Automotive LED Driver with
Integrated Hall-Effect Switch
A1569K
16
Allegro MicroSystems, LLC
955 Perimeter Road
Manchester, NH 03103-3353 U.S.A.
www.allegromicro.com
APPLICATION INFORMATION
Power Dissipation
The most critical design consideration when using a linear regula-
tor such as the A1569K is the power produced internally as heat
and the rate at which that heat can be dissipated.
There are three sources of power dissipation in the A1569K:
• The quiescent power to run the control circuits
• The power in the reference circuit
• The power due to the regulator voltage drop
QUIESCENT POWER
The quiescent power is the product of the quiescent current (IINQ)
and the supply voltage (VIN), and it is not related to the regulated
current. The quiescent power (PQ) is therefore defined as:
PQ = VIN × IINQ (5)
REFERENCE POWER
The reference circuit draws the reference current from the supply
and passes it through the reference resistor to ground. The refer-
ence circuit power is the product of the reference current and the
difference between the supply voltage and the reference voltage,
typically 1.2 V. The reference power (PREF) is therefore defined
as:
REGULATOR POWER
In most application circuits, the largest dissipation will be pro-
duced by the output current regulator. The power dissipated the
current regulator is simply the product of the output current and
the voltage drop across the regulator. The regulator power the
output is defined as:
PREG = (VIN – VLED
) × ILED (7)
Note that the voltage drop across the regulator (VREG) is always
greater than the specified minimum dropout voltage (VDO). The
output current is regulated by making this voltage large enough
to provide the voltage drop from the supply voltage to the total
forward voltage of all LEDs in series (VLED). The total power
dissipated in the A1569K is the sum of the quiescent power, the
reference power, and the power in the regulator:
PD = PQ + PREG – PREF (8)
The power that is dissipated in the LEDs is:
PLED = VLED × ILED (9)
where VLED is the voltage across all LEDs in the string.
From these equations (and as illustrated in Figure 10), it can be
seen that, if the power in the A1569K is not limited, then it will
increase as the supply voltage increases while the power in the
LEDs will remain constant.
Dissipation Limits
There are two features limiting the power that can be dissipated
by the A1569K: thermal shutdown and thermal foldback.
THERMAL SHUTDOWN
If the thermal foldback feature is disabled by connecting the
THTH pin to GND, or if the thermal resistance from the A1569K
to the ambient environment is high, then the silicon temperature
will rise to the thermal shutdown threshold and the current will be
disabled. After the current is disabled, the power dissipated will
drop and the temperature will fall. When the temperature falls by
the hysteresis of the thermal shutdown circuit, the current will be
re-enabled and the temperature will start to rise again. This cycle
will repeat continuously until the ambient temperature drops or
the A1569K is switched off. The period of this thermal shutdown
cycle will depend on several electrical, mechanical, and thermal
parameters.
THERMAL FOLDBACK
If RθJA is low enough, then the thermal foldback feature will have
time to act. This will limit the silicon temperature by reducing the
regulated current and therefore the dissipation.
The thermal monitor will reduce the LED current as the tempera-
ture of the A1569K increases above the thermal monitor activa-
tion temperature (TJM), as shown in Figure 11. The figure shows
the operation of the A1569K with a string of two white LEDs
running at 150 mA. The forward voltage of each LED is 3.15 V,
and the graph shows the current as the supply voltage increases
from 15 to 18 V. As the supply voltage increases, without the
thermal foldback feature, the current would remain at 150 mA, as
shown by the dashed line. The solid line shows the resulting cur-
rent decrease as the thermal foldback feature acts.
If the thermal foldback feature did not affect LED current, the
current would increase the power dissipation and therefore
the silicon temperature. The thermal foldback feature reduces
power in the A1569K in order to limit the temperature increase,
as shown in Figure 12. The figure shows the operation of the
A1569K under the same conditions as Figure 11, that is, a string
of two white LEDs running at 150 mA, with each LED forward
voltage at 3.15 V. The graph shows the temperature as the supply
voltage increases from 15 to 18 V. Without the thermal foldback
PREF =
IN REFREF
R
(6)