TI1 LM3430 Boost controller for led backlighting Datasheet

LM3430
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SNVS472B – JANUARY 2007 – REVISED MAY 2013
Boost Controller for LED Backlighting
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FEATURES
DESCRIPTION
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The LM3430 is a high voltage low-side N-channel
MOSFET controller. Ideal for use in a boost regulator,
the LM3430 can power the LED backlight in LCD
panels, such as in notebook PCs. It contains all of the
features needed to implement single ended primary
topologies. Output voltage regulation is based on
current-mode control, which eases the design of loop
compensation while providing inherent input voltage
feed-forward. The LM3430 includes a start-up
regulator that operates over a wide input range of 6V
to 40V. The PWM controller is designed for high
speed capability including an oscillator frequency
range up to 2 MHz and total propagation delays less
than 100 ns. Additional features include an error
amplifier, precision reference, line under-voltage
lockout,
cycle-by-cycle
current
limit,
slope
compensation, soft-start, external synchronization
capability and thermal shutdown. The LM3430 is
available in the WSON-12 package.
1
2
Internal 40V Startup Regulator
1A Peak MOSFET Gate Driver
VIN Range 6V to 40V
Duty Cycle Limit in Excess of 90%
Programmable UVLO with Hysteresis
Cycle-by-Cycle Current Limit
External Synchronizable (AC-coupled)
Single Resistor Oscillator Frequency Set
Slope Compensation
Adjustable Soft-start
WSON-12 (3mm x 3mm)
APPLICATIONS
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LED Backlight Driver (companion to LM3432)
Boost Converter
SEPIC Converter
Typical Application
VIN
VO
VDHC
NC
VIN
OUT
RT
CS
LM3430
UVLO
GND
SS
VCC
COMP
FB
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.
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LM3430
SNVS472B – JANUARY 2007 – REVISED MAY 2013
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Connection Diagram
1
VDHC
NC
12
2
VIN
SS
11
3
FB
RT
10
CS
9
DAP
4
COMP
5
VCC
UVLO
8
6
OUT
GND
7
Figure 1. 12-Lead WSON Package
PIN DESCRIPTIONS
2
Pin(s)
Name
Description
Application Information
1
VDHC
Proprietary control input from LM3432
This pin accepts a control signal from LM3432 to adjust the output voltage
in real time.
2
VIN
Source input voltage
Input to the start-up regulator. Operates from 6V to 40V.
3
FB
Feedback pin
Inverting input to the internal voltage error amplifier. The non-inverting input
of the error amplifier connects to a 1.25V reference.
4
COMP
Error amplifier output and PWM
comparator input
The control loop compensation components connect between this pin and
the FB pin.
5
VCC
Output of the internal, high voltage
linear regulator.
This pin should be bypassed to the GND pin with a ceramic capacitor.
6
OUT
Output of gate driver
Connect this pin to the gate of the external MOSFET. The gate driver has a
1A peak current capability.
7
GND
System ground
8
UVLO
Input Under-Voltage Lock-out
9
CS
10
RT/SYNC
11
Set the start-up and shutdown levels by connecting this pin to the input
voltage through a resistor divider. A 20 µA current source provides
hysteresis.
Current Sense input
Input for the switch current sensing used for current mode control and for
current limiting.
Oscillator frequency adjust pin and
synchronization input
An external resistor connected from this pin to GND sets the oscillator
frequency. This pin can also accept an ac-coupled input for synchronization
from an external clock.
SS
Soft-start pin
An external capacitor placed from this pin to ground will be charged by a
10 µA current source, creating a ramp voltage to control the regulator startup.
12
NC
No-connect
Leave this pin open-circuit.
DAP
EP
Exposed Pad
Thermal connection pad, connect to GND.
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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)
If Military/Aerospace specified devices are required, please contact the Texas Instruments Sales Office/ Distributors
for availability and specifications.
VALUE / UNIT
VIN to GND
-0.3 V to 45 V
VCC to GND
-0.3 V to 16 V
RT/SYNC to GND
-0.3 V to 5.5 V
OUT to GND
-1.5 V for < 100 ns
All other pins to GND
-0.3 V to 7 V
Power Dissipation
Internally Limited
Junction Temperature
150°C
Storage Temperature
-65°C to +150°C
Soldering Information
ESD Rating
(1)
(2)
Vapor Phase (60 sec.)
215°C
Infrared (15 sec.)
220°C
Human Body Model
(2)
2 kV
Absolute Maximum Ratings are limits beyond which damage to the device may occur. The Recommended Operating Limits define the
conditions within which the device is intended to be functional. For specifications and test conditions, see the Electrical Characteristics.
The human body model is a 100 pF capacitor discharged through a 1.5kΩ resistor into each pin.
RECOMMENDED OPERATING CONDITIONS
(1)
VALUE / UNIT
Supply Voltage
6V to 40V
External Volatge at VCC
7.5V to 14V
Junction Temperature Range
(1)
-40°C to +125°C
Device thermal limitations may limit usable range.
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ELECTRICAL CHARACTERISTICS
Limits in standard type are for TJ = 25°C only; limits in boldface type apply over the junction temperature (TJ) range of -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 = 25°C, and are provided for reference purposes only. VIN = 18V and RT = 27.4 kΩ
unless otherwise indicated. (Note 3)
Symbol
Parameter
Conditions
Min
Typ
Max
Units
1.225
1.250
1.275
V
6.6
7
7.4
3.5
4
SYSTEM PARAMETERS
VFB
FB Pin Voltage
-40°C ≤ TJ ≤ 125°C
START-UP REGULATOR
VCC Regulation
9V ≤ VIN ≤ 40V, ICC = 1 mA
VCC Regulation
6V ≤ VIN < 9V, VCC Pin Open Circuit
ICC
Supply Current
OUT Pin Capacitance = 0, VCC = 10V
ICC-LIM
VCC Current Limit
VCC = 0V, (Note 4, 6)
VIN - VCC
Dropout Voltage Across Bypass Switch
ICC = 0 mA, fSW < 200 kHz, 6V ≤ VIN ≤
8.5V
200
VBYP-HI
Bypass Switch Turn-off Threshold
VIN increasing
8.7
V
VBYP-HYS
Bypass Switch Threshold Hysteresis
VIN Decreasing
260
mV
VIN = 6.0V
58
VIN = 8.0V
53
VIN = 18.0V
1.1
VCC
5
15
35
V
mA
mA
mV
ZVCC
VCC Pin Output Impedance
0 mA ≤ ICC ≤ 5 mA
VCC-HI
VCC Pin UVLO Rising Threshold
5
V
VCC-HYS
VCC Pin UVLO Falling Hysteresis
300
mV
IVIN
Start-up Regulator Leakage
VIN = 40V
150
500
µA
IIN-SD
Shutdown Current
VUVLO = 0V, VCC = Open Circuit
350
450
µA
Ω
ERROR AMPLIFIER
GBW
Gain Bandwidth
ADC
DC Gain
ICOMP
COMP Pin Current Sink Capability
4
VFB = 1.5V, VCOMP = 1V
MHz
75
dB
5
17
mA
1.22
1.25
1.28
V
16
20
24
µA
UVLO
VSD
Shutdown Threshold
ISD-HYS
Shutdown Hysteresis Current Source
CURRENT LIMIT
tLIM-DLY
Delay from ILIM to Output
VCS
Current Limit Threshold Voltage
tBLK
Leading Edge Blanking Time
RCS
CS Pin Sink Impedance
CS steps from 0V to 0.6V
OUT transitions to 90% of VCC
30
0.45
0.5
ns
0.55
65
Blanking active
V
ns
40
75
Ω
SOFT-START
ISS
Soft-start Current Source
7
10
13
µA
VSS-OFF
Soft-start to COMP Offset
0.35
0.55
0.75
V
OSCILLATOR
fSW
VSYNC-HI
4
RT to GND = 84.5 kΩ
(Note 5)
170
200
230
kHz
RT to GND = 27.4 kΩ
(Note 5)
525
600
675
kHz
RT to GND = 16.2 kΩ
(Note 5)
865
990
1115
kHz
Synchronization Rising Threshold
3.8
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ELECTRICAL CHARACTERISTICS (continued)
Limits in standard type are for TJ = 25°C only; limits in boldface type apply over the junction temperature (TJ) range of -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 = 25°C, and are provided for reference purposes only. VIN = 18V and RT = 27.4 kΩ
unless otherwise indicated. (Note 3)
Symbol
Parameter
Conditions
Min
Typ
Max
Units
PWM COMPARATOR
tCOMP-DLY
Delay from COMP to OUT Transition
VCOMP = 2V, CS stepped from 0V to 0.4V
DMIN
Minimum Duty Cycle
VCOMP = 0V
25
ns
DMAX
Maximum Duty Cycle
APWM
COMP to PWM Comparator Gain
VCOMP-OC
COMP Pin Open Circuit Voltage
VFB = 0V
4.3
5.2
6.1
V
ICOMP-SC
COMP Pin Short Circuit Current
VCOMP = 0V, VFB = 1.5V
0.6
1.1
1.5
mA
80
105
130
mV
0
90
%
95
%
0.33
V/V
SLOPE COMPENSATION
VSLOPE
Slope Compensation Amplitude
MOSFET DRIVER
VSAT-HI
Output High Saturation Voltage (VCC –
VOUT)
IOUT = 50 mA
0.25
0.75
V
VSAT-LO
Output Low Saturation Voltage (VOUT)
IOUT = 100 mA
0.25
0.75
V
tRISE
OUT Pin Rise Time
OUT Pin load = 1 nF
18
ns
tFALL
OUT Pin Fall Time
OUT Pin load = 1 nF
15
ns
°C
THERMAL CHARACTERISTICS
TSD
Thermal Shutdown Threshold
165
TSD-HYS
Thermal Shutdown Hysteresis
25
°C
θJA
Junction to Ambient Thermal Resistance
122
°C/W
DQB-12A Package
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TYPICAL PERFORMANCE CHARACTERISTICS
SPACER
6
Efficiency, VO = 40V
VFB vs. Temp (VIN = 18V)
Figure 2.
Figure 3.
VFB vs. VIN (TA = 25°C)
VCC vs. VIN (TA = 25°C)
Figure 4.
Figure 5.
Max Duty Cycle vs. fSW (TA = 25°C)
fSW vs. Temperature (RT = 16.2 kΩ)
Figure 6.
Figure 7.
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TYPICAL PERFORMANCE CHARACTERISTICS (continued)
SPACER
RT vs. fSW (TA = 25°C)
SS vs. Temperature
Figure 8.
Figure 9.
OUT Pin tR vs. Gate Capacitance
OUT Pin tF vs. Gate Capacitance
Figure 10.
Figure 11.
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LM3430
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BLOCK DIAGRAM
BYPASS
SWITCH
(6V to 8.7V)
V
I
N
VCC
7V SERIES
REGULATOR
REFERENCE
ENABLE
+
-
UVLO
5V
1.25V
LOGIC
1.25V
UVLO
HYSTERESIS
CLK
(20 PA)
RT/SYNC
OSC
DRIVER
VDHC
45 PA
VDHC
CONTROL
Max Duty
Limit
0
S
Q
OUT
R
Q
G
N
D
5V
COMP
5k
1.25V
PWM
100 k:
F
B
-+
LOGIC
1.4V
50 k:
SS
CS
2 k:
0.5V
SS
10 PA
SS
-+
CLK + LEB
8
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Example Circuit: LM3430 and LM3432
OTMb
To
MCU
IOUT1
FAULTb
DIMMING
CONTROL
PWM
IOUT2
IREF
MODE
LM3432
VIN
IOUT3
IOUT4
CDHC
IOUT5
VDHC
VCC
GND
IOUT6
RDHC
VIN
L1
CIN
VDHC
CINX
RUV2
NC
VIN
Q1
CO
COX
OUT
UVLO
RUV1
LM3430
RT
RT
VO
D1
SS
RS1
RS2
CS
GND
CF
VCC
CSNS
RSNS
RFB2
CSS
COMP
FB
R1
C2
RFB1
C1
Figure 12. LM3430 with LM3432
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APPLICATION PARAMETERS FOR VARIOUS LED CONFIGURATIONS
Input Voltage
8V to 21V
8V to 21V
8V to 18V
Maximum Output Voltage
33V
50V
33V
LED Configuration
8 LEDs x 6 Strings,
20 mA per string
12 LEDs x 6 Strings,
20 mA per string
8 LEDs x 6 Strings,
20 mA per string
Switching Frequency
1 MHz
1 MHz
2 MHz
L1
22 µH
22 µH
4.7 µH
Co
10 µF, 50V
20 µF, 100V
10 µF, 50V
Cin
10 µF, 50V
10 µF, 50V
10 µF, 50V
Cinx
100 nF
100 nF
100 nF
Css
1 nF
1 nF
1 nF
Rt
16.5 kΩ
16.5 kΩ
8.25 kΩ
Rfb1
4.64 kΩ
3.01 kΩ
16.5 kΩ
Rfb2
118 kΩ
118 kΩ
422 kΩ
Ruv1
10 kΩ
10 kΩ
10 kΩ
Ruv2
49.9 kΩ
49.9 kΩ
49.9 kΩ
12 pF
12 pF
39 pF
R1
75 kΩ
118 kΩ
150 kΩ
C2
220 nF
47 nF
4.7 nF
Rdhc
30 kΩ
9.09 kΩ
60.4 kΩ
Rs1
4.02 kΩ
4.02 kΩ
4.02 kΩ
Rs2
301Ω
301Ω
301Ω
Rsns
0.2Ω (1W)
0.2Ω (1W)
Two 1Ω (1W) in parallel
Csns
1 nF
1 nF
1 nF
Control Loop Compensation
C1
VDHC
Slope Compensation
Current Sensing
10
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APPLICATIONS INFORMATION
OVERVIEW
The LM3430 is a low-side N-channel MOSFET controller that contains all of the features needed to implement
single ended power converter topologies. The LM3430 includes a high-voltage startup regulator that operates
over a wide input range of 6V to 40V. The PWM controller is designed for high speed capability including an
oscillator frequency range up to 2 MHz and total propagation delays less than 100 ns. Additional features include
an error amplifier, precision reference, input under-voltage lockout, cycle-by-cycle current limit, slope
compensation, soft-start, oscillator sync capability and thermal shutdown.
The LM3430 is designed for current-mode control power converters that require a single drive output, such as
boost and SEPIC topologies. The LM3430 provides all of the advantages of current-mode control including input
voltage feed-forward, cycle-by-cycle current limiting and simplified loop compensation.
HIGH VOLTAGE START-UP REGULATOR
The LM3430 contains an internal high-voltage startup regulator that allows the VIN pin to be connected directly to
line voltages as high as 40V. The regulator output is internally current limited to 35 mA (typical). When power is
applied, the regulator is enabled and sources current into an external capacitor, CF, connected to the VCC pin.
The recommended capacitance range for CF is 0.1 µF to 100 µF. When the voltage on the VCC pin reaches the
rising threshold of 5V, the controller output is enabled. The controller will remain enabled until VCC falls below
4.7V. In applications using a transformer, an auxiliary winding can be connected through a diode to the VCC pin.
This winding should raise the VCC pin voltage to above 7.5V to shut off the internal startup regulator. Powering
VCC from an auxiliary winding improves conversion efficiency while reducing the power dissipated in the
controller. The capacitance of CF must be high enough that the it maintains the VCC voltage greater than the
VCC UVLO falling threshold (4.7V) during the initial start-up. During a fault condition when the converter auxiliary
winding is inactive, external current draw on the VCC line should be limited such that the power dissipated in the
start-up regulator does not exceed the maximum power dissipation capability of the controller.
An external start-up or other bias rail can be used instead of the internal start-up regulator by connecting the
VCC and the VIN pins together and feeding the external bias voltage (7.5V to 14V) to the two pins.
INPUT UNDER-VOLTAGE DETECTOR
The LM3430 contains an input Under Voltage Lock Out (UVLO) circuit. UVLO is programmed by connecting the
UVLO pin to the center point of an external voltage divider from VIN to GND. The resistor divider must be
designed such that the voltage at the UVLO pin is greater than 1.25V when VIN is in the desired operating
range. If the under voltage threshold is not met, all functions of the controller are disabled and the controller
remains in a low power standby state. UVLO hysteresis is accomplished with an internal 20 µA current source
that is switched on or off into the impedance of the set-point divider. When the UVLO threshold is exceeded, the
current source is activated to instantly raise the voltage at the UVLO pin. When the UVLO pin voltage falls below
the 1.25V threshold the current source is turned off, causing the voltage at the UVLO pin to fall. The UVLO pin
can also be used to implement a remote enable / disable function. If an external transistor pulls the UVLO pin
below the 1.25V threshold, the converter will be disabled. This external shutdown method is shown in Figure 13.
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VIN
VIN
RUV2
LM3430
UVLO
ON/OFF
RUV1
2N7000 or
Equivalent
GND
Figure 13. Enable/Disable Using UVLO
ERROR AMPLIFIER
An internal high gain error amplifier is provided within the LM3430. The amplifier’s non-inverting input is internally
set to a fixed reference voltage of 1.25V. The inverting input is connected to the FB pin. In non-isolated
applications such as the boost converter the output voltage, VO, is connected to the FB pin through a resistor
divider. The control loop compensation components are connected between the COMP and FB pins. For most
isolated applications the error amplifier function is implemented on the secondary side of the converter and the
internal error amplifier is not used. The internal error amplifier is configured as an open drain output and can be
disabled by connecting the FB pin to ground. An internal 5 kΩ pull-up resistor between a 5V reference and
COMP can be used as the pull-up for an opto-coupler in isolated applications.
CURRENT SENSING AND CURRENT LIMITING
The LM3430 provides a cycle-by-cycle over current protection function. Current limit is accomplished by an
internal current sense comparator. If the voltage at the current sense comparator input exceeds 0.5V, the
MOSFET gate drive will be immediately terminated. A small RC filter, located near the controller, is
recommended to filter noise from the current sense signal. The CS input has an internal MOSFET which
discharges the CS pin capacitance at the conclusion of every cycle. The discharge device remains on an
additional 65 ns after the beginning of the new cycle to attenuate leading edge ringing on the current sense
signal.
The LM3430 current sense and PWM comparators are very fast, and may respond to short duration noise
pulses. Layout considerations are critical for the current sense filter and sense resistor. The capacitor associated
with the CS filter must be located very close to the device and connected directly to the pins of the controller (CS
and GND). If a current sense transformer is used, both leads of the transformer secondary should be routed to
the sense resistor and the current sense filter network. The current sense resistor can be located between the
source of the primary power MOSFET and power ground, but it must be a low inductance type. When designing
with a current sense resistor all of the noise sensitive low-power ground connections should be connected
together locally to the controller and a single connection should be made to the high current power ground
(sense resistor ground point).
12
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OSCILLATOR, SHUTDOWN AND SYNC
A single external resistor, RT, connected between the RT/SYNC and GND pins sets the LM3430 oscillator
frequency. To set the switching frequency, fSW, RT can be calculated from:
-8
RT =
1 - 8 x 10 x fSW
fSW x 5.77 x 10
-11
(fSW in Hz, RT in :)
(1)
The LM3430 can also be synchronized to an external clock. The external clock must have a higher frequency
than the free running oscillator frequency set by the RT resistor. The clock signal should be capacitively coupled
into the RT/SYNC pin with a 100 pF capacitor, shown in Figure 14. A peak voltage level greater than 3.8V at the
RT/SYNC pin is required for detection of the sync pulse. The sync pulse width should be set between 15 ns to
150 ns by the external components. The RT resistor is always required, whether the oscillator is free running or
externally synchronized. The voltage at the RT/SYNC pin is internally regulated to 2V, and the typical delay from
a logic high at the RT/SYNC pin to the rise of the OUT pin voltage is 120 ns. RT should be located very close to
the device and connected directly to the pins of the controller (RT/SYNC and GND).
LM3430
EXTERNAL
CLOCK
CSS
RT/SYNC
100 pF
RT
15 ns to 150 ns
EXTERNAL
CLOCK
120 ns
(Typical)
OUT PIN
Figure 14. Sync Operation
PWM COMPARATOR AND SLOPE COMPENSATION
The PWM comparator compares the current ramp signal with the error voltage derived from the error amplifier
output. The error amplifier output voltage at the COMP pin is offset by 1.4V and then further attenuated by a 3:1
resistor divider. The PWM comparator polarity is such that 0V on the COMP pin will result in a zero duty cycle at
the controller output. For duty cycles greater than 50%, current mode control circuits can experience subharmonic oscillation. By adding an additional fixed-slope voltage ramp signal (slope compensation) this
oscillation can be avoided. The LM3430 generates the slope compensation with a 45 µAP-P sawtooth-waveform
current source generated by the clock. (See Figure 15) This current flows through an internal 2 kΩ resistor to
create a minimum compensation ramp voltage of 100 mV (typical). The amplitude of the compensation ramp
increases when external resistance is added for filtering the current sense (RS1) or in the position RS2. As shown
in Figure 15 and the block diagram, the sensed current slope and the compensation slope add together to create
the signal used for current limiting and for the control loop itself.
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LM3430
ISW
45 uA
0
RS1
RS2
CS
2 k:
0.5V
RSNS
CSNS
+
Current
Limit
VCL
Figure 15. Slope Compensation
In addition to preventing sub-harmonic oscillation, increasing the amplitude of the compensation ramp voltage
decreases the voltage across RSNS required to trip the current limit comparator. This technique can be used to
lower the value of RSNS and reduce power dissipation. Care must be taken not to add too much slope
compensation, however. Reducing RSNS causes the control loop gain to increase, and too large of a
compensation ramp can overwhelm the sensed current signal. This imbalance causes the system to act more
like a voltage-mode regulator with a low frequency double pole that is more difficult to compensate.
SOFT-START
The soft-start feature allows the power converter output to gradually reach the initial steady state output voltage,
thereby reducing start-up stresses and current surges. At power on, after the VCC and input under-voltage
lockout thresholds are satisfied, an internal 10 µA current source charges an external capacitor connected to the
SS pin. The capacitor voltage will ramp up slowly and will limit the COMP pin voltage and the switch current.
MOSFET GATE DRIVER
The LM3430 provides an internal gate driver through the OUT pin that can source and sink a peak current of 1A
to control external, ground-referenced MOSFETs.
DYNAMIC HEADROOM CONTROL
The VDHC pin of the LM3430 can be used in conjunction with the LM3432 to provide on-the-fly adjustments to
the output voltage for maximum efficiency when driving an array of LEDs. When this feature is not being used
the VDHC pin should be left open circuit.
THERMAL SHUTDOWN
Internal thermal shutdown circuitry is provided to protect the LM3430 in the event that the maximum junction
temperature is exceeded. When activated, typically at 165°C, the controller is forced into a low power standby
state, disabling the output driver and the VCC regulator. After the temperature is reduced (typical hysteresis is
25°C) the VCC regulator will be re-enabled and the LM3430 will perform a soft-start.
14
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DESIGN CONSIDERATIONS
The most common circuit controlled by the LM3430 is a non-isolated boost regulator. The boost regulator steps
up the input voltage and has a duty ratio D of:
D=
VO - VIN -VD
VO - VD
(VD is the forward voltage drop of the output diode)
(2)
The following is a design procedure for selecting all the components for the boost converter portion of the
Example Circuit of Figure 12. This circuit operates in continuous conduction mode (CCM), where inductor current
stays above 0A at all times, and delivers an output voltage of 33.0V ±2% at an output current of 180 mA. The
load is a white LED-based LCD monitor backlight, formed by six parallel strings of seven white LEDs each with a
multi-channel linear current regulator to sink 30 mA through each string. The forward voltage of each LED varies
from 3.0V to 4.2V over process and temperature and the current regulator requires approximately 4V of
headroom. The required output voltage is therefore 7 x 4.2V + 4V ≊ 33V.
The input voltage will come from a three-to-four-cell stack of lithium ion batteries (VIN = 9.0V to 16.8V) or a poorly
regulated AC-DC adapter that supplies 14.0V to 20.9V. The diode drop VD will be 0.5V, typical of a Schottky
diode.
SWITCHING FREQUENCY
The selection of switching frequency is based on the tradeoffs between size, cost, and efficiency. In general, a
lower frequency means larger, more expensive inductors and capacitors will be needed. A higher switching
frequency generally results in a smaller but less efficient solution, as the power MOSFET gate capacitances must
be charged and discharged more often in a given amount of time. For this application, a frequency of 600 kHz
was selected as a good compromise between the size of the inductor and efficiency. PCB area and component
height are restricted in this application. Following the equation given for RT in the Applications Information
section, a 27.4 kΩ 1% resistor should be used to switch at 600 kHz.
MOSFET
Selection of the power MOSFET is governed by tradeoffs between cost, size, and efficiency. Breaking down the
losses in the MOSFET is one way to determine relative efficiencies between different devices. For this example,
the SOIC-8 package provides a balance of a small footprint with good efficiency.
Losses in the MOSFET can be broken down into conduction loss, gate charging loss, and switching loss.
Conduction, or I2R loss, PC, is approximately:
PC = D x
IO
1-D
2
x RDSON x 1.3
(3)
The factor 1.3 accounts for the increase in MOSFET on resistance due to heating. Alternatively, the factor of 1.3
can be ignored and the on resistance of the MOSFET can be estimated using the RDSON Vs. Temperature curves
in the MOSFET datasheets.
Gate charging loss, PG, results from the current required to charge and discharge the gate capacitance of the
power MOSFET and is approximated as:
PG = VCC x QG x fSW
(4)
QG is the total gate charge of the MOSFET. Gate charge loss differs from conduction and switching losses
because the actual dissipation occurs in the LM3430 and not in the MOSFET itself. If no external bias is applied
to the VCC pin, additional loss in the LM3430 IC occurs as the MOSFET driving current flows through the VCC
regulator. This loss, PVCC, is estimated as:
PVCC = (VIN – VCC) x QG x fSW
(5)
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Switching loss, PSW, occurs during the brief transition period as the MOSFET turns on and off. During the
transition period both current and voltage are present in the channel of the MOSFET. The loss can be
approximated as:
PSW = 0.5 x VIN x [IO / (1 – D)] x (tR + tF) x fSW
Where
•
tR and tF are the rise and fall times of the MOSFET
(6)
For this example, the maximum drain-to-source voltage applied across the MOSFET is VO plus the ringing due to
parasitic inductance and capacitance. The maximum drive voltage at the gate of the high side MOSFET is VCC,
or 7V typical. The MOSFET selected must be able to withstand 33V plus any ringing from drain to source, and
be able to handle at least 7V plus ringing from gate to source. A minimum voltage rating of 40VD-S and 10VG-S
MOSFET will be used. Comparing the losses in a spreadsheet leads to a 60VD-S rated MOSFET in SO-8 with a
typical RDSON of 22 mΩ, a gate charge of 18 nC, and rise and falls times of 10 ns and 12 ns, respectively.
BOOST DIODE
The boost regulator requires a boost diode D1 (see the Typical Application circuit) to carrying the inductor current
during the MOSFET off-time. The most efficient choice for D1 is a Schottky diode due to low forward drop and
zero reverse recovery time. D1 must be rated to handle the maximum output voltage plus any switching node
ringing when the MOSFET is on. In practice, all switching converters have some ringing at the switching node
due to the diode parasitic capacitance and the lead inductance. D1 must also be rated to handle the average
output current, IO.
The overall converter efficiency becomes more dependent on the selection of D1 at low duty cycles, where the
boost diode carries the load current for an increasing percentage of the time. This power dissipation can be
calculating by checking the typical diode forward voltage, VD, from the I-V curve on the diode's datasheet and
then multiplying it by ID. Diode datasheets will also provide a typical junction-to-ambient thermal resistance, θJA,
which can be used to estimate the operating die temperature of the Schottky. Multiplying the power dissipation
(PD = IO x VD) by θJA gives the temperature rise. The diode case size can then be selected to maintain the
Schottky diode temperature below the operational maximum.
In this example a Schottky diode rated to 40V and 0.5A will be suitable, as the maximum diode current will be
180 mA. A small case such as SOD-123 or SOT-23 can be used if a small footprint is critical. Larger case sizes
generally have lower θJA and lower forward voltage drop, so for better efficiency, a larger case size such as SMA
can be used. In applications with a high boost ratio, such as 1:4, the reverse recovery time, tRR, has a large
impact on losses and efficiency. The Schottky diode selected should therefore have a tRR value below 15 ns.
BOOST INDUCTOR
The first criterion for selecting an inductor is the inductance itself. In fixed-frequency boost converters this value
is based on the desired peak-to-peak ripple current, ΔiL, which flows in the inductor along with the average
inductor current, IL. For a boost converter in CCM IL is greater than the average output current, IO. The two
currents are related by the following expression:
IL = IO / (1 – D)
(7)
As with switching frequency, the inductance used is a tradeoff between size and cost. Larger inductance means
lower input ripple current, however because the inductor is connected to the output during the off-time only there
is a limit to the reduction in output ripple voltage. Lower inductance results in smaller, less expensive magnetics.
An inductance that gives a ripple current of 30% to 50% of IL is a good starting point for a CCM boost converter.
Minimum inductance should be calculated at the extremes of input voltage to find the operating condition with the
highest requirement:
VIN x D
L1 =
fSW x 'iL
(8)
By calculating in terms of amperes, volts, and megahertz, the inductance value will come out in microhenrys.
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In order to ensure that the boost regulator operates in CCM a second equation is needed, and must also be
evaluated at the corners of input voltage to find the minimum inductance required:
D(1-D) x VIN
L2 =
IO x fSW
(9)
By calculating in terms of volts, amps and megahertz the inductance value will come out in microhenrys.
For this design ΔiL will be set to 40% of the maximum IL. Duty cycle is evaluated first at VIN(MIN) and at VIN(MAX).
Second, the average inductor current is evaluated at the two input voltages. Third, the inductor ripple current is
determined. Finally, the inductance can be calculated, and a standard inductor value selected that meets all the
criteria.
Inductance for Minimum Input Voltage
DVIN(MIN) = (33 – 9.0 – 0.5) / (33 – 0.5) = 72% IL-VIN(MIN) = 0.18 / (1 – 0.72) = 0.64A ΔiL = 0.4 x 0.64A = 0.26A
L1-VIN(MIN) =
L2-VIN(MIN) =
9 x 0.72
= 42 PH
0.6 x 0.26
(10)
(11)
0.72 x 0.28 x 9
= 17 PH
0.18 x 0.6
(12)
Inductance for Maximum Input Voltage
DVIN(MAX) = (33 – 20.9) / 33 = 37% IL-VIN(MIAX) = 0.18 / (1 – 0.37) = 0.29A ΔiL = 0.4 x 0.29A = 0.12A
L1-VIN(MAX) =
L2-VIN(MAX) =
20.9 x 0.36
= 105 PH
0.6 x 0.12
(13)
(14)
0.36 x 0.64 x 20.9
= 45 PH
0.18 x 0.6
(15)
Maximum average inductor current occurs at VIN(MIN), and the corresponding inductor ripple current is 0.26AP-P.
Selecting an inductance that exceeds the ripple current requirement at VIN(MIN) and the requirement to stay in
CCM for VIN(MAX) provides a tradeoff that allows smaller magnetics at the cost of higher ripple current at
maximum input voltage. For this example, a 47 µH inductor will satisfy these requirements.
The second criterion for selecting an inductor is the peak current carrying capability. This is the level above
which the inductor will saturate. In saturation the inductance can drop off severely, resulting in higher peak
current that may overheat the inductor or push the converter into current limit. In a boost converter, peak current,
IPK, is equal to the maximum average inductor current plus one half of the ripple current. First, the current ripple
must be determined under the conditions that give maximum average inductor current:
VIN x D
'iL =
fSW x L
(16)
Maximum average inductor current occurs at VIN(MIN). Using the selected inductance of 47 µH yields the
following:
ΔiL = (9 x 0.72) / (0.6 x 47) = 230 mAP-P
(17)
The highest peak inductor current over all operating conditions is therefore:
IPK = IL + 0.5 x ΔiL = 0.64 + 0.115 = 0.76A
(18)
Hence an inductor must be selected that has a peak current rating greater than 0.76A and an average current
rating greater than 0.64A. One possibility is an off-the-shelf 47 µH ±20% inductor that can handle a peak current
of 0.9A and an average current of 0.93A. Finally, the inductor current ripple is recalculated at the maximum input
voltage:
ΔiL-VIN(MAX) = (20.9 x 0.36) / (0.6 x 47) = 267 mAP-P
(19)
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OUTPUT CAPACITOR
The output capacitor in a boost regulator supplies current to the load during the MOSFET on-time and also filters
the AC portion of the load current during the off-time. This capacitor determines the steady state output voltage
ripple, ΔVO, a critical parameter for all voltage regulators. Output capacitors are selected based on their
capacitance, CO, their equivalent series resistance (ESR) and their RMS or AC current rating.
The magnitude of ΔVO is comprised of three parts, and in steady state the ripple voltage during the on-time is
equal to the ripple voltage during the off-time. For simplicity the analysis will be performed for the MOSFET
turning off (off-time) only. The first part of the ripple voltage is the surge created as the output diode D1 turns on.
At this point inductor/diode current is at the peak value, and the ripple voltage increase can be calculated as:
ΔVO1 = IPK x ESR
(20)
The second portion of the ripple voltage is the increase due to the charging of CO through the output diode. This
portion can be approximated as:
ΔVO2 = (IO / CO) x (D / fSW)
(21)
The final portion of the ripple voltage is a decrease due to the flow of the diode/inductor current through the
output capacitor’s ESR. This decrease can be calculated as:
ΔVO3 = ΔiL x ESR
(22)
The total change in output voltage is then:
ΔVO = ΔVO1 + ΔVO2 - ΔVO3
(23)
The combination of two positive terms and one negative term may yield an output voltage ripple with a net rise or
a net fall during the converter off-time. The ESR of the output capacitor(s) has a strong influence on the slope
and direction of ΔVO. Capacitors with high ESR such as tantalum and aluminum electrolytic create an output
voltage ripple that is dominated by ΔVO1 and ΔVO3, with a shape shown in Figure 16. Ceramic capacitors, in
contrast, have very low ESR and lower capacitance. The shape of the output ripple voltage is dominated by
ΔVO2, with a shape shown in Figure 17.
ÂvO
VO
ID
Figure 16. ΔVO Using High ESR Capacitors
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ÂvO
VO
ID
Figure 17. ΔVO Using Low ESR Capacitors
For this example, the load is fairly constant, and the height restriction favors the low profile of ceramic capacitors.
The output ripple voltage waveform of Figure 17 is assumed, and the capacitance will be selected first. The
desired ΔVO is ±2% of 33V, or 1.32VP-P. Beginning with the calculation for ΔVO2, the required minimum
capacitance is:
CO-MIN = (IO / ΔVO) x (DMAX / fSW) CO-MIN = (0.18 / 1.32) x (0.72 / 600000) = 164 nF
(24)
Ceramic capacitors rated 1.0 µF ±20% are available from many manufacturers. The minimum quality dielectric
that is suitable for switching power supply output capacitors is X5R, while X7R (or better) is preferred. Careful
attention must be paid to the DC voltage rating and case size, as ceramic capacitors can lose 60%+ of their
rated capacitance at the maximum DC voltage. For example, the typical loss in capacitance for a 1.0 µF, 50V,
1206-size capacitor is 50% at 30V. This is the reason that ceramic capacitors are often de-rated to 50% of their
capacitance at their working voltage.
The ESR of the selected capacitor has a typical value of 3 mΩ. The worst-case value for ΔVO1 occurs during the
peak current at minimum input voltage:
ΔVO1 = 1.26 x 0.003 = 3.8 mV
(25)
The worst-case capacitor charging ripple occurs at maximum duty cycle, taking into account an output
capacitance of 50% x 1 µF = 500 nF:
ΔVO2 = (0.18 / 5 x 10-7) x (0.72 / 600000) = 432 mV
(26)
Finally, the worst-case value for ΔVO3 occurs when inductor ripple current is highest, at maximum input voltage:
ΔVO3 = 0.398 x 0.003 = 1.2 mV (negligible)
(27)
The output voltage ripple can be estimated by summing the three terms:
ΔVO = 3.8 mV + 432 mV - 1.2 mV = 435 mV
(28)
The RMS current through the output capacitor(s) can be estimated using the following, worst-case equation:
IO-RMS = 1.13 x IL x D x (1 - D)
(29)
The highest RMS current occurs at minimum input voltage. For this example the maximum output capacitor RMS
current is:
IO-RMS(MAX) = 1.13 x 0.64 x (0.72 x 0.28)0.5 = 0.32ARMS
(30)
Ceramic capacitors in 1206 case sizes are generally capable of sustaining RMS currents in excess of 2A, making
them more than adequate for this application.
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VCC DECOUPLING CAPACITOR
The VCC pin should be decoupled with a ceramic capacitor placed as close as possible to the VCC and GND
pins of the LM3430. The decoupling capacitor should have a minimum X5R or X7R type dielectric to ensure that
the capacitance remains stable over voltage and temperature, and be rated to a minimum of 470 nF. One good
choice is a 1.0 µF device with X7R dielectric and 1206 case size rated to 25V.
INPUT CAPACITOR
The input capacitors to a boost regulator control the input voltage ripple, ΔVIN, hold up the input voltage during
load transients, and prevent impedance mismatch (also called power supply interaction) between the LM3430
and the inductance of the input leads. Selection of input capacitors is based on their capacitance, ESR, and RMS
current rating. The minimum value of ESR can be selected based on the maximum output current transient,
ISTEP, using the following expression:
(1-D) x 'vIN
ESRMIN =
2 x ISTEP
(31)
For this example, no specific load transient is given, hence ISTEP is set equal to the maximum load current of 180
mA. The desired ΔVIN is 4%P-P. ΔVIN and duty cycle are taken at minimum input voltage to give the worst-case
value:
ESRMIN = [(1 – 0.72) x 0.36] / 0.36 = 0.28Ω
(32)
The minimum input capacitance can be selected based on ΔVIN, based on the drop in VIN during a load transient,
or based on prevention of power supply interaction. In general, the requirement for greatest capacitance comes
from the power supply interaction. The inductance and resistance of the input source must be estimated, and if
this information is not available, they can be assumed to be 1 µH and 0.1Ω, respectively. Minimum capacitance
is then estimated as:
2 x LS x VO x IO
CMIN =
2
V IN x RS
(33)
As with ESR, the worst-case, highest minimum capacitance calculation comes at the minimum input voltage.
Using the default estimates for LS and RS, minimum capacitance is:
CMIN =
2 x 1 x 33 x 0.18
= 1.5 PF
2
9 x 0.1
(34)
The closest standard 20% capacitor value is 1.5 µF, but because the actual input source impedance and
resistance are not known, a 3.3 µF capacitor will be used. In general, doubling the calculated value of input
capacitance provides a good safety margin. The final calculation is for the RMS current. For boost converters
operating in CCM this can be estimated as:
IRMS = 0.29 x ΔiL(MAX)
(35)
From the inductor section, maximum inductor ripple current is 267 mA, hence the input capacitor(s) must be
rated to handle 0.29 x 0.267 = 77 mARMS.
The input capacitors can be ceramic, tantalum, aluminum, or almost any type, however the low capacitance
requirement makes ceramic capacitors particularly attractive. As with the output capacitors, the minimum quality
dielectric used should X5R, with X7R or better preferred. The voltage rating for input capacitors need not be as
conservative as the output capacitors, as the need for capacitance decreases as input voltage increases. For this
example, the capacitor selected will be 3.3 µF ±20%, rated to 25V, in a 1206 case size. The RMS current rating
is over 1A, more than enough for this application.
CURRENT SENSE FILTER
Parasitic circuit capacitance, inductance and gate drive current create a spike in the current sense voltage at the
point where Q1 turns on. In order to prevent this spike from terminating the on-time prematurely, every circuit
should have a low-pass filter that consists of CCS and RS1, shown in Figure 12. The time constant of this filter
should be long enough to reduce the parasitic spike without significantly affecting the shape of the actual current
sense voltage. The recommended range for RS1 is between 10Ω and 500Ω, and the recommended range for CCS
is between 100 pF and 2.2 nF. For this example, the values of RS1 and CCS will be 100Ω and 1 nF, respectively.
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RSNS AND CURRENT LIMIT
The current sensing resistor RSNS is used for steady state regulation of the inductor current and to sense overcurrent conditions. The resistance value selected must be low enough to keep the power dissipation to a
minimum, yet high enough to provide good signal-to-noise ratio for the current sensing circuitry. The resistance
should be set so that the current limit comparator, with a threshold of 0.5V, trips before the sensed current
exceeds the peak current rating of the inductor.
For this example the inductor peak current rating is 0.9A. The threshold for current limit, ILIM, is set slightly below
to account for tolerance of the circuit components, at a level of 0.8A. The required resistor calculation must take
into account both the switch current through RSNS and the compensation ramp current flowing through the
internal 2 kΩ and external 100Ω resistors:
RSNS =
VCS ± 45 PA x (2 k: + RS1 + RS2)
ILIM
(36)
(37)
RSNS = [0.5 - 45µ x (2000 + 100)] / 0.8 = 0.51Ω
Power dissipation in RSNS can be estimated by calculating the average current. The worst-case average current
through RSNS occurs at minimum input voltage/maximum duty cycle and can be calculated as:
PCS =
IO 2
1-D
x RSNS x D
(38)
(39)
2
PCS = [(0.18 / 0.27) x 0.51] x 0.73 = 0.16W
For this example a 0.51Ω ±1%, thick-film chip resistor in a 1206 case size rated to 0.33W will be used.
CONTROL LOOP COMPENSATION
The LM3430 uses peak current-mode PWM control to correct changes in output voltage due to line and load
transients. Peak current-mode provides inherent cycle-by-cycle current limiting, improved line transient response,
and easier control loop compensation.
The control loop is comprised of two parts. The first is the power stage, which consists of the pulse width
modulator, output filter, and the load. The second part is the error amplifier, which is an op-amp configured as an
inverting amplifier. Figure 18 shows the regulator control loop components.
L
+ C
O
D
VIN
+
-
RO
RSNS
RC
+
RFB2
R1
C2
C1
+
VREF
RFB1
+
-
Figure 18. Power Stage and Error Amp
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One popular method for selecting the compensation components is to create Bode plots of gain and phase for
the power stage and error amplifier. Combined, they make the overall bandwidth and phase margin of the
regulator easy to determine. Software tools such as Excel, MathCAD, and Matlab are useful for observing how
changes in compensation or the power stage affect system gain and phase.
The power stage in a CCM peak current mode boost converter consists of the DC gain, APS, a single low
frequency pole, fLFP, the ESR zero, fZESR, a right-half plane zero, fRHP, and a double pole resulting from the
sampling of the peak current. The power stage transfer function (also called the Control-to-Output transfer
function) can be written:
1+
GPS = APS x
s
s
ZZESR 1 - ZRHP
s
s
s2
1+ Z
1
+
Q
x
+
n
LEP
Z2n
Zn
Where the DC gain is defined as:
(1 - D) x RO
APS =
2 x RSNS
(40)
(41)
Where:
RO = VO / IO
(42)
The system ESR zero is:
ZZESR =
1
RC x C O
(43)
The low frequency pole is:
ZLEP =
1
0.5 x (RO + ESR) x CO
(44)
The right-half plane zero is:
VIN 2
RO x
VO
ZRHP =
L
(45)
The sampling double pole quality factor is:
1
Qn =
S -D + 0.5 + (1 - D)
Se
Sn
(46)
The sampling double corner frequency is:
ωn = π x fSW
(47)
The natural inductor current slope is:
Sn = RSNS x VIN / L
(48)
The external ramp slope is:
Se = 45 µA x (2000 + RS1 + RS2)] x fSW
(49)
In the equation for APS, DC gain is highest when input voltage is at the maximum and output current is at the
lower threshold of CCM operation. (IL = 0.5 x ΔiL) In this the example those conditions are VIN = 20.9V and IO =
180 mA.
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Maximum DC gain is 44 dB. The low frequency pole fP = 2πωP is at 1.9 kHz, the ESR zero fZ = 2πωZ is at 80
MHz, and the right-half plane zero fRHP = 2πωRHP is at 230 kHz. The sampling double-pole occurs at one-half of
the switching frequency. Gain and phase plots for the power stage are shown in Figure 19.
POWER STAGE GAIN (dB)
60
45
30
15
0
-15
-30
100
1k
10k
100k
1M
FREQUENCY (Hz)
POWER STAGE PHASE (°)
180
120
60
0
-60
-120
-180
100
1k
10k
100k
1M
FREQUENCY (Hz)
Figure 19. Power Stage Gain and Phase
The single pole causes a roll-off in the gain of -20 dB/decade at lower frequency, which then flattens out due to
the RHP zero. The sharp drop in gain beginning around 200 kHz is a result of the sampling double pole. The
phase tends towards -90° at lower frequency but then increases to -180° from the RHP zero and the sampling
double pole. The effect of the ESR zero is not seen because its frequency is several decades above the
switching frequency. The combination of increasing gain and decreasing phase makes converters with RHP
zeroes difficult to compensate. Setting the overall control loop bandwidth to 1/3 to 1/10 of the RHP zero
frequency minimizes these negative effects. If this loop were left uncompensated, the bandwidth would be 312
kHz and the phase margin -100°. The converter would oscillate, and therefore is compensated using the error
amplifier and a few passive components.
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The transfer function of the compensation block, GEA, can be derived by treating the error amplifier as an
inverting op-amp with input impedance ZI and feedback impedance ZF. The majority of applications will require a
Type II, or two-pole one-zero amplifier, shown in Figure 18. The LaPlace domain transfer function for this Type II
network is given by the following:
GEA =
ZF
ZI
=
1
X
RFB2 (C1 + C2)
s x R1 x C1 +1
s x R1 x C1 x C2
s
+1
C1 + C2
(50)
Many techniques exist for selecting the compensation component values. The following method is based upon
setting the mid-band gain of the error amplifier transfer function first and then positioning the compensation zero
and pole:
1. Determine the desired control loop bandwidth:The control loop bandwidth, f0dB, is the point at which the
total control loop gain (H = GPS x GEA) is equal to 0 dB. For this example, a low bandwidth of 30 kHz, or
approximately 1/8th of the RHP zero frequency, is chosen because of the wide variation in input voltage.
2. Determine the gain of the power stage at f0dB:This value, A, can be read graphically from the gain plot of
GPS or calculated by replacing the ‘s’ terms in GPS with ‘2πf0dB’. For this example the gain at 30 kHz is
approximately 20 dB.
3. Calculate the negative of A and convert it to a linear gain:By setting the mid-band gain of the error
amplifier to the negative of the power stage gain at f0dB, the control loop gain will equal 0 dB at that
frequency. For this example, -20 dB = 0.1V/V.
4. Select the resistance of the top feedback divider resistor RFB2:This value is arbitrary, however selecting
a resistance between 10 kΩ and 100 kΩ will lead to practical values of R1, C1 and C2. For this example,
RFB2 = 20 kΩ 1%.
5. Set R1 = A x RFB2:For this example: R1 = 0.1 x 20000 = 2 kΩ
6. Select a frequency for the compensation zero, fZ1:The suggested placement for this zero is at the low
frequency pole of the power stage, fLFP = ωLFP / 2π. For this example, fZ1 = fLFP = 1.9 kHz
7. Set
C2 =
1
:
2S x R1 x fZ1
(51)
For this example, C2 = 41.2 nF
8. Select a frequency for the compensation pole, fP1:The suggested placement for this pole is at one-half of
the switching frequency. For this example, fP1 = 200 kHz
9. Set
C1 =
C2
:
2S x C2 x R1 x fP1 -1
(52)
For this example, C1 = 401 pF
10. Plug the closest 1% tolerance values for RFB2 and R1, then the closest 10% values for C1 and C2
into GEA and model the error amp:The open-loop gain and bandwidth of the LM3430’s internal error
amplifier are 75 dB and 4 MHz, respectively. Their effect on GEA can be modeled using the following
expression:
2S x GBW
OPG =
2S x GBW
s+
ADC
(53)
ADC is a linear gain, the linear equivalent of 75 dB is approximately 5600V/V. C1 = 390 pF 10%, C2 = 39 nF
10%, R1 = 2 kΩ 1%
11. Plot or evaluate the actual error amplifier transfer function:
GEA-ACTUAL =
24
GEA x OPG
1 + GEA x OPG
(54)
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20
60
10
40
OVERALL LOOP GAIN (dB)
ERROR AMP GAIN (dB)
12. Plot or evaluate the complete control loop transfer function: The complete control loop transfer function
is obtained by multiplying the power stage and error amplifier functions together. The bandwidth and phase
margin can then be read graphically or evaluated numerically.
The bandwidth of this example circuit is 34 kHz, with a phase margin of 60°.
0
-10
-20
-30
-40
100
1k
10k
100k
20
0
-20
-40
-60
100
1M
1k
180
180
120
120
60
0
-60
-120
-180
100
1k
10k
100k
1M
FREQUENCY (Hz)
OVERALL LOOP PHASE (°)
ERROR AMP PHASE (°)
FREQUENCY (Hz)
10k
100k
1M
60
0
-60
-120
-180
100
FREQUENCY (Hz)
1k
10k
100k
1M
FREQUENCY (Hz)
Figure 20. Error Amplifier Gain and Phase
Figure 21. Overall Loop Gain and Phase
Efficiency Calculations
A reasonable estimation for the efficiency of a boost regulator controlled by the LM3430 can be obtained by
adding together the loss is each current carrying element and using the equation:
K=
PO
PO + Ptotal-loss
(55)
The following shows an efficiency calculation to complement the circuit design from the Design Considerations
section. Output power for this circuit is 33V x 0.18A = 5.9W. Input voltage is assumed to be 12V, and the
calculations used assume that the converter runs in CCM. Duty cycle for VIN = 12V is 63%, and the average
inductor current is 0.49A.
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LM3430
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CHIP OPERATING LOSS
This term accounts for the current drawn at the VIN pin. This current, IIN, drives the logic circuitry and the power
MOSFETs. The gate driving loss term from the power MOSFET section of Design Considerations is included in
the chip operating loss. For the LM3430, IIN is equal to the steady state operating current, ICC, plus the MOSFET
driving current, IGC. Power is lost as this current passes through the internal linear regulator of the LM3430.
IGC = QG X fSW IGC = 18 nC x 600 kHz = 11 mA
(56)
ICC is typically 3.5 mA, taken from the ELECTRICAL CHARACTERISTICS table. Chip Operating Loss is then:
PQ = VIN X (IQ + IGC) PQ = 12 X (3.5m + 11m) = 0.17W
(57)
MOSFET SWITCHING LOSS
PSW = 0.5 x VIN x IL x (tR + tF) x fSW PSW = 0.5 x 12 x 0.49 x (10 ns + 12 ns) x 6 x105 = 39 mW
(58)
MOSFET AND RSNS CONDUCTION LOSS
PC = D x (I2L x (RDSON x 1.3 + RSNS)) PC = 0.63 x (0.492 x (0.029 + 0.51) = 82 mW
(59)
INPUT CAPACITOR LOSS
This term represents the loss as input ripple current passes through the ESR of the input capacitor bank. In this
equation ‘n’ is the number of capacitors in parallel. The 3.3 µF input capacitor selected has an ESR of
approximately 3 mΩ, and ΔiL for a 12V input is 268 mA:
I2IN-RMS x ESR
PCIN =
n
2
IIN-RMS = 0.29 x ΔiL = 0.29 x 0.268 = 0.08A PCIN = 0.08 x 0.003 = 0.3 mW (negligible)
(60)
(61)
OUTPUT CAPACITOR LOSS
This term is calculated using the same method as the input capacitor loss, substituting the output capacitor RMS
current for VIN = 12V:
IO-RMS = 1.13 x 0.49 x (0.37 x 0.63)0.5 = 0.267A PCO = 0.267 x 0.003 = 1 mW
(62)
BOOST INDUCTOR LOSS
PDCR = IL2 x DCR PDCR = 0.492 x 0.18 = 43 mW
(63)
Core loss in the inductor is assumed to be equal to the DCR loss, adding an additional 43 mW to the total
inductor loss.
TOTAL LOSS
PLOSS = Sum of All Loss Terms = 0.38W
(64)
EFFICIENCY
η = 5.9/(5.9 + 0.38) = 94%
(65)
Layout Considerations
To produce an optimal power solution with the LM3430, good layout and design of the PCB are as important as
the component selection. The following are several guidelines to aid in creating a good layout.
FILTER CAPACITORS
The low-value ceramic filter capacitors are most effective when the inductance of the current loops that they filter
is minimized. Place CINX as close as possible to the VIN and GND pins of the LM3430. Place COX close to the
load. CCS should be placed right next to RSNS, and CF next to the VCC and GND pins of the LM3430.
26
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SENSE LINES
The top of RSNS should be connected to the CS pin with a separate trace made as short as possible. Route this
trace away from the inductor and the switch node (where D1, Q1, and L1 connect). For the voltage loop, keep
RFB1/2 close to the LM3430 and run a trace from as close as possible to the positive side of COX to RFB2. As with
the CS line, the FB line should be routed away from the inductor and the switch node. These measures minimize
the length of high impedance lines and reduce noise pickup.
COMPACT LAYOUT
Parasitic inductance can be reduced by keeping the power path components close together and keeping the
area of the loops that high currents travel small. Short, thick traces or copper pours (shapes) are best. In
particular, the switch node should be just large enough to connect all the components together without excessive
heating from the current it carries. The LM3430 (boost converter) operates in two distinct cycles whose high
current paths are shown in Figure 22:
+
-
Figure 22. Boost Converter Current Loops
The dark grey, inner loops represents the high current paths during the MOSFET on-time. The light grey, outer
loop represents the high current path during the off-time.
GROUND PLANE AND SHAPE ROUTING
The diagram of Figure 22 is also useful for analyzing the flow of continuous current vs. the flow of pulsating
currents. The circuit paths with current flow during both the on-time and off-time are considered to be continuous
current, while those that carry current during the on-time or off-time only are pulsating currents. Preference in
routing should be given to the pulsating current paths, as these are the portions of the circuit most likely to emit
EMI. The ground plane of a PCB is a conductor and return path, and it is susceptible to noise injection just as
any other circuit path. The continuous current paths on the ground net can be routed on the system ground plane
with less risk of injecting noise into other circuits. The path between the input source, input capacitor and the
power switch and the path between the output capacitor and the load are examples of continuous current paths.
In contrast, the path between the grounded side of the power switch and the negative output capacitor terminal
carries a large pulsating current. This path should be routed with a short, thick shape, preferably on the
component side of the PCB. Multiple vias in parallel should be used right at the negative pads of the input and
output capacitors to connect the component side shapes to the ground plane. Vias should not be placed directly
at the grounded side of the power switch (or RSNS) as they tend to inject noise into the ground plane. A second
pulsating current loop that is often ignored but must be kept small is the gate drive loop formed by the OUT and
VCC pins, Q1, RSNS and capacitor CF.
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LM3430
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BOM for Example Circuit
28
ID
Part Number
Type
Size
U1
LM3430
Low-Side Controller
WSON-12
Q1
Si4850EY
MOSFET
SO-8
D1
CMHSH5-4
Schottky Diode
L1
SLF7045T-470M90-1PF
Inductor
Cin
C3216X7R1E335M
Capacitor
Co
C3216X7R1H105M
Parameters
Qty
Vendor
1
TI
60V, 31mΩ, 18nC
1
Vishay
SOD-123
40V, 0.5A
1
Central Semi
7.0 x7.0 x 4.5mm
47µH, 0.9A, 180mΩ
1
TDK
1206
3.3µF, 25V, 3mΩ
1
TDK
Capacitor
1206
1µF, 50V, 3mΩ
1
TDK
Cf
C2012X7R1E105K
Capacitor
0805
1µF, 25V
1
TDK
Cinx
Cox
VJ0805Y104KXXAT
Capacitor
0805
100nF 10%
1
Vishay
C1
VJ0805A391KXXAT
Capacitor
0805
390pF 10%
1
Vishay
C2
VJ0805Y393KXXAT
Capacitor
0805
39nF 10%
1
Vishay
Css
VJ0805Y103KXXAT
Capacitor
0805
10nF 10%
1
Vishay
Ccs
VJ0805Y102KXXAT
Capacitor
0805
1nF 10%
1
Vishay
R1
CRCW08052001F
Resistor
0805
2kΩ 1%
1
Vishay
Rfb1
CRCW08057870F
Resistor
0805
787Ω 1%
1
Vishay
Rfb2
CRCW08052002F
Resistor
0805
20kΩ 1%
1
Vishay
Rs1
CRCW0805101J
Resistor
0805
100Ω 5%
1
Vishay
Rsns
ERJ8BQFR51V
Resistor
1206
0.51Ω 1%, 0.33W
1
Panasonic
Rt
CRCW08052742F
Resistor
0805
27.4kΩ 1%
1
Vishay
Ruv1
Ruv2
CRCW08051002F
Resistor
0805
10kΩ 1%
2
Vishay
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SNVS472B – JANUARY 2007 – REVISED MAY 2013
REVISION HISTORY
Changes from Revision B (May 2013) to Revision C
Page
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29
PACKAGE OPTION ADDENDUM
www.ti.com
16-Oct-2015
PACKAGING INFORMATION
Orderable Device
Status
(1)
Package Type Package Pins Package
Drawing
Qty
Eco Plan
Lead/Ball Finish
MSL Peak Temp
(2)
(6)
(3)
Op Temp (°C)
Device Marking
(4/5)
LM3430SD/NOPB
LIFEBUY
WSON
DQB
12
1000
Green (RoHS
& no Sb/Br)
CU SN
Level-1-260C-UNLIM
-40 to 125
L3430
LM3430SDX/NOPB
LIFEBUY
WSON
DQB
12
4500
Green (RoHS
& no Sb/Br)
CU SN
Level-1-260C-UNLIM
-40 to 125
L3430
(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.
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.
Addendum-Page 1
Samples
PACKAGE OPTION ADDENDUM
www.ti.com
16-Oct-2015
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
LM3430SD/NOPB
WSON
DQB
12
1000
178.0
12.4
3.3
3.3
1.0
8.0
12.0
Q1
LM3430SDX/NOPB
WSON
DQB
12
4500
330.0
12.4
3.3
3.3
1.0
8.0
12.0
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)
LM3430SD/NOPB
WSON
DQB
12
1000
210.0
185.0
35.0
LM3430SDX/NOPB
WSON
DQB
12
4500
367.0
367.0
35.0
Pack Materials-Page 2
MECHANICAL DATA
DQB0012A
SDF12A (Rev B)
www.ti.com
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