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[News Feature]
HIGH-POWER WHITE LED DRIVER RUNS BATTERY-OPERATED PORTABLE LIGHTING
Staff
ED Online ID #17873
October 25, 2007
Many people consider
white LEDs to be the
future of lighting.
Strung together, several
LEDs can replace an incandescent
lamp or a compact fluorescent
lamp. High-power white
LEDs need a dc voltage of about
3.6 V at a current of about 350
mA to achieve full brightness,
about 40 lumens.
In portable applications, white
LEDs are often powered by
sealed lead-acid (SLA) batteries
having a typical output of 12 V.
The circuit shown in the figure
takes this 12-V input and uses it
to power a string of white LEDs.
It features low cost, high efficiency,
constant intensity independent
of variations in battery voltage,
dimming capability, and
battery protection.
The driver circuit uses an
SG1524 pulse-width modulation
(PWM) switching regulator (U1)
operating in boost configuration.
This configuration enables U1 to
produce a maximum output of
about 40 V, which can drive a
string of up to 11 serially connected
1-W white LEDs. Because
of the high power dissipation,
the LEDs must be mounted with
a suitable heatsink. The design
of the driver involves the selection
of an inductor, input capacitor,
output capacitor, switching
transistor, and output diode for
a given operating frequency.
Operating frequency is:
FOSC = 1/(R1 * C1) (1)
A frequency of about 100 kHz
is chosen for this example.
Higher frequencies allow smaller
inductances, but they also
increase switching losses.
The battery’s voltage is 13.2 V
when fully charged and about
10.8 V under full discharge conditions.
The voltage across the
LEDs should be high enough to
forward-bias the LEDs under
varying input voltages. To
ensure this, the required duty
cycle is:
D = (VO+ VD - VIN)/(VO + (2)
VD - V DS)
where VO = output voltage
across the LED string; VD =
diode voltage drop; VIN = minimum
SLA voltage; and VDS =
MOSFET voltage drop.
For an eight-LED string, VO =
28.8 V, VIN = 11 V, and VD =
0.4 V for the Schottky diode.
Ignoring VDS, the required duty
cycle is 62.3%. U1 has two
independent switching transistors,
each capable of supplying
about 100 mA and operating
with a maximum duty cycle of
45%. To achieve the required
duty cycle, the two transistors
are connected in parallel. Since
the LEDs need current higher
than 100 mA, an external MOSFET
is required.
To compute the value of L1,
start with the average inductor
current, which is:.
I Lavg= I O/(1 - D) (3)
If the ripple in the inductor current
dIL is a certain percentage
of the average current, the peak
inductor current is:
ILpk = ILavg + dIL/2 (4)
Assuming 40% ripple over the
average current, ILpk = 1.12 A.
Therefore, the inductance is:
L = (VIN * D)/(FOSC * dIL ) (5)
In this example, Equation 5
gives the minimum value of
inductance as 184.3 µH, where
VIN is 11 V. The output capacitor’s
value depends on the ripple
allowed on the output voltage.
Meanwhile, the input
capacitor’s value depends on
the current peak.
To ensure constant illumination,
the current through the LED must
be monitored and maintained
constant. To do this, the current
is converted to voltage by R8,
R11, R12, and U2b and is fed
back to the inverting terminal of
U1’s error amplifier. This negative
feedback adjusts the duty
cycle to maintain the current
through the LEDs. Varying R11
provides dimming of the LEDs.
Op-amp U2a and R9, R13,
R14, and R15 monitor the battery
voltage and switch off the
LEDs whenever the battery voltage
falls below 11 V, thereby
preventing deep discharge of
the battery.
See associated figure
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