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you, then simply set R9 = R
TH(LOW)
If you are using a thermistor that doesn’t have a 1:7 HIGH/
LOW ratio, or you wish to set the HIGH/LOW limits to
different temperatures, then the more generic network in
Figure 11 should work.
Once the thermistor, R
TH
, has been selected and the
thermistor value is known at the temperature limits, then
resistors R9 and R9A are given by:
For NTC thermistors:
R9 = 6 R
TH(LOW)
• R
TH(HIGH)
/(R
TH(LOW)
– R
TH(HIGH)
)
R9A = 6 R
TH(LOW)
• R
TH(HIGH)
/(R
TH(LOW)
– 7 • R
TH(HIGH)
)
where R
TH(LOW)
> 7 • R
TH(HIGH)
For PTC thermistors:
R9 = 6 R
TH(LOW)
• R
TH(HIGH)
/(R
TH(HIGH)
– R
TH(LOW)
)
R9A = 6 R
TH(LOW)
• R
TH(HIGH)
/(R
TH(HIGH)
– 7 •
R
TH(LOW)
)
where R
TH(HIGH)
> 7R
TH(LOW)
Example #1: 10k NTC with custom limits
TLOW = 0°C, THIGH = 50°C
R
TH
= 10k at 25°C,
R
TH(LOW)
= 32.582k at 0°C
R
TH(HIGH)
= 3.635k at 50°C
R9 = 24.55k 24.3k (nearest 1% value)
R9A = 99.6k 100k (nearest 1% value)
Example #2: 100k NTC
TLOW = 5°C, THIGH = 50°C
R
TH
= 100k at 25°C,
R
TH(LOW)
= 272.05k at 5°C
R
TH(HIGH)
= 33.195k at 50°C
R9 = 226.9k 226k (nearest 1% value)
R9A = 1.365M 1.37M (nearest 1% value)
Example #3: 22k PTC
TLOW = 0°C, THIGH = 50°C
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Figure 10. Voltage Divider Thermistor Network Figure 11. General Thermistor Network
LTC4006
NTC
R9
C7 R
TH
4006 F10
6
LTC4006
NTC
R9
C7 R9A R
TH
4006 F11
6
R
TH
= 22k at 25°C,
R
TH(LOW)
= 6.53k at 0°C
R
TH(HIGH)
= 61.4k at 50°C
R9 = 43.9k 44.2k (nearest 1% value)
R9A = 154k
Sizing the Thermistor Hold Capacitor
During the hold interval, C7 must hold the voltage across
the thermistor relatively constant to avoid false readings.
A reasonable amount of ripple on NTC during the hold
interval is about 10mV to 15mV. Therefore, the value of C7
is given by:
C7 = t
HOLD
/(R9/7 • –ln(1 – 8 • 15mV/4.5V))
= 10 • R
RT
• 17.5pF/(R9/7 • –ln(1 – 8 • 15mV/4.5V)
Example:
R9 = 24.3k
R
RT
= 309k (~2 hour timer)
C7 = 0.57µF 0.56µF (nearest value)
Disabling the Thermistor Function
If the thermistor is not needed, connecting a resistor
between DCIN and NTC will disable it. The resistor should
be sized to provide at least 10µA with the minimum voltage
applied to DCIN and 10V at NTC. Do not exceed 30µA into
NTC. Generally, a 301k resistor will work for DCIN less
than 15V. A 499k resistor is recommended for DCIN
between 15V and 24V.
Optional Simple Battery Discharge Path Circuit
It is NOT recommended that one permit battery current to
flow backwards through R
SENSE
, inductor and out the
TGATE MOSFET internal diode to reach V
OUT
. The TGATE
MOSFET is off when V
IN
< V
BAT
. Figure 12 shows an op-
tional high efficiency discharge path for the battery such that
V
OUT
power comes from lossless “diode or” of V
IN
and V
BAT
.
Normally when V
IN
> V
BAT
, P-channel MOSFET Q1B V
GS
=
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0V keeping Q1B in the off state while P-channel MOSFET
Q1A is on. If V
IN
were to suddenly go away, Q1B internal
diode will provide a passive but instant discharge path for
battery current to reach V
OUT
and hold up the load. Q1B
internal diode has the same current rating as the FET itself,
but has a very high V
f
of about a volt such that heat will
quickly build up in Q1B if left alone. However as V
IN
’s voltage
falls below V
BAT
by Q1B’s V
GS
threshold, Q1B will then turn
on shorting out its internal diode removing both the heat
and voltage losses created by the diode. When V
IN
falls to
zero volts, Q1B gate will be driven to the same voltage as
V
BAT
providing the lowest possible RDS
ON
value. A zener
diode along with a 100k resistor in series with the Q1B gate
protects the gate from any hazardous voltage spikes that
can exceed Q1B maximum permissible V
GS
voltage. The
zener voltage rating must be less than Q1B V
GS(MAX)
volt-
age but greater than V
BAT
.
Since Q1A and Q1B are always at opposite states and share
the same load, it is often advantagous to combine both FETs
into a single package and save PCB space. The P
D
rate of
the FET that is on is enhanced when the other FET is off. The
choice of a combined Q1 should take into account the high-
est load current conditions of both paths and choose
whichever is greater as the driving force behind the MOSFET
selection. If the V
IN
supply is going to collapse very slowly
such that Q1B is not turned on quickly enough for the given
load and stay within its P
D
limits, you should install a suit-
able Schottky diode in parallel with Q1B.
PCB Layout Considerations
For maximum efficiency, the switch node rise and fall times
should be minimized. To prevent magnetic and electrical
field radiation and high frequency resonant problems,
proper layout of the components connected to the IC is
essential. (See Figure 13.) Here is a PCB layout priority list
for proper layout. Layout the PCB using this specific order.
1. Input capacitors need to be placed as close as possible
to switching FET’s supply and ground connections.
Shortest copper trace connections possible. These
parts must be on the same layer of copper. Vias must
not be used to make this connection.
2. The control IC needs to be close to the switching FET’s
gate terminals. Keep the gate drive signals short for a
clean FET drive. This includes IC supply pins that con-
nect to the switching FET source pins. The IC can be
placed on the opposite side of the PCB relative to above.
3. Place inductor input as close as possible to switching
FET’s output connection. Minimize the surface area of
this trace. Make the trace width the minimum amount
needed to support current—no copper fills or pours.
Avoid running the connection using multiple layers in
parallel. Minimize capacitance from this node to any
other trace or plane.
Figure 12. Optional Simple High
Efficiency Battery Discharge Path
INDUCTOR R
SENSE
ZENER
18V
Q1B
TGATE
V
BAT
V
OUT
V
IN
4006 F12
Q1A
100k
4006 F13
V
BAT
L1
V
IN
HIGH
FREQUENCY
CIRCULATING
PATH
BAT
SWITCH NODE
C2
C3
D1
Figure 13. High Speed Switching Path
18
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Figure 14. Kelvin Sensing of Charging Current
CSP
4006 F14
DIRECTION OF CHARGING CURRENT
R
SNS
BAT
4. Place the output current sense resistor right next to
the inductor output but oriented such that the IC’s
current sense feedback traces going to resistor are not
long. The feedback traces need to be routed together
as a single pair on the same layer at any given time with
smallest trace spacing possible. Locate any filter
component on these traces next to the IC and not at the
sense resistor location.
5. Place output capacitors next to the sense resistor
output and ground.
6. Output capacitor ground connections need to feed
into same copper that connects to the input capacitor
ground before tying back into system ground.
General Rules
7. Connection of switching ground to system ground or
internal ground plane should be single point. If the
system has an internal system ground plane, a good
way to do this is to cluster vias into a single star point
to make the connection.
8. Route analog ground as a trace tied back to IC ground
(analog ground pin if present) before connecting to
any other ground. Avoid using the system ground
plane. CAD trick: make analog ground a separate
ground net and use a 0 resistor to tie analog ground
to system ground.
9. A good rule of thumb for via count for a given high
current path is to use 0.5A per via. Be consistent.
10. If possible, place all the parts listed above on the same
PCB layer.
11. Copper fills or pours are good for all power connec-
tions except as noted above in Rule 3. You can also use
copper planes on multiple layers in parallel too—this
helps with thermal management and lower trace in-
ductance improving EMI performance further.
12. For best current programming accuracy provide a
Kelvin connection from R
SENSE
to CSP and BAT. See
Figure 13 as an example.
It is important to keep the parasitic capacitance on the R
T
,
CSP and BAT pins to a minimum. The traces connecting
these pins to their respective resistors should be as short
as possible.
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LTC4006EGN-2#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Battery Management 4A, Simplified Li-Ion Charger for 3-Cell
Lifecycle:
New from this manufacturer.
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