
PROG
at a frequency
higher than a few kHz (Figure 4). Charging current will be
proportional to the duty cycle of the switch with full current
at 100% duty cycle.
When a microprocessor DAC output is used to control
charging current, it must be capable of sinking current
at a compliance up to 2.5V if connected directly to the
PROG pin.
APPLICATIONS INFORMATION
WUU
U
even this low current drain. A 47k resistor from adapter
output to ground should be added if Q3 is used to ensure
that the gate is pulled to ground.
With divider current set at 25µA, R4 = 2.465/25µA = 100k
and,
R
RV
RA
k
kA
k
BAT
3
4 2 465
2 465 4 0 05
100 8 4 2 465
2 465 100 0 05
240
=
()
()
+
()
=
()
+
()
=
.
..
..
..µµ
Lithium-ion batteries typically require float voltage accu-
racy of 1% to 2%. Accuracy of the LT1510 OVP voltage is
±0.5% at 25°C and ±1% over full temperature. This leads
to the possibility that very accurate (0.1%) resistors might
be needed for R3 and R4. Actually, the temperature of the
LT1510 will rarely exceed 50°C in float mode because
charging currents have tapered off to a low level, so 0.25%
resistors will normally provide the required level of overall
accuracy.
External Shutdown
The LT1510 can be externally shut down by pulling the V
C
pin low with an open drain MOSFET, such as VN2222. The
V
C
pin should be pulled below 0.8V at room temperature
to ensure shutdown. This threshold decreases at about
2mV/°C. A diode connected between the MOSFET drain
and the V
C
pin will still ensure the shutdown state over all
temperatures, but it results in slightly different conditions
as outlined below.
If the V
C
pin is held below threshold, but above 0.4V, the
current flowing
into
the BAT pin will remain at about
700µA. Pulling the V
C
pin below 0.4V will cause the current
to drop to 200µA and reverse, flowing
out
of the BAT pin.
Although these currents are low, the long term effect may
need to be considered if the charger is held in a shutdown
state for very long periods of time, with the charger input
voltage remaining. Removing the charger input voltage
causes all currents to drop to near zero.
If it is acceptable to have 200µA flowing into the battery
while the charger is in shutdown, simply pull the V
C
pin
directly to ground with the external MOSFET. The resistor
divider used to sense battery voltage will pull current out
Figure 4. PWM Current Programming
PWM
R
PROG
4.64k
300
PROG
C
PROG
1µF
Q1
VN2222
5V
0V
LT1510
1510 F04
I
BAT
= (DC)(1A)
Lithium-Ion Charging
The circuit in Figure 2 uses the 16-pin LT1510 to charge
lithium-ion batteries at a constant 1.3A until battery volt-
age reaches a limit set by R3 and R4. The charger will then
automatically go into a constant-voltage mode with cur-
rent decreasing to zero over time as the battery reaches full
charge. This is the normal regimen for lithium-ion charg-
ing, with the charger holding the battery at “float” voltage
indefinitely. In this case no external sensing of full charge
is needed.
Current through the R3/R4 divider is set at a compromise
value of 25µA to minimize battery drain when the charger
is off and to avoid large errors due to the 50nA bias current
of the OVP pin. Q3 can be added if it is desired to eliminate
11
LT1510/LT1510-5
APPLICATIONS INFORMATION
WUU
U
period, after which the LT1510 can be shut down by
pulling the V
C
pin low with an open collector or drain.
Some external means must be used to detect the need for
additional charging if needed, or the charger may be
turned on periodically to complete a short float-voltage
cycle.
Current trip level is determined by the battery voltage, R1
through R3, and the internal LT1510 sense resistor
( 0.18 pin-to-pin). D2 generates hysteresis in the trip
level to avoid multiple comparator transitions.
Nickel-Cadmium and Nickel-Metal-Hydride Charging
The circuit in Figure 6 uses the 8-pin LT1510 to charge
NiCd or NiMH batteries up to 12V with charging currents
of 0.5A when Q1 is on and 50mA when Q1 is off.
of the battery, canceling part or all of the 200µA. Note that
if net current is into the battery and the battery is removed,
the charger output voltage will float high, to near input
voltage. This could be a problem when reinserting the
battery, if the resulting output capacitor/battery surge
current is high enough to damage either the battery or the
capacitor.
If net current into the battery must be less than zero in
shutdown, there are several options. Increasing divider
current to 300µA - 400µA will ensure that net battery
current is less than zero. For long term storage conditions
however, the divider may need to be disconnected with a
MOSFET switch as shown in Figures 2 and 5. A second
option is to connect a 1N914 diode in series with the
MOSFET drain. This will limit how far the V
C
pin will be pulled
down, and current ( 700µA) will flow
into
the BAT pin, and
therefore out of the battery. This is not usually a problem
unless the charger will remain in the shutdown state with
input power applied for very long periods of time.
Removing input power to the charger will cause the BAT
pin current to drop to near zero, with only the divider
current remaining as a small drain on the battery. Even
that current can be eliminated with a switch as shown in
Figures 2 and 5.
Figure 5. Disconnecting Voltage Divider
Some battery manufacturers recommend termination of
constant-voltage float mode after charging current has
dropped below a specified level (typically 50mA to 100mA)
and
a further time-out period of 30 minutes to 90 minutes
has elapsed. This may extend the life of the battery, so
check with manufacturers for details. The circuit in Figure
7 will detect when charging current has dropped below
75mA. This logic signal is used to initiate a time-out
Figure 6. Charging NiMH or NiCd Batteries
(Efficiency at 0.5A 90%)
For a 2-level charger, R1 and R2 are found from:
I
R
BAT
PROG
=
()( )
2000 2 465.
R
I
R
II
LOW HI LOW
1
2 465 2000
2
2 465 2000
=
()()
=
()()
..
All battery chargers with fast-charge rates require some
means to detect full charge state in the battery to terminate
the high charging current. NiCd batteries are typically
charged at high current until temperature rise or battery
R3
12k
R4
4.99k
0.25%
R5
220k
OVP
V
IN
+
+
4.2V
4.2V
V
BAT
Q3
VN2222
LT1510
1510 F05
SW
BOOST
GND
SENSE
V
CC
PROG
V
C
BAT
R2
11k
+
R1
100k
Q1
VN2222
* TOKIN OR MARCON CERAMIC
 SURFACE MOUNT
** COILTRONICS CTX33-2
WALL
ADAPTER
1510 F05.5
C1
0.22µF
C
IN
*
10µF
L1**
33µH
LT1510
D1
1N5819
D3
1N5819
D2
1N914
+
C
OUT
22µF
TANT
0.1µF
+
1k
1µF
300
2V TO
20V
I
BAT
ON: I
BAT
= 0.5A
OFF: I
BAT
= 0.05A
12
LT1510/LT1510-5
APPLICATIONS INFORMATION
WUU
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Figure 7. Current Comparator for Initiating Float Time-Out
0.18
GND
NEGATIVE EDGE
TO TIMER
INTERNAL
SENSE
RESISTOR
1510 F06
3.3V OR 5V
ADAPTER
OUTPUT
3
8
7
1
4
2
LT1510
D1
1N4148
C1
0.1µF
BAT
SENSE
R1*
1.6k
R4
470k
R3
430k
R2
560k
LT1011
D2
1N4148
* TRIP CURRENT =
R1(V
BAT
)
(R2 + R3)(0.18)
+
voltage decrease is detected as an indication of near full
charge. The charging current is then reduced to a much
lower value and maintained as a constant trickle charge.
An intermediate “top off” current may be used for a fixed
time period to reduce 100% charge time.
NiMH batteries are similar in chemistry to NiCd but have
two differences related to charging. First, the inflection
characteristic in battery voltage as full charge is ap-
proached is not nearly as pronounced. This makes it more
difficult to use dV/dt as an indicator of full charge, and
change of temperature is more often used with a tempera-
ture sensor in the battery pack. Secondly, constant trickle
charge may not be recommended. Instead, a moderate
level of current is used on a pulse basis ( 1% to 5% duty
cycle) with the time-averaged value substituting for a
constant low trickle.
Thermal Calculations
If the LT1510 is used for charging currents above 0.4A, a
thermal calculation should be done to ensure that junction
temperature will not exceed 125°C. Power dissipation in
the IC is caused by bias and driver current, switch resis-
tance, switch transition losses and the current sense
resistor. The following equations show that maximum
practical charging current for the 8-pin SO package
(125° C/W thermal resistance) is about 0.8A for an 8.4V
battery and 1.1A for a 4.2V battery. This assumes a 60°C
maximum ambient temperature. The 16-pin SO, with a
thermal resistance of 50°C/W, can provide a full 1.5A
charging current in many situations. The 16-pin PDIP falls
between these extremes. Graphs are shown in the Typical
Performance Characteristics section.
P mA V mA V
V
V
mA I
P
IV
V
V
P
IRV
V
tVI f
P
BIAS IN BAT
BAT
IN
BAT
DRIVER
BAT BAT
BAT
IN
SW
BAT SW BAT
IN
OL IN BAT
SENSE
=
()()
+
()
+
()
+
()()
[]
=
()( )
+
()
=
()( )( )
+
()()( )()
=
35 15
75 0012
1
30
55
0
2
2
2
..
..
.. 18
2
()()
I
BAT
R
SW
= Switch ON resistance 0.35
t
OL
= Effective switch overlap time 10ns
f = 200kHz (500kHz for LT1510-5)

LT1510CS#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Battery Management 200kHz 1.5A Stepdn Bat Charger
Lifecycle:
New from this manufacturer.
Delivery:
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