Automotive High Current LED Controller
A6265
13
Allegro MicroSystems, LLC
115 Northeast Cutoff
Worcester, Massachusetts 01615-0036 U.S.A.
1.508.853.5000; www.allegromicro.com
Application Information
Component Selection
External component selection is critical to the successful appli-
cation of the LED driver. Although the inductor, the switching
MOSFET, and the output capacitor are the most critical elements,
the specification of the rectifying diode and sense resistors should
also be carefully considered.
The starting point for component selection is to define the maxi-
mum LED current, the voltage across the LEDs, and the input
operating voltage range. This then allows the average inductor
current under worst case conditions to be calculated. The induc-
tor value is then selected based on the acceptable inductor ripple
current. The amount of ripple current will then determine the
maximum inductor current under worst case conditions. From
this current the switch current sense resistor can be calculated.
LED Current Sense Resistor (R
LS
) If the voltage at the
IREF pin, V
IREF
, is greater than 1V, or if IREF is tied to VREG,
then the value of the LED current sense resistor, R
LS
, can be
calculated from:
R
LS
= V
IDL
/ I
LED
(max) (11)
where V
IDL
is the differential voltage across the LED current
sense amplifier and I
LED
(max) is the maximum LED current.
If V
IREF
is less than 1 V, then the value of the LED current sense
resistor can be calculated from:
R
LS
= V
IREF
/ (10 × I
LED
(max) ) (12)
The typical value for V
IDL
is 100
mV. Examples of various sense
resistor values are given in table 2.
In boost mode, the power loss in the current sense resistor is
worse at the lowest input voltage:
P
LOSS
= (V
LED
/ V
IN
(min)
) × R
LS
× I
2
LED
(13)
In buck-boost mode, the power loss in the current sense resistor is
worse at the lowest input voltage:
P
LOSS
= ( [ V
IN
+ V
LED
] / V
IN
) × R
LS
× I
2
LED
(14)
The resistors should be of a low inductance construction. Surface
mount chip resistors are usually the most suitable, however, axial
or radial leaded resistors can be used provided that the lead length
is kept to a minimum.
Inductor Selection Selecting the correct inductance is a
balance between choosing a value that is small enough to help
reduce size and cost, but high enough to ensure that the inductor
current ripple is kept to an acceptable level. A reasonable target
for the ripple current is 20% of the maximum average current.
The inductor current equations differ slightly depending on
whether the A6265 is configured as a boost or as a buck-boost
converter.
• In a boost converter configuration:
The maximum average inductor current is approximately:
I
L(av)
(max) = I
LED
(max) × V
LED
/ V
IN
(min) (15)
The inductor current ripple is approximately:
I
LRIP
= V
IN
× (V
LED
V
IN
) / (f
OSC
× L × V
LED
) (16)
The inductor value is therefore:
L = V
IN
× ( V
LED
V
IN
) / (f
OSC
× I
LRIP
× V
LED
) (17)
• In a buck-boost configuration:
The maximum average inductor current is approximately:
I
L(av)
(max) = I
LED
(max) × ( V
IN
(min) + V
LED
) / V
IN
(min) (18)
The inductor current ripple is approximately:
I
LRIP
= V
IN
× V
LED
/ (f
OSC
× L × [V
IN
+ V
LED
] ) (19)
The inductor value is therefore:
L = V
IN
× V
LED
/ (f
OSC
× I
LRIP
× [ V
IN
+ V
LED
] ) (20)
where:
V
LED
is the voltage across the LED string,
V
IN
is the supply voltage,
V
IN
(min) is the minimum supply voltage,
L is the inductor value, and
f
OSC
is the oscillator frequency.
With an internal oscillator frequency of 350 kHz, the value of
the inductor for most cases will be between 20 and 50 H. The
maximum inductor current can then be calculated as:
I
L(PK)
= I
L(av)
(max) + (I
RIP
/ 2) (21)
Table 2. Sense Resistor Values
I
LED
(max)
(mA)
R
LS
(mΩ)
350 286
700 143
1000 100
Automotive High Current LED Controller
A6265
14
Allegro MicroSystems, LLC
115 Northeast Cutoff
Worcester, Massachusetts 01615-0036 U.S.A.
1.508.853.5000; www.allegromicro.com
This defines the minimum peak switch current as set by the
switch current sense resistor.
The current rating for the inductor should be greater, by some
margin, than the peak value above, I
L(PK)
. When selecting an
inductor from manufacturers datasheets, there are two current
levels usually defined, the smallest value being the figure to work
with:
• Saturation level, where the inductance value typically drops by
10%, or
• Temperature rise, where the part experiences a certain rise in
temperature at full rated current. This parameter can be defined
between a 20°C and 50°C rise in temperature. It is important to
understand how manufacturers define the maximum operating
temperature, because this can often incorporate the self-heating
temperature rise.
In most cases the limiting current is usually the saturation value.
To improve efficiency, the inductor should also have low winding
resistance, typically < 50 m, and the core material will usually
be ferrite, with low losses at the oscillator frequency.
Recommended inductor manufacturers/series are:
• Coilcraft/ MSS1278T
• TDK/ SLF12575 type H
Diode The diode should have a low forward voltage, to reduce
conduction losses, and a low capacitance, to reduce switching
losses. Schottky diodes can provide both these features if care-
fully selected. The forward voltage drop is a natural advantage
for Schottky diodes and reduces as the current rating increases.
However, as the current rating increases, the diode capacitance
also increases so the optimum selection is usually the lowest cur-
rent rating above the required maximum, in this case I
L(PK)
.
Switch Current Sense Resistor (RSS) Neither the absolute
value of the switch current nor the accuracy of the measurement
is important, because the regulator will continuously adjust the
switch current, within a closed loop, to provide sufficient energy
for the output. For maximum accuracy the switch sense resistor
value should be chosen to maximize the differential signal seen
by the sense amplifier. The input limit of the sense amplifier,
V
IDS
, and the maximum switch current, I
S
(max), therefore define
the maximum value of the sense resistor as:
R
SS
= V
IDS
/ I
S
(max) (22)
Where I
S
(max) is the maximum switch current and should be set
above the maximum inductor current, I
L(PK)
.
This represents the maximum measurable value of the switch
(and inductor) current; however, the peak switch current will
always be less than this, set by the control circuit, depending on
the input voltage and the required load conditions. Because the
switch current control is within a closed loop, it is possible to
reduce the value of the sense resistor to reduce its power dissipa-
tion. However this will reduce the accuracy of the regulated LED
current.
In Boost mode, the power loss in the switch sense resistor is
worse at the lowest input voltage:
P
LOSS
= (V
LED
[V
LED
V
IN
(min)] / V
IN
(min)
2
) × R
SS
× I
2
LED
(23)
In Buck Boost mode, the power loss in the switch sense resistor
is worse at the lowest input voltage:
P
LOSS
= (V
LED
/ V
IN
(min))(V
LED
+ V
IN
(min)) × R
SS
× I
2
LED
(24)
External Switch MOSFET A logic-level N-channel MOSFET
is used as the switch for the DC-to-DC converter. In the boost
configuration the voltage at the drain of the MOSFET is equal
to the maximum voltage across the string of LEDs. In the
buck-boost configuration the output voltage is referenced to
the positive supply. This means that the voltage at the drain of
the MOSFET will reach a voltage equal to the sum of the LED
voltage and the supply voltage. Under load dump conditions,
up to 90 V may be present on this node. In this case the external
MOSFET should therefore be rated at greater than 100 V.
The peak switch current is defined by the maximum inductor cur-
rent, I
L(PK)
. However in most cases the MOSFET will be chosen
by selecting low on-resistance, which usually results in a current
rating of several times the required peak current.
In addition to minimizing cost, the choice of MOSFET should
consider both the on-resistance and the total gate charge. The
total gate charge will determine the average current required from
the internal regulator and thus the power dissipation.
Automotive High Current LED Controller
A6265
15
Allegro MicroSystems, LLC
115 Northeast Cutoff
Worcester, Massachusetts 01615-0036 U.S.A.
1.508.853.5000; www.allegromicro.com
Output Capacitor There are several points to consider when
selecting the output capacitor.
Unlike some switch-mode regulators, the value of the output
capacitor in this case is not critical for output stability. The
capacitor value is only limited by the required maximum ripple
voltage.
Due to the switching topology used, the ripple current for this
circuit is high because the output capacitor provides the LED
current when the switch is active. The capacitor is then recharged
each time the inductor passes energy to the output. The ripple
current on the output capacitor will be equal to the peak inductor
current.
Normally this large ripple current, in conjunction with the
requirement for a larger capacitance value for stability, would
dictate the use of large electrolytic capacitors. However in this
case stability is not a consideration, and the capacitor value can
be low, allowing the use of ceramic capacitors.
To minimize self-heating effects and voltage ripple, the equiva-
lent series resistance (ESR), and the equivalent series inductance
(ESL) should be kept as low as possible. This can be achieved by
multilayer ceramic chip (MLCC) capacitors. To reduce perfor-
mance variation over temperature, low drift types such as X7R
and X5R should be used.
The value of the output capacitor will typically be about 10
F
and it should be rated above the maximum voltage defined by the
series output LEDs.
Reverse Supply Protection Protection for the A6265 is
provided by an external low current diode between the supply
and the VIN pin, as shown in the Functional Block Diagrams
section. The isolation MOSFET shown in figure 3 is only able to
provide isolation when the supply polarity is correct. However,
with an additional P-channel MOSFET, it is also possible to
provide reverse battery protection to the switching elements and
the LEDs. The additional FET should be connected, as shown in
figure 4, with the drain to the supply and the source to the source
connection of the original isolation MOSFET.
In the complete circuit, consideration should be given to limiting
the maximum gate-source voltage of the FET. If the supply volt-
age is likely to exceed 20 V, then either: a Zener clamp must be
added in parallel with the gate-source resistor to prevent damage
to the FET, or a second resistor added as shown in figure 3.
To FF1
VBAT
To VIN
Figure 4. Example of a supply isolation MOSFET

A6265KLPTR-T

Mfr. #:
Manufacturer:
Description:
IC LED DRIVER CTRLR DIM 16TSSOP
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