19-0821; Rev 0; 5/07
MAX16809 Evaluation Kit
The MAX16809 evaluation kit (EV kit) is a 16-channel,
constant-current LED driver, capable of driving 40mA
each to 16 LED strings with a total forward voltage of
up to 32V. The MAX16809 EV kit is based on the
MAX16809 device, which has 16 constant-current-sinking outputs with sink current settable using a single
resistor and a high-performance, current-mode pulsewidth-modulator (PWM) controller, for implementing a
DC-DC converter that generates the supply voltage to
drive the LED strings.
The MAX16809 EV kit operates at supply voltages
between 9V to 16V and temperatures ranging from
0°C to +70°C. It features a PWM dimming control,
adaptive control of the LED supply voltage, which
depends upon the operating voltage of the LED strings,
a built-in clock generator, and a low-current shutdown.
The MAX16809 EV kit is a fully assembled and tested
board.
Features
♦ 9V to 16V Supply Voltage Range
♦ 40mA LED Current (Per Each LED String)
♦ Single-Resistor Current Adjust for 16 Channels
♦ Up to 32V LED String Voltage
♦ Boost Converter to Generate LED Supply Voltage
♦ Adaptive LED Supply Voltage Control Increases
Efficiency
♦ PWM Dimming Control
♦ Output-Voltage-Spike Protection for InductiveOutput Lines
♦ Proven PCB Layout
Ordering Information
PART
TEMP RANGE
IC PACKAGE
MAX16809EVKIT+
0°C to +70°C*
38 TQFN-EP†
+Denotes a lead-free and RoHS-compliant EV kit.
*This limited temperature range applies to the EV kit PCB only.
The MAX16809 IC temperature range is -40°C to +125°C.
†EP = Exposed paddle.
Component List
DESIGNATION
C1–C4, C6, C7,
C8, C10, C11,
C19–C23, C25,
C26
C5, C24, C30,
C31, C33
C9
C12, C13, C14
C15
QTY
DESCRIPTION
DESIGNATION
QTY
C16, C17, C18
3
22µF ±20%, 50V electrolytic
capacitors
Panasonic EEEFK1H220P
1
560pF ±10%, 50V C0G capacitor
(0603)
KEMET C0603C561K5RACTU
Murata GRM188R71H561KA01D
1
10pF ±10%, 50V C0G capacitor
(0603)
TDK C1608C0G1H00DB
Murata GRM1885C1H100JA01D
1
220pF ±10%, 50V C0G capacitor
(0603)
KEMET C0603C221K5RACTU
Murata GRM188R71H221KA01D
1
100pF ±10%, 50V C0G capacitor
(0603)
KEMET C0603C101K5RACTU
Murata GRM188R71H101KA01D
16
1nF ±10%, 50V X7R capacitors
(0603)
Murata GRM188R71H103KA01D
KEMET C0603C103K5RACTU
C27
5
0.1µF ± 10%, 50V X7R capacitors
(0603)
Murata GRM188R71H104KA93D
TDK C1608X7R1H104K
C28
1
1µF ±20%, 16V X7R capacitor
(0805)
Murata GRM21BR71C105KA01L
TDK C2012X7R1C105K
3
22µF ±20% 35V electrolytic
capacitors
Panasonic EEEFK1V220R
1
1µF ±20%, 50V X7R capacitor
(1210)
KEMET C3225X7R1H105M
Murata GRM32ER71H105KA01L
C29
C32
DESCRIPTION
________________________________________________________________ Maxim Integrated Products
For pricing, delivery, and ordering information, please contact Maxim/Dallas Direct! at
1-888-629-4642, or visit Maxim’s website at www.maxim-ic.com.
1
Evaluates: MAX16809
General Description
MAX16809 Evaluation Kit
Evaluates: MAX16809
Component List (continued)
DESIGNATION
QTY
C34
1
C35
D1
D2
D3–D10
D11
10nF ±10%, 50V X7R capacitor
(0603)
KEMET C0603C103K5RACTU
Murata GRM188R71H103KA01D
0
Not installed, capacitor
1
33V zener diode (SOD323)
Diodes Inc. MMSZ5257BS-7
DESCRIPTION
Q2
1
60V, 5.5A N-channel MOSFET
Vishay Si4450DY
R1
1
430Ω ±1% resistor (0603)
R2
1
330kΩ ±1% resistor (0603)
8.45kΩ ±1% resistor (0603)
R3
1
R4, R6, R10
3
22kΩ ±1% resistors (0603)
R5
1
180kΩ ±1% resistor (0603)
R7
1
10.5kΩ ±1% resistor (0603)
R8
1
10Ω ±1% resistor (0603)
R9
1
1.2kΩ ±1% resistor (0603)
8
15V dual zener diodes (SOT323)
Diodes AZ23C15-7-F
R10
1
22kΩ ±1% resistor (0603)
R11
1
50kΩ ±1% resistor (0603)
20mA switching diode (SOD323)
Diodes Inc. 1N4148WS-7
R12
1
75mΩ ±1% resistor (0603)
R13
0
Not installed, resistor
40V small-signal Schottky diode
(SOD523)
Diodes Inc. SDM03U40
R14
1
2.2kΩ ±1% resistor (0603)
R15
1
10kΩ ±1% resistor (0603)
U1
1
MAX16809ATU+ (38-pin TQFN,
5mm x 7mm)
U2
1
Digital pnp transistor
ROHM DTA114WKA
U3
1
Digital npn transistor
ROHM DTC114WKA
U4
1
Dual inverter with hysteresis
Texas Instruments
SN74LVC2G14DCKR
—
1
PCB: MAX16809 Evaluation Kit+
GND, GND,
PWM, SHDN,
VBIAS, VIN
6
J1
1
0.1in 20-pin header
1
27µH, 3.2A inductor
Coilcraft MSS1260-273ML
1
Switching transistor (SOT523)
Diodes Inc. MMBT2222AT-7-F
Q1
QTY
1A, 40V Schottky diode (SMA)
Diodes Inc. CMSH1-40M
Central Semiconductor CMSH1-40M
1
L1
DESIGNATION
1
1
D12
DESCRIPTION
Wire loops
Component Suppliers
SUPPLIER
PHONE
FAX
WEBSITE
Central Semiconductor Corp.
631-435-1110
631-435-3388
www.centralsemi.com
Coilcraft, Inc.
847-639-6400
847-639-1469
www.coilcraft.com
Diodes Inc.
805-446-4800
805-446-4850
www.diodes.com
KEMET Corp.
978-658-1663
978-658-1790
www.kemet.com
Murata Mfg. Co., Ltd.
770-436-1300
770-436-3030
www.murata.com
ROHM Co., Ltd.
858-625-3630
858-625-3670
www.rohm.com
TDK Corp.
847-390-4373
847-390-4428
—
—
402-563-6866
402-563-6296
Texas Instruments Inc.
Vishay
www.component.tdk.com
www.ti.com
www.vishay.com
Note: Indicate that you are using the MAX16809 when contacting these component suppliers.
2
_______________________________________________________________________________________
MAX16809 Evaluation Kit
Recommended Equipment
• One 16V, 5A adjustable power supply
• One 5V power supply
• 16 LED strings with a total forward voltage ≤ 32V
• One multimeter
• One PWM signal generator (optional)
Procedure
The MAX16809 EV kit is fully assembled and tested.
Follow the steps below to verify operation. Caution: Do
not turn on the power supply until all connections
are completed.
1) Connect LED strings with operating voltage of
approximately 32V between VLED (pins 1-4 of J1)
and OUT0–OUT15 (pins 5-20 of J1). All 16 channels
should have an LED string load connected of the
same type.
2) Connect the DC power supply (16V, 5A) to VIN and
GND.
3) Connect a DC power supply (0 to 5V) to VBIAS and
GND.
4) Turn on the power supplies and apply 10V to VIN
and 3V to 5V to VBIAS. Connect SHDN and PWM to
3V to 5V. All of the LEDs should turn on. Measure
the current through any LED string, which should be
40mA ±7%.
5) Increase the supply voltage to 16V and the LED
currents will be stable. Measure the current through
any LED string, which should be 40mA ±7%.
6) Apply a PWM signal with amplitude of 3V to 5V and
a frequency between 100Hz and 2kHz to the PWM
input. The LED brightness should increase as the
PWM duty cycle increases and viceversa.
7) Connect SHDN to GND and all LEDs should turn off.
Detailed Description
The MAX16809 EV kit is a 16-channel, constant-current
LED driver capable of driving 40mA each to 16 LED
strings, with a total forward voltage of up to 32V. The
MAX16809 EV kit can drive a total of 160 white LEDs in
16 strings, with operating current up to 40mA. The
MAX16809 EV kit can operate at input supply voltages
between 9V and 16V.
The MAX16809 EV kit evaluates the MAX16809 IC, which
has two major sections. The first section consists of 16
constant-current LED drivers capable of sinking up to
55mA when on and blocking up to 36V when off. The second section is a high-performance current-mode PWM
controller that can control a DC-DC converter to generate
the supply voltage for driving the LED strings. The
MAX16809 EV kit uses the PWM controller to drive a
boost converter, which takes a 9V to 16V input and generates a 33V LED supply voltage. To drive a constant current into an LED string, connect the LED string between
the 33V output and any of the 16 constant-current-sink
outputs. The resistor (R1) from the SET pin to ground programs the sink current of each output. The sink current of
any output can be up to 55mA and the amplitude is the
same value for all the outputs. The difference between the
total forward voltage and the LED supply voltage drops
between the constant-current-sink output and ground,
and is dissipated as power in the device.
The LED supply voltage generated by the boost converter in the MAX16809 EV kit is adaptive. The LED
string with the highest total forward voltage dominates
the control loop, and the boost-converter voltage is
adjusted so that the driver associated with that string
receives just enough voltage required for current drive.
All the other strings, with lower total forward voltages,
will have excess supply voltage, which is then dropped
in the associated driver. This feedback mechanism
ensures that the linear-current-control circuit dissipates
the minimum possible power. An on-board inverter
(U4A) is configured to generate the clock input for the
MAX16809. The constant-current output-driver circuits
and U4 need a 3.3V to 5V input, which should be supplied externally. If 5V is not available, it can be generated using an emitter-follower buffer from the REF output
of MAX16809.
Boost Converter
The boost converter that generates the 33V LED supply
voltage operates at a switching frequency of 350kHz in
continuous-conduction mode (CCM). The current-mode
PWM controller in the MAX16809 drives the external
MOSFET (Q2) to control the boost converter. The
MOSFET is turned on at the beginning of every switching
cycle and turned off when the current through the inductor (L1) reaches the peak value set by the error-amplifieroutput voltage. Inductor current is sensed from the voltage across the ground-referenced current-sense resistor (parallel combination of R12 and R13). This currentsense information is passed on to the current-sense
comparators in the MAX16809 through the CS pin.
During the on period of the MOSFET, the inductor
stores energy from the input supply. When the switch is
turned off, the inductor generates sufficient voltage in
reverse direction to discharge the stored energy to
VLED. This generated voltage forms a source, in series
with the input supply voltage, and drives VLED through
the rectifier diode (D2).
_______________________________________________________________________________________
3
Evaluates: MAX16809
Quick Start
Evaluates: MAX16809
MAX16809 Evaluation Kit
As the boost converter is operated in CCM, only part of
the stored energy in the inductor is discharged to VLED.
The advantages of CCM include reduced input and output filtering, reduced EMI due to lower peak currents,
and higher converter efficiency. However, these advantages come at the cost of a right-half-plane zero in the
converter-transfer function. Compensating this zero
requires reducing the system bandwidth, which affects
the converter-dynamic response. As the 16-channel,
constant-current-sink outputs control the current through
the LEDs, slower control of VLED does not affect the
LED operation. Compensation of the feedback circuit is
explained in the Feedback Compensation section.
An internal comparator turns off the gate pulse to the
external MOSFET if the voltage at the CS pin exceeds
0.3V. The current through the inductor that produces
0.3V at the CS pin is the maximum inductor current
possible (the actual current can be a little higher than
this limit due to the 60ns propagation delay from the CS
pin to the MOSFET drive output). This condition can
happen when the feedback loop is broken, when the
output capacitor charges during power-up, or when
there is an overload at the output. This feature protects
the MOSFET by limiting the maximum current passing
through it during such conditions.
The RC filter, consisting of R9 and C10, removes the
voltage spike across the current-sense resistors produced by the turn-on gate current of the MOSFET and
the reverse-recovery current of D2. Without filtering,
these current spikes can cause sense comparators to
falsely trigger and turn off the gate pulse prematurely.
The filter time constant should not be higher than
required (the MAX16809 EV kit uses a 120ns time constant), as a higher time constant adds additional delay
to the current-sense voltage, effectively increasing the
current limit.
During normal operating conditions, the feedback loop
controls the peak current. The error amplifier compares
a scaled-down version of the LED supply voltage
(VLED) with a highly accurate 2.5V reference. The error
amplifier and compensation network then amplify the
error signal, and the current comparator compares this
signal to the sensed-current voltage to create a PWM
drive output.
Power-Circuit Design
Initially, decide the input supply voltage range, output
voltage VLED (the sum of the maximum LED total forward voltage and 1V bias voltage for the constant-current-sink output), and the output current IOUT (the sum
of all the LED string currents).
4
Calculate maximum duty cycle DMAX using the following
equation:
DMAX =
VLED + VD − VINMIN
VLED + VD − VFET
where VD is the forward drop of the rectifier diode D2
(~0.6V), VINMIN is the minimum input supply voltage (in
this case, 9V), and VFET is the average drain-to-source
voltage of the MOSFET Q2 when it is on.
Select the switching frequency F SW based on the
space, noise, dynamic response, and efficiency constraints. Select the maximum peak-to-peak ripple on
the inductor current ILPP. For the MAX16809 EV kit,
FSW is 350kHz and ILPP is ±30% of the average inductor current. Use the following equations to calculate the
maximum average-inductor current ILAVG and peak
inductor current ILPEAK:
IL AVG =
IOUT
1− DMAX
Since ILPP is ±30% of the average-inductor current
ILAVG:
ILPP = IL AVG × 0.3 × 2
ILPEAK = IL AVG +
ILPP
2
Calculate the minimum inductance value LMIN with the
inductor current ripple set to the maximum value:
LMIN =
(VINMIN − VFET ) × DMAX
FSW × ILPP
Choose an inductor that has a minimum inductance
greater than this calculated value.
Calculate the current-sense resistor (R12 in parallel
with R13) using the equation below:
RCS =
0.3 × 0.75
ILPEAK
where 0.3V is the maximum current-sense signal voltage. The factor 0.75 is for compensating the reduction
of maximum current-sense voltage due to the addition
of slope compensation. Check this factor and adjust
after the slope compensation is calculated. See the
Slope Compensation section for more information.
_______________________________________________________________________________________
MAX16809 Evaluation Kit
The continuous drain-current rating of the selected
MOSFET when the case temperature is at +70°C should
be greater than that calculated by the following equation.
The MOSFET must be mounted on a board, as per
manufacturer specifications, to dissipate the heat:
IL SAT = 1.1 × ILPEAK
Calculate the output capacitor COUT (parallel combination of C16, C17, C18, and C24) using the following
equation:
COUT =
DMAX × IOUT
VLEDPP × FSW
where VLEDPP is the peak-to-peak ripple in the LED
supply voltage. The value of the calculated output
capacitance will be much lower than what is actually
necessary for feedback loop compensation. See the
Feedback Compensation section to calculate the output capacitance based on the compensation requirements.
Calculate the input capacitor CIN (parallel combination
of C12, C13, C14, and C5) using the following equation:
ILPP
CIN =
8 × FSW × VINPP
where VINPP is the peak-to-peak input ripple voltage.
This equation assumes that input capacitors supply
most of the input ripple current.
Selection of Power Semiconductors
The switching MOSFET (Q2) should have a voltage rating sufficient to withstand the maximum output voltage,
together with the diode drop of D2, and any possible
overshoot due to ringing caused by parasitic inductances and capacitances. Use a MOSFET with voltage
rating higher than that calculated by the following
equation:
VDS = (VLED + VD ) ×1.3
The factor of 1.3 provides a 30% safety margin.
⎛
⎞
IL AVG2
⎟ × 1.3
IDRMS = ⎜
⎜ DMAX ⎟
⎝
⎠
The MOSFET dissipates power due to both switching
losses, as well as conduction losses. Use the following
equation to calculate the conduction losses in the
MOSFET:
PCOND =
IL AVG2
× RDSON
DMAX
where RDSON is the on-state drain-source resistance of
the MOSFET with an assumed junction temperature of
100°C.
Use the following equation to calculate the switching
losses in the MOSFET:
PSW =
1 ⎞
IL AVG × VLED2 × CGD × FSW ⎛ 1
×⎜
+
⎟
2
⎝ IGON IGOFF ⎠
where IGON and IGOFF are the gate currents of the
MOSFET (with V GS equal to the threshold voltage)
when it is turned on and turned off, respectively, and
CGD is the gate-to-drain MOSFET capacitance. Choose
a MOSFET that has a higher power rating than that calculated by the following equation when the MOSFET
case temperature is at +70°C:
PTOT = PCOND + PSW
The MAX16809 EV kit uses a Schottky diode as the
boost-converter rectifier (D2). A Schottky rectifier diode
produces less forward drop and puts the least burden
on the MOSFET during reverse recovery. If a diode with
considerable reverse-recovery time is used, it should be
considered in the MOSFET switching-loss calculation.
The Schottky diode selected should have a voltage rating 20% above the maximum boost-converter output
voltage. The current rating of the diode should be
greater than ID in the following equation:
⎛
IL AVG2
ID = ⎜
⎜ 1− DMAX
⎝
⎞
⎟ × 1.2
⎟
⎠
_______________________________________________________________________________________
5
Evaluates: MAX16809
The saturation current limit of the selected inductor
(ILSAT) should be greater than the value given by the
equation below. Selecting an inductor with 10% higher
ILSAT rating is a good choice:
Evaluates: MAX16809
MAX16809 Evaluation Kit
Slope Compensation
When the boost converter operates in CCM with more
than 50% duty cycle, subharmonic oscillations occur if
slope compensation is not implemented. Subharmonic
oscillations do not allow the PWM duty cycle to settle to
a peak current value set by the voltage-feedback loop.
The duty cycle oscillates back and forth about the
required value, usually at half the switching frequency.
Subharmonic oscillations die out if a sufficient negative
slope is added to the inductor peak current. This
means that for any peak current set by the feedback
loop, the output pulse terminates sooner than normally
expected. The minimum slope compensation that
should be added to stabilize the current loop is half of
the worst-case (max) falling slope of inductor current.
Adding a ramp to the current-sense signal, with positive slope in sync with the switching frequency, can
produce the desired function. The greater the duty
cycle, the greater the added voltage, and the greater
the difference between the set current and the actual
inductor current. In the MAX16809 EV kit, the oscillator
ramp signal is buffered using Q1 and added to the current-sense signal with proper scaling to implement the
slope compensation. Follow the steps below to calculate the component values for slope compensation.
Calculate the worst-case falling slope of the inductor
current using the following equation:
IL SLOPE =
(VLEDMAX + VD − VINMIN )
LMIN
From the inductor current falling slope, find its equivalent voltage slope across the current-sense resistor RCS
(R12 parallel with R13) using the following equation:
VSLOPE = IL SLOPE × RCS
The minimum voltage slope that should be added to
the current-sense waveform is half of VSLOPE for ensuring stability up to 100% duty cycle. As the maximum
continuous duty cycle used is less than 100%, the minimum required compensation slope becomes:
V
× (2DMAX − 1) × 1.1
VCSLOPE = SLOPE
DMAX
The factor 1.1 provides a 10% margin. Resistors R9
and R10 determine the attenuation of the buffered voltage slope from the emitter of Q1. The forward drop of
6
signal diode D11, together with the VBE of Q1, almost
cancel the 1.1V offset of the ramp waveform. Calculate
the approximate slope of the oscillator ramp using the
following equation:
VRSLOPE = 1.7 × FSW
where 1.7V is the ramp amplitude and F SW is the
switching frequency.
Select the value of R9 such that the input bias current of
the current-sense comparators does not add considerable error to the current-sense signal. The value of R10
for the slope compensation is given by the equation:
⎛ VRSLOPE ⎞
R10 = ⎜
− 1⎟ × R9
⎝ VCSLOPE ⎠
LED Driver
The MAX16809 features a 16-channel, constant-current
LED driver, with each channel capable of sinking up to
55mA of LED current. The LED strings are connected
between VLED and the constant-current-sink outputs to
drive regulated current through LED strings. The current through all 16 channels is controlled through resistor (R1) from the SET pin to ground. The MAX16809 EV
kit sets the current through each string at 40mA and the
maximum LED supply voltage to 33V. The MAX16809
EV kit drives LED strings with a total forward voltage of
up to 32V.
A 4-wire serial interface with four inputs (DIN, CLK, LE,
and OE) individually control the constant-current outputs. In the MAX16809 EV kit, a 50kHz clock signal,
generated by U4A, clocks 16 1s into the internal shift
register by tying DIN and LE to 5V. The clock-generation
circuit can be avoided if a microcontroller provides the
function.
The output enable (OE) can provide PWM dimming. An
inverted PWM signal, generated by the inverter U4B, is
necessary to drive the OE pin. When the PWM signal is
low (LED drivers off), it also influences the feedback
with the network formed by R6 and D12. See the
Adaptive LED Supply Voltage Control section for more
details.
If an inverted PWM signal is available, use the circuit
shown in Figure1 to drive the OE input and feedback
network.
_______________________________________________________________________________________
MAX16809 Evaluation Kit
Evaluates: MAX16809
COMP
C28
10pF
R5
180kΩ
C29
220pF
VLED
R2
330kΩ
R11
50kΩ
D1
33V
R7
10.5kΩ
FB
3 D10
AZ23C15-7
3 D3
AZ23C15-7
R6
22kΩ
VBIAS
C30
0.1μF
5
4
3
U4B
R15
10kΩ
SN74LVC2G14
D12
SDM03U40
1
2
1
2
2
OUT0 OUT1
PWM
OUT14 OUT15
OEB
Figure 1. Inverting PWM Drive Circuit
Output Current Setting
The amplitude of the output sink currents for all 16
channels is set to the same value by the resistor (R1)
from the SET pin to ground. The minimum allowed
value of RSET is 311Ω, which sets the output currents to
55mA. The maximum allowed value of RSET is 5kΩ. The
MAX16809 EV kit uses 430Ω for RSET, which sets the
output current to 40mA. To set a different output current, use the following equation:
RSET =
17100
IOUT
where RSET is the current-setting resistor (R1) value in
ohms and IOUT is the desired output current in milliamps.
Adaptive LED Supply Voltage Control
To reduce power dissipation in the IC, the MAX16809
EV kit features adaptive control of VLED based on the
operating voltage of the LED strings. The constant-current-sink outputs can sink stable currents with output
voltages as low as 0.8V. The voltage at each of the 16
outputs will be the difference between VLED and the
total forward voltage of the LED string connected to
that output. The MAX16809 EV kit implements a feedback mechanism to sense the voltage at each of the 16
constant-current-sink outputs. Using dual zener diodes
(D3–D10), the MAX16809 EV kit selects the lowest driver voltage (with the greatest LED string voltage) to
regulate. The boost-converter PWM then adjusts so that
VLED is high enough for this sink output to settle to
approximately 0.8V. All the other strings have sufficient
voltage, as their total forward voltages are lower. The
feedback mechanism ensures that the IC dissipates the
minimum possible power. For adaptive control to function efficiently connect LED strings to all 16 channels
and use an equal number of LEDs from the same bin in
each string. If some of the 16 channels are not used,
then the zener diodes (D3–D10) should be removed
from the unused channels.
Use the equation below to calculate the value of R2 to
get the required minimum voltage at the sink outputs:
R2 =
(VFLED + VS − 2.5) × R7
2.5 − VDZ − VS
where 2.5V is the feedback reference, VDZ is the forward drop of the ORing diode (D3–D10), VS = 0.5V is
the required sink-output voltage, and VFLED is the nominal total forward voltage of the LED strings. Select the
value of R2 such that R7 is approximately 10kΩ.
The zener diodes (D3–D10) also provide output overvoltage protection. If an LED string gets partially or fully
shorted, making the sink-output voltage go high, the
15V zener diode connected to that output conducts in
reverse direction, and limits the VLED voltage. Under
this condition, the other LED strings might not turn on.
When the outputs are off, the LED drivers are at high
impedance and the feedback network now combines
R6 and D12 to provide a path for the feedback current
and to control VLED. Use the following equation to
_______________________________________________________________________________________
7
Evaluates: MAX16809
MAX16809 Evaluation Kit
calculate the value of R6 to get the required LED supply voltage during PWM off time:
R6 =
R2 × (2.5 - 0.4)
VLEDOFF - 2.5
where 2.5V is the feedback-reference voltage, 0.4V is
the total voltage dropped by D4 and PWM input, and
VLED OFF is the desired LED supply voltage during
PWM off time. VLEDOFF should be set to the worst-case
LED string voltage plus some additional headroom for
the LED drivers (0.8V), as well as a reserve voltage
(approximately 1V). The reserve voltage allows the
MAX16809 to provide current for very short PWM dimming on-pulses. With pulses as low as 2µs, the VLED
control loop is not able to react, and the output capacitors provide all the current. For longer PWM dimming
pulses, the control loop reacts and the supply operates
at the adaptive voltage level.
During an open LED condition, the 33V zener diode
(D1) limits the maximum LED supply voltage to 35.5V. If
VLED attempts to increase beyond this level, D1 conducts in reverse direction and pulls the FB pin high,
which causes the boost regulator to cut back on the
PWM signal and reduce the output voltage.
PWM Dimming
The PWM dimming controls the LED brightness by
adjusting the duty cycle of the PWM input signal. A
high voltage at the PWM input enables the output current; a low voltage turns off the output current. Connect
a signal with peak amplitude of 3V to 5V and with frequency from 100Hz to 2kHz to the PWM input and vary
the duty cycle to adjust the LED brightness. The LED
brightness increases when the duty cycle increases
and vice versa. If an inverted PWM signal is available,
use that signal to implement PWM dimming, as shown
in Figure 1.
Feedback Compensation
Like any other circuit with feedback, the boost converter that generates the supply voltage for the LED strings
needs to be compensated for stable control of its output voltage. As the boost converter is operated in continuous-conduction mode, there exists a right-halfplane (RHP) zero in the power-circuit transfer function.
This zero adds a 20dB/decade gain together with a 90degree phase lag, which is difficult to compensate. The
easiest way to avoid this zero is to roll off the loop gain
8
to 0dB at a frequency less than half of the RHP zero frequency with a -20dB/decade slope. For a boost converter, the worst-case RHP zero frequency (FZRHP) is
given by the following equation:
FZRHP =
VLED(1− DMAX )2
2π × L × IO
where DMAX is the maximum duty cycle, L is the inductance of the inductor, and I O is the output current,
which is the sum of all the LED string currents.
The boost converter used in the MAX16809 EV kit is
operated with current-mode control. There are two
feedback loops within a current-mode-controlled converter: an inner loop that controls the inductor current
and an outer loop that controls the output voltage. The
amplified voltage error produced by the outer voltage
loop is the input to the inner current loop that controls
the peak inductor current.
The internal current loop converts the double-pole 2ndorder system, formed by the inductor and the output
capacitor COUT, to a 1st-order system having a single
pole consisting of the output filter capacitor and the output load. As the output load is a constant current (i.e.,
very high Thevenin impedance), this pole is located near
the origin (0Hz). The phase lag created by the output
pole for any frequency will be 90 degrees. Since the
power-circuit DC gain is limited by other factors, the gain
starts falling at -20dB/decade from a non-zero frequency
before which the power-circuit gain stabilizes.
Total gain of the feedback loop at DC is given by the
following equation:
GTOT = GP × GEA × GFB
where GP is the power-circuit DC gain, and GEA is the
error-amplifier open-loop DC gain, typically 100dB. GFB
is the gain of the feedback network for adaptive control
of the VLED, which is seen from VLED to the erroramplifier input (FB pin). The adaptive control senses
the voltages at the 16 constant-current-sink outputs
and adjusts the feedback to control these voltages to a
minimum value (Figure 2). As the LEDs carry constant
current, the voltage across the LEDs does not change
with variations in VLED. Any change in VLED directly
reflects to the constant-current-sink outputs and to the
error-amplifier input, making GFB equal to unity.
_______________________________________________________________________________________
MAX16809 Evaluation Kit
GP =
ΔVLED
ΔEA OUT
Calculate the power-circuit DC gain using the following
equation:
1
GP =
2
⎛
VIN
I ⎞
+ O ⎟ × RCS × 3
⎜
2 V
IN ⎠
⎝ 2 × L × FSW × VLED
where RCS is the current-sense resistor, F SW is the
switching frequency, and the factor 3 is to account for
the attenuation of error-amp output before it is fed to
the current-sense comparator.
The power-circuit gain is lowest at the minimum input
supply voltage and highest at the maximum input supply voltage. Any input supply voltage between 9V and
16V can be used for power-circuit gain calculation, as
the final compensation values obtained are the same.
Calculate the frequency FP2, at which the power-circuit
gain starts falling, at -20dB/decade using the following
equation:
FP2 =
(1− DMAX )
2π × COUT × 3 × RCS × GP
where COUT is the output filter capacitor, which is the
parallel combination of C16, C17, C18, and C24. Adjust
the output capacitance so that the product of FP2 and
GP is below FZRHP / 6. The value of output capacitance
obtained this way will be much greater than the value
obtained using the maximum output voltage ripple
specification.
The compensation strategy is as follows. The gain-frequency response of the feedback loop should cross 0dB
at or below half of the RHP zero frequency, with a slope of
-20dB/decade for the feedback to be stable and have
sufficient phase margin. The compensation network from
COMP pin to FB pin of the MAX16809 (formed by R5,
C28, C29, and R11) offers one dominant pole (P1), a zero
(Z1), and a high-frequency pole (P3). There are two very
low frequency poles and a zero in the loop before the
crossover frequency. The function of the zero (Z1) is to
compensate for the output pole and to reduce the slope
of the loop gain from -40dB/decade to -20dB/decade,
and also to reduce the phase lag by 90 degrees.
Choose the crossover frequency to be half of the worstcase RHP zero frequency:
FC =
FZRHP
2
Place the zero (Z1) at one-third of the crossover frequency, so that the phase margin starts improving from
a sufficiently lower frequency:
FZ1 =
FC
3
Use the following equation to calculate the dominant
pole location, so that the loop gain crosses 0dB at FC:
FP1 =
FZRHP × FZ1
2 × GTOT × FP2
Since the open-loop gain of the error amplifier can have
variations, the dominant pole location can also vary
from device to device. In the MAX16809 EV kit, the
dominant pole location is decided by the error-amplifier
gain, so the combined effect is a constant-gain-bandwidth product.
Select the value of R11 such that the input bias current
of the error amplifier does not cause considerable drop
across it. The effective AC impedance seen from the
FB pin is the sum of R11 and R7. It is preferable to
keep R7 much lower, compared to R11, to have better
control on the AC impedance. Find C29 using the following equation:
C29 =
1
2π × GEA × (R11+ R7) × FP1
The location of the zero (Z1) decided by R5 and C29 is
given by the following equation:
FZ1 =
1
2π × R5 × C29
Place the high-frequency pole (P3), formed by C28,
C29, and R5, at half the switching frequency to provide
further attenuation to any high-frequency signal propagating through the system. The location of the high-frequency pole (FP3) is given by the following equation,
and should be used to calculate the value of C28:
FP3 =
1
1 ⎞
⎛ 1
+
2π × R5 × ⎜
⎟
⎝ C28 C29 ⎠
−1
_______________________________________________________________________________________
9
Evaluates: MAX16809
The DC gain of the power circuit is expressed as the
change in the output voltage, with respect to the
change in error-amplifier output voltage. As the boost
converter in the MAX16809 EV kit drives a constantcurrent load, the power-circuit DC gain is calculated
based on a constant-current load:
Evaluates: MAX16809
MAX16809 Evaluation Kit
The MAX16809 EV kit uses electrolytic capacitors at the
output for filtering, so the zero produced by the ESR of
the capacitors can be low enough to be within or near
the crossover frequency. This zero should be compensated using an additional pole (P4) placed at the ESR
zero location. The ESR zero frequency is calculated
using the following equation:
1
FZESR =
2π × ESR × COUT
Use the following equation to calculate the value of C35
to place the pole (P4) at the ESR zero frequency:
1
C35 =
2π × FZESR × R7
If ceramic capacitors are used at the output for filtering,
the frequency of zero produced by the ESR and the
capacitance will be above the crossover frequency
(0dB gain frequency) of the feedback loop and need
not be considered in the compensation design.
Layout Considerations
LED driver circuits based on the MAX16809 device use
a high-frequency switching converter to generate the
supply voltage for LED strings. Proper care must be
taken while laying out the circuit to ensure proper operation. The switching-converter part of the circuit has
nodes with very fast voltage changes, producing highfrequency electric fields, and branches with fast current
changes, producing high-frequency magnetic fields. As
the circuit converts power, the amplitude of these fields
will be high and can easily couple to sensitive parts of
the circuit, creating undesirable effects. Follow the
guidelines below to reduce noise as much as possible:
1) Connect the bypass capacitors from REF and VCC
as close as possible to the device and connect the
capacitor grounds to the analog ground plane
using vias close to the capacitor terminals. Connect
the AGND pin of the device to the analog ground
plane using a via close to the pin. Lay the analog
ground plane on the inner layer, preferably next to
the top layer. Use the analog ground plane to cover
the entire area under critical-signal components for
the power converter.
2) Keep the oscillator timing capacitor and resistor
very close to the RTCT pin and make the connection as short as possible. Connect the ground of the
timing capacitor to the analog ground plane using a
via close to the capacitor terminal. Make sure that
no switching node is present near the RTCT node
and keep the area of the copper connected to the
pin small. Keep the REF connection to the timing
resistor short and away from any switching node.
10
3) Have a power ground plane for the switching-converter power circuit under the power components
(input filter capacitor, output filter capacitor, inductor,
MOSFET, rectifier diode, and current-sense resistor).
Connect all the ground connections to the power
ground plane using vias close to the terminals.
4) There are two loops in the power circuit that carry
high-frequency switching currents. One loop is
when the MOSFET is on (from the input filter capacitor positive terminal, through the inductor, the
MOSFET, and the current-sense resistor, to the
input capacitor negative terminal). The other loop is
when the MOSFET is off (from the input capacitor
positive terminal, through the inductor, the rectifier
diode, and the output filter capacitor, to the input
capacitor negative terminal). Analyze these two
loops and make the loop areas as small as possible. Wherever possible, have a return path on the
power ground plane for the switching currents on
the top-layer copper tracks, or through power components. This reduces the loop area considerably
and provide a low inductance path for the switching
currents. Reducing the loop area also reduces radiation during switching.
5) The gate-drive current of the MOSFET is another
high-frequency switching current to consider. There
are two major loops: one during the MOSFET turn-on
edge and the second during the turn-off edge. The
MOSFET turn-on loop is from the VCC bypass
capacitor positive terminal, through the MOSFET driver in the device, the gate-drive resistor, the MOSFET gate to source (CGS and CGD), and the currentsense resistor to the VCC bypass capacitor negative
terminal. There is no direct path for the current from
the current-sense resistor to return to the VCC
bypass capacitor through the ground plane, as the
VCC bypass capacitor is connected to the analog
ground plane and the current-sense resistor is connected to the power ground plane. The best solution
is to connect the analog ground plane to the power
ground plane directly under the MOSFET gate-drive
track. This ensures that the turn-off current also has a
return path on the ground plane.
6) The drain node of the MOSFET is a switching node.
Keep this node area small to reduce radiation and
capacitive coupling to other sensitive parts of the
circuit. However, the track should be wide enough
to carry the large switching currents.
7) Keep the node area and track length on the FB pin
small to reduce any noise pickup.
______________________________________________________________________________________
MAX16809 Evaluation Kit
Power Dissipation
The MAX16809 dissipates power during normal operating conditions. The heat transferred to the exposed pad
from the die should be properly dissipated to the board
to prevent the device from entering into thermal shutdown. The exposed pad land area on the top layer
should be of the same size as that of the exposed pad.
Thermal vias are used to carry the heat from the
exposed pad to other layers of the board and spread it
across the board area through copper planes. Thermal
vias should have a 0.4mm hole size and should be
placed at a distance of 1mm from center to center. For
a four-layer board, these vias should be connected to
the bottom ground plane and to one internal ground
plane. Do not use thermal relief for the thermal vias;
instead, use solid copper to get the minimum thermal
resistance.
Use the following equation to calculate the total power
dissipated in the MAX16809 device during normal
operation:
PD =
∑ VSN × IN + IB × VIN
N = 0 − 15
where IN is the LED current in channel N, VS is the
operating voltage of each of the LED driver outputs with
respect to GND pins, IB is the input bias current of
MAX16809 including the average of MOSFET drive current, and VIN is the input supply voltage. To dissipate
1W of power, the exposed pad of the device should be
connected to a minimum of two square inches of copper ground plane with 70µ copper thickness.
______________________________________________________________________________________
11
Evaluates: MAX16809
8) Connect the power ground plane for the constantcurrent LED driver part of the circuit to the boostconverter output filter capacitor negative terminal.
12
G2
SHDN
PWM
GND
VBIAS
GND
VIN
VBIAS
C12
22μF
35V
C13
22μF
35V
VIN
C14
22μF
35V
EEEFK1V220R
R12
75mΩ
1%
R13
OPEN
3 2 1
Q2
Si4450DY
5 6 7 8
C15
1μF
50V
4
C32
100pF
R9
1.2kΩ
1%
R4
22kΩ
R8 1%
10Ω
1%
D2
CMSH1-40M
C17
22μF
50V
C34
10nF
R10
22kΩ
1%
D11
1N4148
2
1
C18
22μF
50V
2
-
5 +
C27
560pF
R3
8.45kΩ
1%
1
U4A
R14
2.2kΩ
1%
Q1
MMBT2222
C16
22μF
50V
EEEFK1H220P
C24
L1
0.1μF
27μH
50V
MSS1278
G1
G1
SN74LVC2G14
6
23
OUT2
26
27
28
OUT5
OUT6
OUT7
R15
10kΩ
1%
31
30
29
25
OUT4
24
22
OUT3
21
OUT1
20
OUT0
CLK
C33
0.1μF
VLED
18
17
16
15
14
G1
13
U1
MAX16809
2
5
32
-
+
33
36
C30
0.1μF
35
SN74LVC2G14
4
34
OEB
37
OE
G2
G1
1
2
3
4
5
6
7
8
9
VIN
OUT8
OUT9
OUT10
OUT11
OUT12
OUT13
10 OUT14
11 OUT15
12
EP
C31
0.1μF
38
N.C.
FB
COMP
OUT8
OUT9
OUT10
OUT11
OUT12
OUT13
OUT14
OUT15
N.C. AGND OUT VCC N.C. REF N.C.
3
U4B
N.C.
CS
RTCT
OUT7
OUT6
OUT5
OUT4
OUT3
OUT2
OUT1
OUT0
LE
EP
R1
430Ω
1%
CLK DIN PGND PGND V+ SET DOUT
19
CLK
OUT
C9
1μF
GND 1
OUT
3
IN 2
U2
C35
OPEN
VLED
DTA114WKA
G1
VBIAS
R5
180kΩ
1%
R11
C29
50kΩ
220pF 1%
OE
DTC114WKA
2 IN
U3
1 GND
3
C28
10pF
C5
0.1μF
D12
SDM03U40
R6
22kΩ
1%
R2
330kΩ
1%
R7
10.5kΩ
1%
D1
33V
1
2
2
1
1
2
2
1
1
2
3 D6
AZ23C15-7
6
1
2
3
4
5
9
AZ23C15-7
D8
AZ23C15-7
D9
AZ23C15-7
D10
20
AZ23C15-7
D7
19
OUT8
18
17
16
15
14
13
12
OUT9
OUT10
OUT11
OUT12
OUT13
OUT14
OUT15
OUT0
11
OUT2
OUT1
10
OUT3
8
2
1
3 D5
AZ23C15-7
C23
1nF
C6
1nF
C1
1nF
7
1
2
3 D4
AZ23C15-7
C26
1nF
C22
1nF
C11
1nF
C8
1nF
C3
1nF
OUT4
2
1
C25
1nF
3 D3
AZ23C15-7
C20
1nF
C21
1nF
C19
1nF
C10
1nF
C7
1nF
C2
1nF
OUT5
OUT6
OUT7
OUT0
OUT1
OUT2
OUT3
OUT4
OUT5
OUT6
OUT7
OUT8
OUT9
OUT10
OUT11
OUT12
OUT13
OUT14
OUT15
VLED
VLED
J1A
C4
1nF
Evaluates: MAX16809
MAX16809 Evaluation Kit
Figure 2. MAX16809 EV Kit Schematic
______________________________________________________________________________________
MAX16809 Evaluation Kit
Evaluates: MAX16809
Figure 3. MAX16809 EV Kit Component Placement Guide—Component Side
______________________________________________________________________________________
13
Evaluates: MAX16809
MAX16809 Evaluation Kit
Figure 4. MAX16809 EV Kit PCB Layout—Component Side
14
______________________________________________________________________________________
MAX16809 Evaluation Kit
Evaluates: MAX16809
Figure 5. MAX16809 EV Kit PCB Layout—Inner Layer 1
______________________________________________________________________________________
15
Evaluates: MAX16809
MAX16809 Evaluation Kit
Figure 6. MAX16809 EV Kit PCB Layout—Inner Layer 2
16
______________________________________________________________________________________
MAX16809 Evaluation Kit
Evaluates: MAX16809
Figure 7. MAX16809 EV Kit PCB Layout—Solder Side
Maxim cannot assume responsibility for use of any circuitry other than circuitry entirely embodied in a Maxim product. No circuit patent licenses are
implied. Maxim reserves the right to change the circuitry and specifications without notice at any time.
Maxim Integrated Products, 120 San Gabriel Drive, Sunnyvale, CA 94086 408-737-7600 ____________________ 17
© 2007 Maxim Integrated Products
is a registered trademark of Maxim Integrated Products, Inc.