LTC4012/
LTC4012-1/LTC4012-2
22
4012fa
R
IN
should not be less than 2.37k or more than 6.04k. Val-
ues of R
IN
greater than 3.01k may cause some reduction in
programmed current accuracy. Use these equations and
guidelines, as represented in Table 6, to help select the cor-
rect inductor value. This table was developed for C-grade
p
arts to maintain maximum ∆I
L
near 0.6 I
MAX
with f
PWM
at
550kHz and V
BAT
= 0.5 V
CLP
(the point of maximum ∆I
L
),
assuming that inductor value could also vary by 25% at
I
MAX
. For I-grade parts, reduce maximum ∆I
L
to less than
0.4 I
MAX
, but only if the IC will actually be used to charge
batteries over the wider I-grade temperature range. In that
case, a good starting point can be found by multiplying
the inductor values shown in Table 6 by a factor of 1.6 and
rounding up to the nearest standard value.
Table 6. Minimum Typical Inductor Values
V
CLP
L1
(Typ)
I
MAX
R
SENSE
R
IN
R
PROG
<10V ≥10µH 1A 100mΩ 3.01k 26.7k
10V to 20V ≥20µH 1A 100mΩ 3.01k 26.7k
>20V ≥28µH 1A 100mΩ 3.01k 26.7k
<10V ≥5.1µH 2A 50mΩ 3.01k 26.7k
10V to 20V ≥10µH 2A 50mΩ 3.01k 26.7k
>20V ≥14µH 2A 50mΩ 3.01k 26.7k
<10V ≥3.4µH 3A 33mΩ 3.01k 26.7k
10V to 20V ≥6.8µH 3A 33mΩ 3.01k 26.7k
>20V ≥9.5µH 3A 33mΩ 3.01k 26.7k
<10V ≥2.5µH 4A 25mΩ 3.01k 26.7k
10V to 20V ≥5.1µH 4A 25mΩ 3.01k 26.7k
>20V ≥7.1µH 4A 25mΩ 3.01k 26.7k
To guarantee that a chosen inductor is optimized in any
given application, use the design equations provided and
perform bench evaluation in the target application, par-
ticularly at duty cycles below 20% or above 80% where
PWM frequency can be much less than the nominal value
of 550kHz.
TGATE BOOST Supply
Use the external components shown in Figure 11 to de-
velop a bootstrapped BOOST supply for the TGATE FET
driver. A good set of equations governing selection of the
two capacitors is:
C
Q
V
C C
G
1
20
4 5
2 20 1= =
.
,
where Q
G
is the rated gate charge of the top external NFET
with V
GS
= 4.5V. The maximum average diode current is
then given by:
I
D
= Q
G
• 665kHz
To improve efficiency by increasing V
GS
applied to the
top FET, substitute a Schottky diode with low reverse
leakage for D1.
PWM jitter has been observed in some designs operating
at higher V
IN
/V
OUT
ratios. This jitter does not substantially
affect DC charge current accuracy. A series resistor with a
value of 5Ω to 20Ω can be inserted between the cathode
of D1 and the BOOST pin to remove this jitter, if present.
A resistor case size of 0603 or larger is recommended to
lower ESL and achieve the best results.
applications inForMation
Figure 11. TGATE Boost Supply
20
17
BOOST
INTV
DD
18
SW
LTC4012
4012 F11
C2
2µF
C1
0.1µF
L1
TO
R
SENSE
D1
1N4148
23
4012fa
LTC4012/
LTC4012-1/LTC4012-2
applications inForMation
FET Selection
Two external power MOSFETs must be selected for use
with the charger: an N-channel power switch (top FET)
and an N-channel synchronous rectifier (bottom FET).
Peak gate-to-source drive levels are internally set to
about 5V. Consequently, logic-level FETs must be used.
In addition to the fundamental DC current, selection
criteria for these MOSFETs also include channel resis-
tance R
DS(ON)
, total gate charge Q
G
, reverse transfer
capacitance C
RSS
, maximum rated drain-source voltage
BV
DSS
and switching characteristics such as t
d(ON/OFF)
.
Power dissipation for each external FET is given by:
P
V I T R
V
k V
D TOP
BAT MAX DS ON
CLP
C
( )
( )
=
+
( )
+
2
1 δ
LLP MAX RSS
D BOT
CLP BAT M
I C kHz
P
V V I
2
665
( )
=
( )
AAX DS ON
CLP
T R
V
2
1
( )
+
( )
δ
where δ is the temperature dependency of R
DS(ON)
,
∆T is the temperature rise above the point specified in
the FET data sheet for R
DS(ON)
and k is a constant in-
versely related to the internal LTC4012 top gate driver.
The term (1 + δ
T)
is generally given for a MOSFET in the
form of a normalized R
DS(ON)
curve versus temperature,
but δ of 0.005/°C can be used as a suitable approxima-
tion for logic-level FETs if other data is not available.
C
RSS
= ∆Q
GD
/V
DS
is usually specified in the MOSFET
characteristics. The constant k = 2 can be used in estimat-
ing top FET dissipation. The LTC4012 is designed to work
best with external FET switches with a total gate charge
at 5V of 15nC or less.
For V
CLP
< 20V, high charge current efficiency generally
improves with larger FETs, while for V
CLP
> 20V, top gate
transition losses increase rapidly to the point that using
a topside NFET with higher R
DS(ON)
but lower C
RSS
can
actually provide higher efficiency. If the charger will be
operated with a duty cycle above 85%, overall efficiency
is normally improved by using a larger top FET.
The synchronous (bottom) FET losses are greatest at high
input voltage or during a short circuit, which forces a low
side duty cycle of nearly 100%. Increasing the size of this
FET lowers its losses but increases power dissipation in the
LTC4012. Using asymmetrical FETs will normally achieve
cost savings while allowing optimum efficiency.
Select FETs with BV
DSS
that exceeds the maximum V
CLP
voltage that will occur. Both FETs are subjected to this level
of stress during operation. Many logic-level MOSFETs are
limited to 30V or less.
The LTC4012 uses an improved adaptive TGATE and
BGATE drive that is insensitive to MOSFET inertial delays,
t
d(ON/OFF)
, to avoid overlap conduction losses. Switching
characteristics from power MOSFET data sheets apply
only to a specific test fixture, so there is no substitute for
bench evaluation of external FETs in the target application.
In general, MOSFETs with lower inertial delays will yield
higher efficiency.
Diode Selection
A Schottky diode in parallel with the bottom FET and/or
top FET in an LTC4012 application clamps SW during the
non-overlap times between conduction of the top and
bottom FET switches. This prevents the body diode of the
MOSFETs from forward biasing and storing charge, which
could reduce efficiency as much as 1%. One or both diodes
can be omitted if the efficiency loss can be tolerated. A 1A
Schottky is generally a good size for 3A chargers due to the
low duty cycle of the non-overlap times. Larger diodes can
actually result in additional efficiency (transition) losses
due to larger junction capacitance.
Loop Compensation and Soft-Start
The three separate PWM control loops of the LTC4012
can be compensated by a single set of components at-
tached between the ITH pin and GND. As shown in the
typical LTC4012 application, a 6.04k resistor in series
with a capacitor of at least 0.1µF provides adequate loop
compensation for the majority of applications.
LTC4012/
LTC4012-1/LTC4012-2
24
4012fa
Figure 12. High Speed Switching Path
4012 F12
V
BAT
L1
R
SENSE
HIGH
FREQUENCY
CIRCULATING
PATH
BAT
ANALOG
GROUND
SYSTEM
GROUND
SWITCH NODE
C
IN
SWITCHING GROUND
C
OUT
V
IN
GND
D1
+
The LTC4012 can be soft-started with the compensation
capacitor on the ITH pin. At start-up, ITH will quickly rise
to about 0.25V, then ramp up at a rate set by the com-
pensation capacitor and the 40µA ITH bias current. The
full programmed charge current will be reached when ITH
reaches approximately 2V. With a 0.1µF capacitor, the time
to reach full charge current is usually greater than 1.5ms.
This capacitor can be increased if longer start-up times
are required, but loop bandwidth and dynamic response
will be reduced.
INTV
DD
Regulator Output
Bypass the INTV
DD
regulator output to GND with a low
ESR X5R or X7R ceramic capacitor with a value of 0.47µF
or larger. The capacitor used to build the BOOST supply
(C2 in Figure 11) can serve as this bypass. Do not draw
more than 30mA from this regulator for the host system,
governed by IC power dissipation.
Calculating IC Power Dissipation
The user should ensure that the maximum rated junction
temperature is not exceeded under all operating conditions.
The thermal resistance of the LTC4012 package (θ
JA
) is
37°C/W, provided the Exposed Pad is in good thermal
contact with the PCB. The actual thermal resistance in the
application will depend on forced air cooling and other heat
sinking means, especially the amount of copper on the PCB
to which the LTC4012 is attached. The following formula
may be used to estimate the maximum average power dis-
sipation P
D
(in watts) of the LTC4012, which is dependent
upon the gate charge of the external MOSFETs. This gate
charge, which is a function of both gate and drain voltage
swings, is determined from specifications or graphs in the
manufacturer’s data sheet. For the equation below, find the
gate charge for each transistor assuming 5V gate swing and
a drain voltage swing equal to the maximum V
CLP
voltage.
Maximum LTC4012 power dissipation under normal op-
erating conditions is then given by:
P
D
= DCIN(3mA + I
DD
+ 665kHz(Q
TGATE
+ Q
BGATE
))
– 5I
DD
applications inForMation
where:
I
DD
= Average external INTV
DD
load current, if any
Q
TGATE
= Gate charge of external top FET in Coulombs
Q
BGATE
= Gate charge of external bottom FET in
Coulombs
PCB Layout Considerations
To prevent magnetic and electrical field radiation and
high frequency resonant problems, proper layout of the
components connected to the LTC4012 is essential. Refer
to Figure 12. For maximum efficiency, the switch node
rise and fall times should be minimized. The following
PCB design priority list will help insure proper topology.
Layout the PCB using this specific order.
1.
Input capacitors should be placed as close as possible
to switching FET supply and ground connections with
the shortest copper traces possible. The switching
FETs must be on the same layer of copper as the input
capacitors. Vias should not be used to make these
connections.
2.
Place
the LTC4012 close to the switching FET gate
terminals, keeping the connecting traces short to
produce clean drive signals. This rule also applies to IC
supply and ground pins that connect to the switching
FET source pins. The IC can be placed on the opposite
side of the PCB from the switching FETs.

LTC4012IUF#TRPBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Battery Management Hi Eff, Multi-Chemistry Bat Chr w/ PwrPa
Lifecycle:
New from this manufacturer.
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