TI LM3445

LM3445
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SNVS570L – JANUARY 2009 – REVISED MAY 2013
Triac Dimmable Offline LED Driver
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FEATURES
DESCRIPTION
•
•
•
The LM3445 is an adaptive constant off-time AC/DC
buck (step-down) constant current controller designed
to be compatible with triac dimmers. The LM3445
provides a constant current for illuminating high
power LEDs and includes a triac dim decoder. The
dim decoder allows wide range LED dimming using
standard triac dimmers. The high frequency capable
architecture allows the use of small external passive
components. The LM3445 includes a bleeder circuit
to ensure proper triac operation by allowing current
flow while the line voltage is low to enable proper
firing of the triac. A passive PFC circuit ensures good
power factor by drawing current directly from the line
for most of the cycle, and provides a constant positive
voltage to the buck regulator. Additional features
include thermal shutdown, current limit and VCC
under-voltage lockout.
1
2
•
•
•
•
•
•
•
Triac Dim Decoder Circuit for LED Dimming
Application Voltage Range 80VAC – 277VAC
Capable of Controlling LED Currents Greater
Than 1A
Adjustable Switching Frequency
Low Quiescent Current
Adaptive Programmable Off-Time Allows for
Constant Ripple Current
Thermal Shutdown
No 120Hz Flicker
Low Profile 10-Pin VSSOP Package or 14-Pin
SOIC
Patent Pending Drive Architecture
APPLICATIONS
•
•
•
•
Retro Fit Triac Dimming
Solid State Lighting
Industrial and Commercial Lighting
Residential Lighting
Typical LM3445 LED Driver Application Circuit
C7
+
14 Series connected LEDs
D9
BR1
C10
D8
R2
C9
D4
+
C12
Q1
TRIAC
DIMMER
95.0
VBUCK
D3
VLED
-
VLED-
D2
VAC
D1
D10
R5
Q3
C5
L2
90.0
R4
EFFICIENCY (%)
V+
85.0
10 Series connected LEDs
80.0
LM3445MM
1 ASNS
U1
BLDR 10
ICOLL
R1
2 FLTR1
C3
VCC 9
75.0
80
90
100
110
120
130
140
LINE VOLTAGE (VAC)
3 DIM
GATE 8
4 COFF
ISNS 7
5 FLTR2
GND 6
Q2
R3
C4
C11
1
2
Please be aware that an important notice concerning availability, standard warranty, and use in critical applications of
Texas Instruments semiconductor products and disclaimers thereto appears at the end of this data sheet.
All trademarks are the property of their respective owners.
PRODUCTION DATA information is current as of publication date.
Products conform to specifications per the terms of the Texas
Instruments standard warranty. Production processing does not
necessarily include testing of all parameters.
Copyright © 2009–2013, Texas Instruments Incorporated
LM3445
SNVS570L – JANUARY 2009 – REVISED MAY 2013
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DEVICE INFORMATION
(1)
ORDER NUMBER (1)
TOP MARK
LM3445M/NOPB
SULB
LM3445MM/NOPB
SULB
LM3445MMX/NOPB
LM3445M
LM3445MX/NOPB
LM3445M
For the most current package and ordering information, see the Package Option Addendum at the end of this document, or see the TI
web site at www.ti.com.
Connection Diagram
Top View
Top View
COFF
1
14 DIM
N/C
2
13 FLTR1
FLTR2
3
12 ASNS
7 ISNS
GND
4
11 N/C
6 GND
N/C
5
10 BLDR
N/C
6
9 VCC
ISNS
7
8 GATE
ASNS
1
10 BLDR
FLTR1
2
9 VCC
DIM
3
8 GATE
COFF
4
FLTR2
5
Figure 1. 10-Pin VSSOP
Package Number DGS
Figure 2. 14-Pin SOIC
Package Number D
PIN DESCRIPTIONS
2
SOIC
VSSOP
Name
Description
12
1
ASNS
PWM output of the triac dim decoder circuit. Outputs a 0 to 4V PWM signal with a duty cycle
proportional to the triac dimmer on-time.
13
2
FLTR1
First filter input. The 120Hz PWM signal from ASNS is filtered to a DC signal and compared to a 1 to
3V, 5.85 kHz ramp to generate a higher frequency PWM signal with a duty cycle proportional to the
triac dimmer firing angle. Pull above 4.9V (typical) to tri-state DIM.
14
3
DIM
1
4
COFF
OFF time setting pin. A user set current and capacitor connected from the output to this pin sets the
constant OFF time of the switching controller.
3
5
FLTR2
Second filter input. A capacitor tied to this pin filters the PWM dimming signal to supply a DC voltage
to control the LED current. Could also be used as an analog dimming input.
4
6
GND
Circuit ground connection.
7
7
ISNS
LED current sense pin. Connect a resistor from main switching MOSFET source, ISNS to GND to set
the maximum LED current.
8
8
GATE
Power MOSFET driver pin. This output provides the gate drive for the power switching MOSFET of the
buck controller.
9
9
VCC
10
10
BLDR
2,5,6,11
-
N/C
Input/output dual function dim pin. This pin can be driven with an external PWM signal to dim the
LEDs. It may also be used as an output signal and connected to the DIM pin of other LM3445s or
other LED drivers to dim multiple LED circuits simultaneously.
Input voltage pin. This pin provides the power for the internal control circuitry and gate driver.
Bleeder pin. Provides the input signal to the angle detect circuitry as well as a current path through a
switched 230Ω resistor to ensure proper firing of the triac dimmer.
No Connect
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These devices have limited built-in ESD protection. The leads should be shorted together or the device placed in conductive foam
during storage or handling to prevent electrostatic damage to the MOS gates.
ABSOLUTE MAXIMUM RATINGS
(1) (2)
BLDR to GND
-0.3V to +17V
VCC, GATE, FLTR1 to GND
-0.3V to +14V
ISNS to GND
-0.3V to +2.5V
ASNS, DIM, FLTR2, COFF to GND
-0.3V to +7.0V
COFF Input Current
100mA
Continuous Power Dissipation (3)
ESD Susceptibility, HBM
Internally Limited
(4)
2 kV
Junction Temperature (TJ-MAX)
150°C
Storage Temperature Range
-65°C to +150°C
Maximum Lead Temperature Range (Soldering)
(1)
(2)
(3)
(4)
260°C
Absolute maximum ratings are limits beyond which damage to the device may occur. Operating Ratings are conditions for which the
device is intended to be functional, but device parameter specifications may not be guaranteed. For ensured specifications and test
conditions, see the Electrical Characteristics. All voltages are with respect to the potential at the GND pin, unless otherwise specified.
If Military/Aerospace specified devices are required, please contact the Texas Instruments Sales Office/Distributors for availability and
specifications.
Internal thermal shutdown circuitry protects the device from permanent damage. Thermal shutdown engages at TJ = 165°C (typ.) and
disengages at TJ = 145°C (typ).
Human Body Model, applicable std. JESD22-A114-C.
OPERATING CONDITIONS
VCC
8.0V to 12V
−40°C to +125°C
Junction Temperature
ELECTRICAL CHARACTERISTICS
Limits in standard type face are for TJ = 25°C and those with boldface type apply over the full Operating Temperature
Range ( TJ = −40°C to +125°C). Minimum and Maximum limits are specified through test, design, or statistical correlation.
Typical values represent the most likely parametric norm at TJ = +25ºC, and are provided for reference purposes only.
Symbol
Parameter
Conditions
Bleeder resistance to GND
IBLDR = 10mA
Min
Typ
Max
Units
230
325
Ω
Operating supply current
2.00
2.85
mA
Rising threshold
7.4
7.7
V
BLEEDER
RBLDR
VCC SUPPLY
IVCC
VCC-UVLO
Falling threshold
6.0
Hysterisis
6.4
1
COFF
VCOFF
Time out threshold
1.276
1.327
V
RCOFF
Off timer sinking impedance
1.225
33
60
Ω
tCOFF
Restart timer
180
µs
CURRENT LIMIT
VISNS
ISNS limit threshold
tISNS
Leading edge blanking time
125
ns
Current limit reset delay
180
µs
33
ns
ISNS limit to GATE delay
1.174
ISNS = 0 to 1.75V step
1.269
1.364
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ELECTRICAL CHARACTERISTICS (continued)
Limits in standard type face are for TJ = 25°C and those with boldface type apply over the full Operating Temperature
Range ( TJ = −40°C to +125°C). Minimum and Maximum limits are specified through test, design, or statistical correlation.
Typical values represent the most likely parametric norm at TJ = +25ºC, and are provided for reference purposes only.
Symbol
Parameter
Conditions
Min
Typ
Max
Units
INTERNAL PWM RAMP
fRAMP
Frequency
VRAMP
Valley voltage
0.96
1.00
1.04
Peak voltage
2.85
3.00
3.08
Maximum duty cycle
96.5
98.0
6.79
7.21
DRAMP
5.85
kHz
V
%
DIM DECODER
tANG_DET
VASNS
Angle detect rising threshold
Observed on BLDR pin
ASNS filter delay
ASNS VMAX
IASNS
VDIM
7.81
4
3.85
4.00
ASNS drive capability sink
VASNS = 2V
7.6
ASNS drive capability source
VASNS = 2V
-4.3
DIM low sink current
VDIM = 1V
DIM High source current
VDIM = 4V
DIM low voltage
PWM input voltage
threshold
1.65
DIM high voltage
VTSTH
Tri-state threshold voltage
RDIM
DIM comparator tri-state impedance
Apply to FLTR1 pin
4.15
V
mA
2.80
-4.00
0.9
V
µs
-3.00
1.33
V
2.33
3.15
4.87
5.25
10
V
MΩ
CURRENT SENSE COMPARATOR
VFLTR2
FLTR2 open circuit voltage
RFLTR2
FLTR2 impedance
VOS
720
750
780
mV
0.1
4.0
mV
V
420
Current sense comparator offset voltage
-4.0
kΩ
GATE DRIVE OUTPUT
VDRVH
GATE high saturation
IGATE = 50 mA
0.24
0.50
VDRVL
GATE low saturation
IGATE = 100 mA
0.22
0.50
IDRV
Peak souce current
GATE = VCC/2
-0.77
Peak sink current
GATE = VCC/2
0.88
Rise time
Cload = 1 nF
15
Fall time
Cload = 1 nF
15
tDV
A
ns
THERMAL SHUTDOWN
TSD
Thermal shutdown temperature
See
(1)
Thermal shutdown hysteresis
165
°C
20
THERMAL SHUTDOWN
RθJA
(1)
4
VSSOP-10 junction to ambient
121
°C/W
Junction-to-ambient thermal resistance is highly application and board-layout dependent. In applications where high maximum power
dissipation exists, special care must be paid to thermal dissipation issues in board design. In applications where high power dissipation
and/or poor package thermal resistance is present, the maximum ambient temperature may have to be derated. Maximum ambient
temperature (TA-MAX) is dependent on the maximum operating junction temperature (TJ-MAX-OP = 125°C), the maximum power dissipation
of the device in the application (PD-MAX), and the junction-to ambient thermal resistance of the part/package in the application (RθJA), as
given by the following equation: TA-MAX = TJ-MAX-OP – (RθJA × PD-MAX).
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TYPICAL PERFORMANCE CHARACTERISTICS
fSW vs Input Line Voltage
Efficiency vs Input Line Voltage
95.0
300k
14 Series connected LEDs
250k
7 LEDs in Series (VO = 24.5V)
90.0
EFFICIENCY (%)
fSW (Hz)
200k
150k
100k
85.0
10 Series connected LEDs
80.0
50k
C11 = 2.2 nF, R3 = 348 k:
0
80
90
100
110
120
130
75.0
80
140
90
LINE VOLTAGE (VAC)
100
110
120
130
140
LINE VOLTAGE (VAC)
Figure 3.
Figure 4.
BLDR Resistor vs Temperature
VCC UVLO vs Temperature
300
8.0
UVLO (VCC) Rising
280
260
UVLO (V)
BLDR RESISTOR (Ö)
7.5
240
7.0
UVLO (VCC) Falling
6.5
220
200
-50 -25
0
25
50
75
6.0
-50 -25
100 125 150
0
TEMPERATURE (°C)
25
50
75
100 125 150
TEMPERATURE (°C)
Figure 5.
Figure 6.
Min On-Time (tON) vs Temperature
Off Threshold (C11) vs Temperature
200.0
1.29
190.0
180.0
VOFF (V)
tON-MIN (ns)
1.28
170.0
1.27
OFF Threshold at C11
1.26
160.0
150.0
-50 -25
0
25
50
75
100 125 150
1.25
-50 -25
0
25
50
75
100 125 150
TEMPERATURE (°C)
TEMPERATURE (°C)
Figure 7.
Figure 8.
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TYPICAL PERFORMANCE CHARACTERISTICS (continued)
Normalized Variation in fSW over VBUCK Voltage
Leading Edge Blanking Variation Over Temperature
1.50
15.0
100 units tested
Room (25°C)
1.25
1.00
NUMBER OF UNITS
NORMALIZED SW FREQ
Series
connected LEDs
3 LEDs
5 LEDs
0.75
0.50
Hot (125°C)
Cold (-40°C)
10.0
5.0
7 LEDs
9 LEDs
0.25
0
50
100
150
200
0.0
80
VBUCK (V)
120
140
160
180
LEADING EDGE BLANKING (ns)
Figure 9.
6
100
Figure 10.
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SIMPLIFIED INTERNAL BLOCK DIAGRAM
VCC
ANGLE DETECT
BLDR
LM3445
INTERNAL
REGULATORS
4 Ps
7.2V
VCC UVLO
230
BLEEDER
THERMAL
SHUTDOWN
COFF
33:
ASNS
MOSFET
DRIVER
COFF
GATE
1.276V
S
START
Q
R
0V to 4V
LATCH
750 mV
50k
DIM DECODER
4.9V
PWM
370k
Tri-State
CONTROLLER
FLTR1
RAMP
I-LIM
DIM
RAMP GEN.
5.9 kHz
3V
1V
1.27V
ISNS
1k
LEADING EDGE BLANKING
FLTR2
125 ns
GND
Figure 11. Simplified Block Diagram
APPLICATION INFORMATION
FUNCTIONAL DESCRIPTION
The LM3445 contains all the necessary circuitry to build a line-powered (mains powered) constant current LED
driver whose output current can be controlled with a conventional triac dimmer.
OVERVIEW OF PHASE CONTROL DIMMING
A basic "phase controlled" triac dimmer circuit is shown in Figure 12.
BRIGHT
R1
250 kÖ
DIM
TRIAC
MAINS AC
R2
3.3 kÖ
DIAC
C1
100 nF
LOAD
Figure 12. Basic Triac Dimmer
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An RC network consisting of R1, R2, and C1 delay the turn on of the triac until the voltage on C1 reaches the
trigger voltage of the diac. Increasing the resistance of the potentiometer (wiper moving downward) increases the
turn-on delay which decreases the on-time or "conduction angle" of the triac (θ). This reduces the average power
delivered to the load. Voltage waveforms for a simple triac dimmer are shown in Figure 13. Figure 13a shows the
full sinusoid of the input voltage. Even when set to full brightness, few dimmers will provide 100% on-time, i.e.,
the full sinusoid.
(a)
(b)
DELAY
?
(c)
?
DELAY
Figure 13. Line Voltage and Dimming Waveforms
Figure 13b shows a theoretical waveform from a dimmer. The on-time is often referred to as the "conduction
angle" and may be stated in degrees or radians. The off-time represents the delay caused by the RC circuit
feeding the triac. The off-time be referred to as the "firing angle" and is simply 180° - θ.
Figure 13c shows a waveform from a so-called reverse phase dimmer, sometimes referred to as an electronic
dimmer. These typically are more expensive, microcontroller based dimmers that use switching elements other
than triacs. Note that the conduction starts from the zero-crossing, and terminates some time later. This method
of control reduces the noise spike at the transition.
Since the LM3445 has been designed to assess the relative on-time and control the LED current accordingly,
most phase-control dimmers, both forward and reverse phase, may be used with success.
8
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THEORY OF OPERATION
Refer to Figure 14 which shows the LM3445 along with basic external circuitry.
V+
VBUCK
D3
C7
+
D9
BR1
C10
D8
R2
C9
D4
+
C12
Q1
TRIAC
DIMMER
VLED
-
R4
VLED-
D2
VAC
D1
D10
R5
Q3
C5
L2
LM3445MM
1 ASNS
U1
BLDR 10
ICOLL
R1
2 FLTR1
C3
3 DIM
VCC 9
GATE 8
4 COFF
ISNS 7
5 FLTR2
GND 6
Q2
R3
C4
C11
Figure 14. LM3445 Schematic
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SENSING THE RECTIFIED TRIAC WAVEFORM
A bridge rectifier, BR1, converts the line (mains) voltage (Figure 15c) into a series of half-sines as shown in
Figure 15b. Figure 15a shows a typical voltage waveform after diode D3 (valley fill circuit, or VBUCK).
VBUCK
(a)
VBR1
(b)
VAC
(c)
t
Figure 15. Voltage Waveforms After Bridge Rectifier Without Triac Dimming
Figure 16c and Figure 16b show typical triac dimmed voltage waveforms before and after the bridge rectifier.
Figure 16a shows a typical triac dimmed voltage waveform after diode D3 (valley fill circuit, or VBUCK).
VBUCK
(a)
t
VBR1
(b)
t
VAC
(c)
t
delay
?
Figure 16. Voltage Waveforms After Bridge Rectifier With Triac Dimming
LM3445 LINE SENSING CIRCUITRY
An external series pass regulator (R2, D1, and Q1) translates the rectified line voltage to a level where it can be
sensed by the BLDR pin on the LM3445.
10
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V+
R2
Q1
D2
D1
R5
C5
R11
LM3445MM
U1
1 ASNS
BLDR 10
R1
2
FLTR1
3
DIM
VCC 9
C3
GATE
8
4 COFF
ISNS 7
5 FLTR2
GND 6
C4
Figure 17. LM3445 AC Line Sense Circuitry
D1 is typically a 15V zener diode which forces transistor Q1 to “stand-off” most of the rectified line voltage.
Having no capacitance on the source of Q1 allows the voltage on the BLDR pin to rise and fall with the rectified
line voltage as the line voltage drops below zener voltage D1 (see ANGLE DETECT).
A diode-capacitor network (D2, C5) is used to maintain the voltage on the VCC pin while the voltage on the
BLDR pin goes low. This provides the supply voltage to operate the LM3445.
Resistor R5 is used to bleed charge out of any stray capacitance on the BLDR node and may be used to provide
the necessary holding current for the dimmer when operating at light output currents.
TRIAC HOLDING CURRENT RESISTOR
In order to emulate an incandescent light bulb (essentially a resistor) with any LED driver, the existing triac will
require a small amount of holding current throughout the AC line cycle. An external resistor (R5) needs to be
placed on the source of Q1 to GND to perform this function. Most existing triac dimmers only require a few
milliamps of current to hold them on. A few “less expensive” triacs sold on the market will require a bit more
current. The value of resistor R5 will depend on:
• What type of triac the LM3445 will be used with
• How many light fixtures are running off of the triac
With a single LM3445 circuit on a common triac dimmer, a holding current resistor between 3 kΩ and 5 kΩ will
be required. As the number of LM3445 circuits is added to a single dimmer, the holding resistor R5’s resistance
can be increased. A few triac dimmers will require a resistor as low as 1 kΩ or lower for a single LM3445 circuit.
The trade-off will be performance vs efficiency. As the holding resistor R5 is increased, the overall efficiency per
LM3445 will also increase.
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ANGLE DETECT
The Angle Detect circuit uses a comparator with a fixed threshold voltage of 7.21V to monitor the BLDR pin to
determine whether the triac is on or off. The output of the comparator drives the ASNS buffer and also controls
the Bleeder circuit. A 4 µs delay line on the output is used to filter out noise that could be present on this signal.
The output of the Angle Detect circuit is limited to a 0V to 4.0V swing by the buffer and presented to the ASNS
pin. R1 and C3 comprise a low-pass filter with a bandwidth on the order of 1.0Hz.
The Angle Detect circuit and its filter produce a DC level which corresponds to the duty cycle (relative on-time) of
the triac dimmer. As a result, the LM3445 will work equally well with 50Hz or 60Hz line voltages.
BLEEDER
While the BLDR pin is below the 7.21V threshold, the bleeder MOSFET is on to place a small load (230Ω) on the
series pass regulator. This additional load is necessary to complete the circuit through the triac dimmer so that
the dimmer delay circuit can operate correctly. Above 7.21V, the bleeder resistor is removed to increase
efficiency.
FLTR1 PIN
The FLTR1 pin has two functions. Normally, it is fed by ASNS through filter components R1 and C3 and drives
the dim decoder. However, if the FLTR1 pin is tied above 4.9V (typical), e.g., to VCC, the Ramp Comparator is
tri-stated, disabling the dim decoder. See MASTER/SLAVE OPERATION.
DIM DECODER
The ramp generator produces a 5.85 kHz saw tooth wave with a minimum of 1.0V and a maximum of 3.0V. The
filtered ASNS signal enters pin FLTR1 where it is compared against the output of the Ramp Generator.
The output of the ramp comparator will have an on-time which is inversely proportional to the average voltage
level at pin FLTR1. However, since the FLTR1 signal can vary between 0V and 4.0V (the limits of the ASNS pin),
and the Ramp Generator signal only varies between 1.0V and 3.0V, the output of the ramp comparator will be on
continuously for VFLTR1 < 1.0V and off continuously for VFLTR1 > 3.0V. This allows a decoding range from 45° to
135° to provide a 0 – 100% dimming range.
The output of the ramp comparator drives both a common-source N-channel MOSFET through a Schmitt trigger
and the DIM pin (see MASTER/SLAVE OPERATION for further functions of the DIM pin). The MOSFET drain is
pulled up to 750 mV by a 50 kΩ resistor.
Since the MOSFET inverts the output of the ramp comparator, the drain voltage of the MOSFET is proportional
to the duty cycle of the line voltage that comes through the triac dimmer. The amplitude of the ramp generator
causes this proportionality to "hard limit" for duty cycles above 75% and below 25%.
The MOSFET drain signal next passes through an RC filter comprised of an internal 370 kΩ resistor, and an
external capacitor on pin FLTR2. This forms a second low pass filter to further reduce the ripple in this signal,
which is used as a reference by the PWM comparator. This RC filter is generally set to 10Hz.
The net effect is that the output of the dim decoder is a DC voltage whose amplitude varies from near 0V to 750
mV as the duty cycle of the dimmer varies from 25% to 75%. This corresponds to conduction angles of 45° to
135°, respectively.
The output voltage of the Dim Decoder directly controls the peak current that will be delivered by Q2 during its
on-time. See BUCK CONVERTER for details.
As the triac fires beyond 135°, the DIM decoder no longer controls the dimming. At this point the LEDs will dim
gradually for one of two reasons:
1. The voltage at VBUCK decreases and the buck converter runs out of headroom and causes LED current to
decrease as VBUCK decreases.
2. Minimum on-time is reached which fixes the duty-cycle and therefore reduces the voltage at VBUCK.
The transition from dimming with the DIM decoder to headroom or minimum on-time dimming is seamless. LED
currents from full load to as low as 0.5 mA can be easily achieved.
12
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VALLEY-FILL CIRCUIT
VBUCK supplies the power which drives the LED string. Diode D3 allows VBUCK to remain high while V+ cycles on
and off. VBUCK has a relatively small hold capacitor C10 which reduces the voltage ripple when the valley fill
capacitors are being charged. However, the network of diodes and capacitors shown between D3 and C10 make
up a "valley-fill" circuit. The valley-fill circuit can be configured with two or three stages. The most common
configuration is two stages. Figure 18 illustrates a two and three stage valley-fill circuit.
V+
VBUCK
D3
C7
+
VBUCK
V+ D3
R6
D9
C7
+
D8
D8
D4
R8
C10
+
C10
R6
D9
D6
R8
+
D5
R7
C9
C8
D4
D7
C9
+
R7
Figure 18. Two and Three Stage Valley Fill Circuit
The valley-fill circuit allows the buck regulator to draw power throughout a larger portion of the AC line. This
allows the capacitance needed at VBUCK to be lower than if there were no valley-fill circuit, and adds passive
power factor correction (PFC) to the application. Besides better power factor correction, a valley-fill circuit allows
the buck converter to operate while separate circuitry translates the dimming information. This allows for dimming
that isn’t subject to 120Hz flicker that can be perceived by the human eye.
VALLEY-FILL OPERATION
When the “input line is high”, power is derived directly through D3. The term “input line is high” can be explained
as follows. The valley-fill circuit charges capacitors C7 and C9 in series (see Figure 19) when the input line is
high.
VBUCK
V+
D3
+
C7
+
VBUCK
2
C10
D8
D4
+
VBUCK
2
+
C9
-
Figure 19. Two Stage Valley-Fill Circuit When AC Line is High
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The peak voltage of a two stage valley-fill capacitor is:
VVF-CAP =
VAC-RMS
2
2
(1)
As the AC line decreases from its peak value every cycle, there will be a point where the voltage magnitude of
the AC line is equal to the voltage that each capacitor is charged. At this point diode D3 becomes reversed
biased, and the capacitors are placed in parallel to each other (Figure 20), and VBUCK equals the capacitor
voltage.
VBUCK
V+
D3
C7
+
+
VBUCK
D9
C10
D8
D4
+
VBUCK
+
C9
-
Figure 20. Two Stage Valley-Fill Circuit When AC Line is Low
A three stage valley-fill circuit performs exactly the same as two-stage valley-fill circuit except now three
capacitors are now charged in series, and when the line voltage decreases to:
VVF-CAP =
VAC-RMS
3
2
(2)
Diode D3 is reversed biased and three capacitors are in parallel to each other.
The valley-fill circuit can be optimized for power factor, voltage hold up and overall application size and cost. The
LM3445 will operate with a single stage or a three stage valley-fill circuit as well. Resistor R8 functions as a
current limiting resistor during start-up, and during the transition from series to parallel connection. Resistors R6
and R7 are 1 MΩ bleeder resistors, and may or may not be necessary for each application.
BUCK CONVERTER
The LM3445 is a buck controller that uses a proprietary constant off-time method to maintain constant current
through a string of LEDs. While transistor Q2 is on, current ramps up through the inductor and LED string. A
resistor R3 senses this current and this voltage is compared to the reference voltage at FLTR2. When this
sensed voltage is equal to the reference voltage, transistor Q2 is turned off and diode D10 conducts the current
through the inductor and LEDs. Capacitor C12 eliminates most of the ripple current seen in the inductor. Resistor
R4, capacitor C11, and transistor Q3 provide a linear current ramp that sets the constant off-time for a given
output voltage.
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VBUCK
R4
C12
D10
Q3
L2
ICOLL
LM3445MM
GATE
4
COFF
8
ISNS
7
GND
6
Q2
R3
C11
Figure 21. LM3445 Buck Regulation Circuit
OVERVIEW OF CONSTANT OFF-TIME CONTROL
A buck converter’s conversion ratio is defined as:
VO
tON
VIN = D = tON + tOFF = tON x fSW
(3)
Constant off-time control architecture operates by simply defining the off-time and allowing the on-time, and
therefore the switching frequency, to vary as either VIN or VO changes. The output voltage is equal to the LED
string voltage (VLED), and should not change significantly for a given application. The input voltage or VBUCK in
this analysis will vary as the input line varies. The length of the on-time is determined by the sensed inductor
current through a resistor to a voltage reference at a comparator. During the on-time, denoted by tON, MOSFET
switch Q2 is on causing the inductor current to increase. During the on-time, current flows from VBUCK, through
the LEDs, through L2, Q2, and finally through R3 to ground. At some point in time, the inductor current reaches a
maximum (IL2-PK) determined by the voltage sensed at R3 and the ISNS pin. This sensed voltage across R3 is
compared against the voltage of dim decoder output, FLTR2, at which point Q2 is turned off by the controller.
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IL2-PK
'iL
IAVE
IL2-MIN
IL2 (t)
tON
tOFF
t
Figure 22. Inductor Current Waveform in CCM
During the off-period denoted by tOFF, the current through L2 continues to flow through the LEDs via D10.
MASTER/SLAVE OPERATION
Multiple LM3445s can be configured so that large strings of LEDs can be controlled by a single triac dimmer. By
doing so, smooth consistent dimming for multiple LED circuits is achieved.
When the FLTR1 pin is tied above 4.9V (typical), preferably to VCC, the ramp comparator is tri-stated, disabling
the dim decoder. This allows one or more LM3445 devices or PWM LED driver devices (slaves) to be controlled
by a single LM3445 (master) by connecting their DIM pins together.
MASTER/SLAVE CONFIGURATION
TI offers an LM3445 demonstration PCB for customer evaluation through our website. The following description
and theory uses reference designators that follow our evaluation PCB. The LM3445 Master/Slave schematics are
illustrated below (Figure 23 through Figure 25) for clarity. Each board contains a separate circuit for the Master
and Slave function. Both the Master and Slave boards will need to be modified from their original stand alone
function so that they can be coupled together. Only the Master LM3445 requires use of the Master/Slave circuit
for any number of slaves.
MASTER BOARD MODIFICATIONS
•
•
•
Remove R10 and replace with a BAS40 diode
Connect TP18 to TP14 (VCC)
Connect TP17 (gate of Q5) to TP15 (gate of Q2)
SLAVE BOARD(S) MODIFICATIONS
•
•
Remove R11 (disconnects BLDR)
Tie TP14 (FLTR1) to VCC
MASTER/SLAVE(S) INTERCONNECTION
•
•
Connect TP19 of Master to TP10 of Slave (Master VCC Control)
Connect TP6 (DIM pin) of Master to TP6 (DIM pin) of Slave (Master DIM Control)
MASTER/SLAVE THEORY OF OPERATION
By placing two series diodes on the Master VCC circuit one forces the master VCC UVLO to become the
dominant threshold. When Master VCC drops below UVLO, GATE stops switching and the RC timer (>200 µs)
rises above the TL431 threshold (2.5V) which in turn pulls down on the gate of the Slave pass device (Q1).
The valley-fill circuit could consist of one large circuit to power all LM3445 series connected, or each LM3445
circuit could have a separate valley-fill circuit located near the buck converter.
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MASTER/SLAVE CONNECTION DIAGRAM
V+
V+
MASTER LM3445
SLAVE LM3445
R2
R2
TP10
Q1
Q1
D2
MASTER
VCC CTRL
BAS40
D2
R10
D1
D1
R5
C5
R5
C5
R11
R11
LM3445MM
R1
LM3445MM
MASTER-VBUCK
U1
1 ASNS BLDR 10
VCC 9
2 FLTR1
2 FLTR1
C3
3 DIM
U1
1 ASNS BLDR 10
MASTERBUCK
GATE 8
3 DIM
VCC 9
GATE 8
4 COFF
ISNS 7
4 COFF
ISNS 7
5 FLTR2
GND 6
5 FLTR2
GND 6
TP18
TP19
C4
SLAVE
BUCK
C4
R13
C13
SLAVE-VBUCK
R12
D11
TP17
Q5
C14
MASTER
DIM CTRL
MASTER/
SLAVE
CIRCUIT
Figure 23. Master Slave Configuration
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MASTER/SLAVE BLOCK DIAGRAMS
V+
N
BR1
Valley-Fill
CKT
Valley-Fill
CKT
Valley-Fill
CKT
SLAVE
BUCK
SLAVE
BUCK
MASTER
BUCK
L
MASTER
CTRL
MASTER
VCC
MASTER
DIM
Figure 24. Master/Slave Configuration With Separate Valley-Fill Circuits
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V+
Large Valley-Fill CKT
N
BR1
MASTER
BUCK
L
SLAVE
BUCK
SLAVE
BUCK
MASTER
CTRL
MASTER
VCC CTRL
MASTER
DIM CTRL
Figure 25. Master/Slave Configuration With One Valley-Fill Circuit
THERMAL SHUTDOWN
Thermal shutdown limits total power dissipation by turning off the output switch when the IC junction temperature
exceeds 165°C. After thermal shutdown occurs, the output switch doesn’t turn on until the junction temperature
drops to approximately 145°C.
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DESIGN GUIDE
DETERMINING DUTY-CYCLE (D)
Duty cycle (D) approximately equals:
VLED
tON
=
D
=
VBUCK
tON + tOFF = tON x fSW
(4)
With efficiency considered:
1 u VLED = D
K VBUCK
(5)
For simplicity, choose efficiency between 75% and 85%.
CALCULATING OFF-TIME
The “Off-Time” of the LM3445 is set by the user and remains fairly constant as long as the voltage of the LED
stack remains constant. Calculating the off-time is the first step in determining the switching frequency of the
converter, which is integral in determining some external component values.
PNP transistor Q3, resistor R4, and the LED string voltage define a charging current into capacitor C11. A
constant current into a capacitor creates a linear charging characteristic.
i = C dv
dt
(6)
Resistor R4, capacitor C11 and the current through resistor R4 (iCOLL), which is approximately equal to VLED/R4,
are all fixed. Therefore, dv is fixed and linear, and dt (tOFF) can now be calculated.
tOFF = C11 x 1.276V x
R4
VLED
(7)
Common equations for determining duty cycle and switching frequency in any buck converter:
fSW =
1
tOFF + tON
t
V
= V LED
D = t +ONt
BUCK
ON
OFF
tOFF
'¶ = t +
tOFF
ON
(8)
Therefore:
fSW = tD , and fSW = 1t - D
OFF
ON
(9)
With efficiency of the buck converter in mind:
VLED
VBUCK = K u D
(10)
Substitute equations and rearrange:
fSW =
§
¨1
©
VLED ·
1
K u VBUCK ¸¹
tOFF
(11)
Off-time, and switching frequency can now be calculated using the equations above.
SETTING THE SWITCHING FREQUENCY
Selecting the switching frequency for nominal operating conditions is based on tradeoffs between efficiency
(better at low frequency) and solution size/cost (smaller at high frequency).
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The input voltage to the buck converter (VBUCK) changes with both line variations and over the course of each
half-cycle of the input line voltage. The voltage across the LED string will, however, remain constant, and
therefore the off-time remains constant.
The on-time, and therefore the switching frequency, will vary as the VBUCK voltage changes with line voltage. A
good design practice is to choose a desired nominal switching frequency knowing that the switching frequency
will decrease as the line voltage drops and increase as the line voltage increases (see Figure 26).
1.50
NORMALIZED SW FREQ
Series
connected LEDs
1.25
1.00
3 LEDs
5 LEDs
0.75
0.50
7 LEDs
9 LEDs
0.25
0
50
100
150
200
VBUCK (V)
Figure 26. Graphical Illustration of Switching Frequency vs VBUCK
The off-time of the LM3445 can be programmed for switching frequencies ranging from 30 kHz to over 1 MHz. A
trade-off between efficiency and solution size must be considered when designing the LM3445 application.
The maximum switching frequency attainable is limited only by the minimum on-time requirement (200 ns).
Worst case scenario for minimum on time is when VBUCK is at its maximum voltage (AC high line) and the LED
string voltage (VLED) is at its minimum value.
VLED(MIN)
1
1
tON(MIN) = K u V
BUCK(MAX) fSW
(12)
The maximum voltage seen by the Buck Converter is:
VBUCK(MAX) = VAC-RMS(MAX) x 2
(13)
INDUCTOR SELECTION
The controlled off-time architecture of the LM3445 regulates the average current through the inductor (L2), and
therefore the LED string current. The input voltage to the buck converter (VBUCK) changes with line variations and
over the course of each half-cycle of the input line voltage. The voltage across the LED string is relatively
constant, and therefore the current through R4 is constant. This current sets the off-time of the converter and
therefore the output volt-second product (VLED x off-time) remains constant. A constant volt-second product
makes it possible to keep the ripple through the inductor constant as the voltage at VBUCK varies.
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VBUCK
VLED
C12
-
D10
L2
VL2
Q2
R3
Figure 27. LM3445 External Components of the Buck Converter
The equation for an ideal inductor is:
Q = L di
dt
(14)
Given a fixed inductor value, L, this equation states that the change in the inductor current over time is
proportional to the voltage applied across the inductor.
During the on-time, the voltage applied across the inductor is,
VL(ON-TIME) = VBUCK - (VLED + VDS(Q2) + IL2 x R3)
(15)
Since the voltage across the MOSFET switch (Q2) is relatively small, as is the voltage across sense resistor R3,
we can simplify this to approximately,
VL(ON-TIME) = VBUCK - VLED
(16)
During the off-time, the voltage seen by the inductor is approximately:
VL(OFF-TIME) = VLED
(17)
The value of VL(OFF-TIME) will be relatively constant, because the LED stack voltage will remain constant. If we
rewrite the equation for an inductor inserting what we know about the circuit during the off-time, we get:
'i
VL(OFF-TIME) = VLED = L x 't
(I
-I
)
VL(OFF-TIME) = VLED = L x (MAX) (MIN)
't
(18)
Re-arranging this gives:
LED
'i # tOFF x VL2
(19)
From this we can see that the ripple current (Δi) is proportional to off-time (tOFF) multiplied by a voltage which is
dominated by VLED divided by a constant (L2).
These equations can be rearranged to calculate the desired value for inductor L2.
VLED
L2 # tOFF x 'i
(20)
Where:
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tOFF =
VLED
1
K u VBUCK
fSW
(21)
1 VLED
K u VBUCK
fSW x 'i
(22)
1
Finally:
VLED 1
L2 =
Refer to DESIGN EXAMPLE to better understand the design process.
SETTING THE LED CURRENT
The LM3445 constant off-time control loop regulates the peak inductor current (IL2). The average inductor current
equals the average LED current (IAVE). Therefore the average LED current is regulated by regulating the peak
inductor current.
IL2-PK
'iL
IAVE
IL2-MIN
IL2 (t)
tON
tOFF
t
Figure 28. Inductor Current Waveform in CCM
Knowing the desired average LED current, IAVE and the nominal inductor current ripple, ΔiL, the peak current for
an application running in continuous conduction mode (CCM) is defined as follows:
L
IL2-PK = IAVE + 'i
2
(23)
Or, the maximum, or "undimmed", LED current would then be,
L
IAVE(UNDIM) = IL2-PK(UNDIM) - 'i
2
(24)
This is important to calculate because this peak current multiplied by the sense resistor R3 will determine when
the internal comparator is tripped. The internal comparator turns the control MOSFET off once the peak sensed
voltage reaches 750 mV.
IL-PK(UNDIM) =
750 mV
R3
(25)
Current Limit: Under normal circumstances, the trip voltage on the PWM comparator would be less than or
equal to 750 mV, depending on the amount of dimming. However, if there is a short circuit or an excessive load
on the output, higher than normal switch currents will cause a voltage above 1.27V on the ISNS pin which will
trip the I-LIM comparator. The I-LIM comparator will reset the RS latch, turning off Q2. It will also inhibit the Start
Pulse Generator and the COFF comparator by holding the COFF pin low. A delay circuit will prevent the start of
another cycle for 180 µs.
VALLEY FILL CAPACITORS
Determining voltage rating and capacitance value of the valley-fill capacitors:
The maximum voltage seen by the valley-fill capacitors is:
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VVF-CAP =
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VAC(MAX) 2
#stages
(26)
This is, of course, if the capacitors chosen have identical capacitance values and split the line voltage equally.
Often a 20% difference in capacitance could be observed between like capacitors. Therefore a voltage rating
margin of 25% to 50% should be considered.
Determining the capacitance value of the valley-fill capacitors:
The valley fill capacitors should be sized to supply energy to the buck converter (VBUCK) when the input line is
less than its peak divided by the number of stages used in the valley fill (tX). The capacitance value should be
calculated when the triac is not firing, i.e. when full LED current is being drawn by the LED string. The maximum
power is delivered to the LED string at this time, and therefore the most capacitance will be needed.
30°
150°
tX
VBUCK
8.33 ms
t
180°
0°
Figure 29. Two Stage Valley-Ffill VBUCK Voltage with no TRIAC Dimming
From the above illustration and the equation for current in a capacitor, i = C x dV/dt, the amount of capacitance
needed at VBUCK will be calculated as follows:
At 60Hz, and a valley-fill circuit of two stages, the hold up time (tX) required at VBUCK is calculated as follows. The
total angle of an AC half cycle is 180° and the total time of a half AC line cycle is 8.33 ms. When the angle of the
AC waveform is at 30° and 150°, the voltage of the AC line is exactly ½ of its peak. With a two stage valley-fill
circuit, this is the point where the LED string switches from power being derived from AC line to power being
derived from the hold up capacitors (C7 and C9). 60° out of 180° of the cycle or 1/3 of the cycle the power is
derived from the hold up capacitors (1/3 x 8.33 ms = 2.78 ms). This is equal to the hold up time (dt) from the
above equation, and dv is the amount of voltage the circuit is allowed to droop. From the next section
(“Determining Maximum Number of Series Connected LEDs Allowed”) we know the minimum VBUCK voltage will
be about 45V for a 90VAC to 135VAC line. At 90VAC low line operating condition input, ½ of the peak voltage is
64V. Therefore with some margin the voltage at VBUCK can not droop more than about 15V (dv). (i) is equal to
(POUT/VBUCK), where POUT is equal to (VLED x ILED). Total capacitance (C7 in parallel with C9) can now be
calculated. See DESIGN EXAMPLE for further calculations of the valley-fill capacitors.
Determining Maximum Number of Series Connected LEDs Allowed:
The LM3445 is an off-line buck topology LED driver. A buck converter topology requires that the input voltage
(VBUCK) of the output circuit must be greater than the voltage of the LED stack (VLED) for proper regulation. One
must determine what the minimum voltage observed by the buck converter will be before the maximum number
of LEDs allowed can be determined. Two variables will have to be determined in order to accomplish this.
1. AC line operating voltage. This is usually 90VAC to 135VAC for North America. Although the LM3445 can
operate at much lower and higher input voltages a range is needed to illustrate the design process.
2. How many stages are implemented in the valley-fill circuit (1, 2 or 3).
In this example the most common valley-fill circuit will be used (two stages).
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45° 90° 135°
VPEAK
VAC
t
Figure 30. AC Line with Firing Angles
Figure 31 show three triac dimmed waveforms. One can easily see that the peak voltage (VPEAK) from 0° to 90°
will always be:
VAC-RMS-PK 2
(27)
Once the triac is firing at an angle greater than 90° the peak voltage will lower and equal to:
VAC-RMS-PK 2 x SIN(T)
(28)
The voltage at VBUCK with a valley fill stage of two will look similar to the waveforms of Figure 32.
The purpose of the valley fill circuit is to allow the buck converter to pull power directly off of the AC line when
the line voltage is greater than its peak voltage divided by two (two stage valley fill circuit). During this time, the
capacitors within the valley fill circuit (C7 and C8) are charged up to the peak of the AC line voltage. Once the
line drops below its peak divided by two, the two capacitors are placed in parallel and deliver power to the buck
converter. One can now see that if the peak of the AC line voltage is lowered due to variations in the line voltage,
or if the triac is firing at an angle above 90°, the DC offset (VDC) will lower. VDC is the lowest value that voltage
VBUCK will encounter.
VBUCK(MIN) =
VAC-RMS(MIN) 2 x SIN(T)
#stages
(29)
Example:
Line voltage = 90VAC to 135VAC
Valley-Fill = two stage
o
90 2 x SIN(135 )
= 45V
VBUCK(MIN) =
2
(30)
Depending on what type and value of capacitors are used, some derating should be used for voltage droop when
the capacitors are delivering power to the buck converter. When the triac is firing at 135° the current through the
LED string will be small. Therefore the droop should be small at this point and a 5% voltage droop should be a
sufficient derating. With this derating, the lowest voltage the buck converter will see is about 42.5V in this
example.
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VPEAK
VPEAK
V+
V+
VPEAK
V+
t
t
θ = 45°
t
θ = 90°
θ = 135°
Figure 31. AC Line with Various Firing Angles
VPEAK
VPEAK
V+
V+
VDC
V
DC
VDC
t
t
Figure 32. VBUCK Waveforms with Various Firing Angles
To determine how many LEDs can be driven, take the minimum voltage the buck converter will see (42.5V) and
divide it by the worst case forward voltage drop of a single LED.
Example: 42.5V/3.7V = 11.5 LEDs (11 LEDs with margin)
OUTPUT CAPACITOR
A capacitor placed in parallel with the LED or array of LEDs can be used to reduce the LED current ripple while
keeping the same average current through both the inductor and the LED array. With a buck topology the output
inductance (L2) can now be lowered, making the magnetics smaller and less expensive. With a well designed
converter, you can assume that all of the ripple will be seen by the capacitor, and not the LEDs. One must
ensure that the capacitor you choose can handle the RMS current of the inductor. Refer to manufacture’s
datasheets to ensure compliance. Usually an X5R or X7R capacitor between 1 µF and 10 µF of the proper
voltage rating will be sufficient.
SWITCHING MOSFET
The main switching MOSFET should be chosen with efficiency and robustness in mind. The maximum voltage
across the switching MOSFET will equal:
VDS(MAX) = VAC-RMS(MAX) 2
(31)
The average current rating should be greater than:
IDS-MAX = ILED(-AVE)(DMAX)
26
(32)
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RE-CIRCULATING DIODE
The LM3445 Buck converter requires a re-circulating diode D10 (see the Typical Application circuit to carry the
inductor current during the MOSFET Q2 off-time. The most efficient choice for D10 is a diode with a low forward
drop and near-zero reverse recovery time that can withstand a reverse voltage of the maximum voltage seen at
VBUCK. For a common 110VAC ± 20% line, the reverse voltage could be as high as 190V.
VD t VAC-RMS(MAX) 2
(33)
The current rating must be at least:
ID = 1 - (DMIN) x ILED(AVE)
(34)
Or:
ID = 1 -
VLED(MIN)
x ILED(AVE)
VBUCK(MAX)
(35)
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DESIGN EXAMPLE
The following design example illustrates the process of calculating external component values.
Known:
1. Input voltage range (90VAC – 135VAC)
2. Number of LEDs in series = 7
3. Forward voltage drop of a single LED = 3.6V
4. LED stack voltage = (7 x 3.6V) = 25.2V
Choose:
1. Nominal switching frequency, fSW-TARGET = 250 kHz
2. ILED(AVE) = 400 mA
3. Δi (usually 15% - 30% of ILED(AVE)) = (0.30 x 400 mA) = 120 mA
4. Valley fill stages (1,2, or 3) = 2
5. Assumed minimum efficiency = 80%
Calculate:
1. Calculate minimum voltage VBUCK equals:
o
90 2 x SIN(135 )
= 45V
2
VBUCK(MIN) =
(36)
2. Calculate maximum voltage VBUCK equals:
VBUCK(MAX) = 135 2 = 190V
(37)
3. Calculate tOFF at VBUCK nominal line voltage:
1
u 25.2V
0.8 115 2
= 3.23 Ps
(250 kHz)
1
tOFF =
(38)
4. Calculate tON(MIN) at high line to ensure that tON(MIN) > 200 ns:
1
u 25.2V
0.8 135 2
tON (MIN) =
1
1
u 25.2V
0.8 135 2
u 3.23 Ps = 638 ns
(39)
5. Calculate C11 and R4:
6. Choose current through R4: (between 50 µA and 100 µA) 70 µA
VLED
R4 =
ICOLL
= 360 k:
(40)
7. Use a standard value of 365 kΩ
8. Calculate C11:
C11 =
VLED tOFF
= 175 pF
R4 1.276
9.
10. Use standard value of 120 pF
11. Calculate ripple current: 400 mA X 0.30 = 120 mA
12. Calculate inductor value at tOFF = 3 µs:
1
u 25.2V
0.8 115 2
= 580 PH
(350 kHz x 0.1A)
(41)
25.2V 1
L2 =
(42)
13. Choose C10: 1.0 µF 200V
14. Calculate valley-fill capacitor values: VAC low line = 90VAC, VBUCK minimum equals 60V (no triac dimming at
maximum LED current). Set droop for 20V maximum at full load and low line.
28
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SNVS570L – JANUARY 2009 – REVISED MAY 2013
i = C dv
dt
(43)
i) equals POUT/VBUCK (270 mA), dV equals 20V, dt equals 2.77 ms, and then CTOTAL equals 37 µF. Therefore
C7 = C9 = 22 µF
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29
LM3445
SNVS570L – JANUARY 2009 – REVISED MAY 2013
www.ti.com
LM3445 DESIGN EXAMPLE 1
INPUT = 90VAC TO 135VAC, VLED = 7 x HB LED STRING APPLICATION @ 400 MA
VBUCK
V+
TP3
D3
TP4
LED+
BR1
+
R6
D9
C7
R8
D8
C10
C2
+
L4
D4
R7
C9
VLED
R4
C12
C15
L3
C1
D10
V+
TP10
TP5
LEDVLED-
D12
Q3
R2
L5
TP14
Q1
D2
R10
L2
D1
R5
C5
L1
R11
ICOLL
RT1
R14
LM3445MM
TP11
F1
U1
1 ASNS
J1
BLDR 10
R1
2
FLTR1
3
DIM
VCC 9
TP12
C3
VAC
TRIAC
DIMMER
TP15
GATE
8
Q2
TP6
TP16
Master-Slave Circuitry
TP18
TP19
4 COFF
ISNS 7
5 FLTR2
GND 6
R3
C4
C13
R12
R13
TP7-9
C11
D11
TP17
30
Q5
C14
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LM3445
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SNVS570L – JANUARY 2009 – REVISED MAY 2013
Table 1. Bill of Materials
Qty
Ref Des
Description
Mfr
Mfr PN
1
U1
IC, CTRLR, DRVR-LED, VSSOP10
TI
LM3445MM
1
BR1
Bridge Rectifiier, SMT, 400V, 800 mA
DiodesInc
HD04-T
1
L1
Common mode filter DIP4NS, 900 mA, 700 µH
Panasonic
ELF-11090E
1
L2
Inductor, SHLD, SMT, 1A, 470 µH
Coilcraft
MSS1260-474-KLB
2
L3, L4
Diff mode inductor, 500 mA 1 mH
Coilcraft
MSS1260-105KL-KLB
HI1206T161R-10
1
L5
Bead Inductor, 160Ω, 6A
Steward
3
C1, C2, C15
Cap, Film, X2Y2, 12.5MM, 250VAC, 20%, 10 nF
Panasonic
ECQ-U2A103ML
1
C3
Cap, X7R, 0603, 16V, 10%, 470 nF
MuRata
GRM188R71C474KA88D
1
C4
Cap, X7R, 0603, 16V, 10%, 100 nF
MuRata
GRM188R71C104KA01D
2
C5, C6
Cap, X5R, 1210, 25V, 10%, 22 µF
MuRata
GRM32ER61E226KE15L
2
C7, C9
Cap, AL, 200V, 105C, 20%, 33 µF
UCC
EKXG201ELL330MK20S
1
C10
Cap, Film, 250V, 5%, 10 nF
Epcos
B32521C3103J
1
C12
Cap, X7R, 1206, 50V, 10%, 1.0 uF
Kemet
C1206F105K5RACTU
1
C11
Cap, C0G, 0603, 100V, 5%, 120 pF
MuRata
GRM1885C2A121JA01D
1
C13
Cap, X7R, 0603, 50V, 10%, 1.0 nF
Kemet
C0603C102K5RACTU
1
C14
Cap, X7R, 0603, 50V, 10%, 22 nF
Kemet
C0603C223K5RACTU
1
D1
Diode, ZNR, SOT23, 15V, 5%
OnSemi
BZX84C15LT1G
2
D2, D13
Diode, SCH, SOD123, 40V, 120 mA
NXP
BAS40H
4
D3, D4, D8, D9
Diode, FR, SOD123, 200V, 1A
Rohm
RF071M2S
1
D10
Diode, FR, SMB, 400V, 1A
OnSemi
MURS140T3G
1
D11
IC, SHNT, ADJ, SOT23, 2.5V, 0.5%
TI
TL431BIDBZR
1
D12
TVS, VBR = 209V
LittleFuse
P6SMB220CA
1
R1
Resistor, 0603, 1%, 280 kΩ
Panasonic
ERJ-3EKF2803V
1
R2
Resistor, 1206, 1%, 100 kΩ
Panasonic
ERJ-8ENF1003V
1
R3
Resistor, 1210, 5%, 1.8Ω
Panasonic
ERJ-14RQJ1R8U
1
R4
Resistor, 0603, 1%, 576 kΩ
Panasonic
ERJ-3EKF5763V
1
R5
Resistor, 1206, 1%, 1.00 kΩ
Panasonic
ERJ-8ENF1001V
2
R6, R7
Resistor, 0805, 1%, 1.00 MΩ
Rohm
MCR10EZHF1004
2
R8, R10
Resistor, 1206, 0.0Ω
Yageo
RC1206JR-070RL
1
R9
Resistor, 1812, 0.0Ω
1
R11
Resistor, 0603, 0.0Ω
Yageo
RC0603JR-070RL
1
R12
Resistor, 0603, 1%, 33.2 kΩ
Panasonic
ERJ-3EKF3322V
1
R13
Resistor, 0603, 1%, 2.0 kΩ
Panasonic
ERJ-3EKF2001V
1
R14
Resistor, 0805, 1%, 3.3 MΩ
Rohm
MCR10EZHF3304
1
RT1
Thermistor, 120V, 1.1A, 50Ω @ 25°C
Thermometrics
CL-140
2
Q1, Q2
XSTR, NFET, DPAK, 300V, 4A
Fairchild
FQD7N30TF
1
Q3
XSTR, PNP, SOT23, 300V, 500 mA
Fairchild
MMBTA92
1
Q5
XSTR, NFET, SOT23, 100V, 170 mA
Fairchild
BSS123
1
J1
Terminal Block 2 pos
Phoenix Contact
1715721
1
F1
Fuse, 125V, 1,25A
bel
SSQ 1.25
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31
LM3445
SNVS570L – JANUARY 2009 – REVISED MAY 2013
www.ti.com
REVISION HISTORY
Changes from Revision K (May 2013) to Revision L
•
32
Page
Changed layout of National Data Sheet to TI format .......................................................................................................... 31
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PACKAGE OPTION ADDENDUM
www.ti.com
8-Nov-2013
PACKAGING INFORMATION
Orderable Device
Status
(1)
Package Type Package Pins Package
Drawing
Qty
Eco Plan
Lead/Ball Finish
MSL Peak Temp
(2)
(6)
(3)
Green (RoHS
& no Sb/Br)
CU SN
Level-1-260C-UNLIM
Op Temp (°C)
Device Marking
(4/5)
LM3445M/NOPB
ACTIVE
SOIC
D
14
55
LM3445MM/NOPB
ACTIVE
VSSOP
DGS
10
1000
Green (RoHS CU NIPDAUAG | CU SN Level-1-260C-UNLIM
& no Sb/Br)
-40 to 125
SULB
LM3445MMX/NOPB
ACTIVE
VSSOP
DGS
10
3500
Green (RoHS CU NIPDAUAG | CU SN Level-1-260C-UNLIM
& no Sb/Br)
-40 to 125
SULB
LM3445MX/NOPB
ACTIVE
SOIC
D
14
2500
Green (RoHS
& no Sb/Br)
CU SN
Level-1-260C-UNLIM
LM3445M
LM3445M
(1)
The marketing status values are defined as follows:
ACTIVE: Product device recommended for new designs.
LIFEBUY: TI has announced that the device will be discontinued, and a lifetime-buy period is in effect.
NRND: Not recommended for new designs. Device is in production to support existing customers, but TI does not recommend using this part in a new design.
PREVIEW: Device has been announced but is not in production. Samples may or may not be available.
OBSOLETE: TI has discontinued the production of the device.
(2)
Eco Plan - The planned eco-friendly classification: Pb-Free (RoHS), Pb-Free (RoHS Exempt), or Green (RoHS & no Sb/Br) - please check http://www.ti.com/productcontent for the latest availability
information and additional product content details.
TBD: The Pb-Free/Green conversion plan has not been defined.
Pb-Free (RoHS): TI's terms "Lead-Free" or "Pb-Free" mean semiconductor products that are compatible with the current RoHS requirements for all 6 substances, including the requirement that
lead not exceed 0.1% by weight in homogeneous materials. Where designed to be soldered at high temperatures, TI Pb-Free products are suitable for use in specified lead-free processes.
Pb-Free (RoHS Exempt): This component has a RoHS exemption for either 1) lead-based flip-chip solder bumps used between the die and package, or 2) lead-based die adhesive used between
the die and leadframe. The component is otherwise considered Pb-Free (RoHS compatible) as defined above.
Green (RoHS & no Sb/Br): TI defines "Green" to mean Pb-Free (RoHS compatible), and free of Bromine (Br) and Antimony (Sb) based flame retardants (Br or Sb do not exceed 0.1% by weight
in homogeneous material)
(3)
MSL, Peak Temp. - The Moisture Sensitivity Level rating according to the JEDEC industry standard classifications, and peak solder temperature.
(4)
There may be additional marking, which relates to the logo, the lot trace code information, or the environmental category on the device.
(5)
Multiple Device Markings will be inside parentheses. Only one Device Marking contained in parentheses and separated by a "~" will appear on a device. If a line is indented then it is a continuation
of the previous line and the two combined represent the entire Device Marking for that device.
(6)
Lead/Ball Finish - Orderable Devices may have multiple material finish options. Finish options are separated by a vertical ruled line. Lead/Ball Finish values may wrap to two lines if the finish
value exceeds the maximum column width.
Addendum-Page 1
Samples
PACKAGE OPTION ADDENDUM
www.ti.com
8-Nov-2013
Important Information and Disclaimer:The information provided on this page represents TI's knowledge and belief as of the date that it is provided. TI bases its knowledge and belief on information
provided by third parties, and makes no representation or warranty as to the accuracy of such information. Efforts are underway to better integrate information from third parties. TI has taken and
continues to take reasonable steps to provide representative and accurate information but may not have conducted destructive testing or chemical analysis on incoming materials and chemicals.
TI and TI suppliers consider certain information to be proprietary, and thus CAS numbers and other limited information may not be available for release.
In no event shall TI's liability arising out of such information exceed the total purchase price of the TI part(s) at issue in this document sold by TI to Customer on an annual basis.
Addendum-Page 2
PACKAGE MATERIALS INFORMATION
www.ti.com
11-Oct-2013
TAPE AND REEL INFORMATION
*All dimensions are nominal
Device
Package Package Pins
Type Drawing
SPQ
Reel
Reel
A0
Diameter Width (mm)
(mm) W1 (mm)
B0
(mm)
K0
(mm)
P1
(mm)
W
Pin1
(mm) Quadrant
3.4
1.4
8.0
12.0
Q1
LM3445MM/NOPB
VSSOP
DGS
10
1000
178.0
12.4
5.3
LM3445MMX/NOPB
VSSOP
DGS
10
3500
330.0
12.4
5.3
3.4
1.4
8.0
12.0
Q1
LM3445MX/NOPB
SOIC
D
14
2500
330.0
16.4
6.5
9.35
2.3
8.0
16.0
Q1
Pack Materials-Page 1
PACKAGE MATERIALS INFORMATION
www.ti.com
11-Oct-2013
*All dimensions are nominal
Device
Package Type
Package Drawing
Pins
SPQ
Length (mm)
Width (mm)
Height (mm)
LM3445MM/NOPB
VSSOP
DGS
10
1000
210.0
185.0
35.0
LM3445MMX/NOPB
VSSOP
DGS
10
3500
367.0
367.0
35.0
LM3445MX/NOPB
SOIC
D
14
2500
367.0
367.0
35.0
Pack Materials-Page 2
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