LINEAR TECHNOLOGY LT3435 Technical data

Step-Down Switching Regulator
with 100µA Quiescent Current
FEATURES
Wide Input Range: 3.3V to 60V
3A Peak Switch Current
Burst Mode® Operation: 100µA Quiescent Current**
Low Shutdown Current: IQ < 1µA
Power Good Flag with Programmable Threshold
Load Dump Protection to 60V
500kHz Switching Frequency
Saturating Switch Design: 0.1 On-Resistance
Peak Switch Current Maintained Over Full Duty Cycle Range*
1.25V Feedback Reference Voltage
Easily Synchronizable
Soft-Start Capability
Small 16-Pin Thermally Enhanced TSSOP Package
U
APPLICATIO S
High Voltage Power Conversion
14V and 42V Automotive Systems
Industrial Power Systems
Distributed Power Systems
Battery-Powered Systems
USB Powered Systems
, LTC and LT are registered trademarks of Linear Technology Corporation.
Burst Mode is a registered trademark of Linear Technology Corporation. All other trademarks are the property of their respective owners. *Protected by U.S. Patents including 6498466 **See Burst Mode Operation section for conditions.
LT3435
High Voltage 3A, 500kHz
U
The LT regulator that accepts input voltages up to 60V. A high efficiency 3A, 0.1 switch is included on the die along with all the necessary oscillator, control and logic circuitry. Current mode topology is used for fast transient response and good loop stability.
Innovative design techniques along with a new high volt­age process achieve high efficiency over a wide input range. Efficiency is maintained over a wide output current range by employing Burst Mode operation at low currents, utilizing the output to bias the internal circuitry, and by using a supply boost capacitor to fully saturate the power switch. Patented circuitry maintains peak switch current over the full duty cycle range.* Shutdown reduces input supply current to less than 1µA. External synchronization can be implemented by driving the SYNC pin with logic-level inputs. A single capacitor from the C provides a controlled output voltage ramp (soft-start). The device also has a power good flag with a programmable threshold and time-out and thermal shutdown protection.
The LT3435 is available in a 16-pin TSSOP package with an exposed pad leadframe for low thermal resistance.
®
3435 is a 500kHz monolithic buck switching
pin to the output
SS
TYPICAL APPLICATIO
14V to 3.3V Step-Down Converter with
100µA No Load Quiescent Current
4700pF
10k
V
IN
1µF
4.7µF 100V CER
470pF
V
IN
SHDN
V
C
C
T
SYNC GND
LT3435
BOOST
SW
C
V
BIAS
PGFB
0.33µF
0.1µF
SS
27pF
FB
PG
15µH
B360A
U
165k
100k
Efficiency and Power Loss
vs Load CurrentSupply Current vs Input Voltage
3435 TA02
10
10
1
0.1
0.01
0.001
3435fa
POWER LOSS (W)
60
100
VIN = 12V
90
80
V
OUT
70
60
50
40
EFFICIENCY (%)
30
20
10
0
0.0001
= 5V
EFFICIENCY
V
= 3.3V
OUT
0.001 LOAD CURRENT (A)
0.01
TYPICAL POWER LOSS
0.1 1
150
V
OUT
3.3V
4148
1%
1%
2A
100µF
+
10V TANT
3435 TA01
125
100
75
50
SUPPLY CURRENT (µA)
25
0
10
0
20
INPUT VOLTAGE (V)
30 40
V
= 3.3V
OUT
= 25°C
T
A
50
3435 TA03
1
LT3435
FE PACKAGE
16-LEAD PLASTIC TSSOP
1
2
3
4
5
6
7
8
TOP VIEW
16
15
14
13
12
11
10
9
NC
SW
V
IN
V
IN
SW
BOOST
C
T
GND
PGOOD
SHDN
SYNC
PGFB
FB
V
C
BIAS
C
SS
17
WW
W
U
ABSOLUTE AXI U RATI GS
(Note 1)
VIN, SHDN, BIAS, PGOOD, SW ............................... 60V
BOOST Pin Above SW ............................................ 35V
BOOST Pin Voltage ................................................. 68V
SYNC, CSS, PGFB, FB................................................ 6V
Operating JunctionTemperature Range
(Note 2) ........................................... – 40°C to 125°C
Storage Temperature Range ................. –65°C to 150°C
Lead Temperature (Soldering, 10 sec).................. 300°C
UUW
PACKAGE/ORDER I FOR ATIO
T
= 125°C, θJA = 45°C/W, θ
EXPOSED PAD (PIN 17) IS GND, MUST BE SOLDERED TO GND (PIN 8)
JMAX
ORDER PART NUMBER
LT3435EFE LT3435IFE
Order Options Tape and Reel: Add #TR Lead Free: Add #PBF Lead Free Tape and Reel: Add #TRPBF
Lead Free Part Marking: http://www.linear.com/leadfree/
Consult LTC Marketing for parts specified with wider operating temperature ranges.
= 10°C/W
JC(PAD)
FE PART MARKING
3435EFE 3435IFE
ELECTRICAL CHARACTERISTICS
temperature range, otherwise specifications are at T
The ● denotes the specifications which apply over the full operating
= 25°C. VIN = 12V, SHDN = 12V, BIAS = 5V, FB/PGFB = 1.25V, CSS/SYNC = 0V
J
unless otherwise noted.
SYMBOL PARAMETER CONDITIONS MIN TYP MAX UNITS
V
SHDN
I
SHDN
I
VINS
I
VIN
I
BIASS
I
BIAS
V
REF
I
FB
2
SHDN Threshold 1.15 1.3 1.45 V
SHDN Input Current SHDN = 12V
Minimum Input Voltage (Note 3)
Supply Shutdown Current SHDN = 0V, BOOST = 0V, FB/PGFB = 0V 0.1 2 µA
Supply Sleep Current (Note 4) BIAS = 0V, FB = 1.35V
FB = 1.35V
Supply Quiescent Current BIAS = 0V, FB = 1.15V 3.3 7 mA
BIAS = 5V, FB = 1.15V 2.6 6 mA
Minimum BIAS Voltage (Note 5)
BIAS Sleep Current (Note 4)
BIAS Quiescent Current SYNC = 3.3V 700 900 µA
Minimum Boost Voltage (Note 6) ISW = 1.5A 1.8 V
Input Boost Current (Note 7) ISW = 3A 65 85 mA
Reference Voltage (V
FB Input Bias Current 75 200 nA
EA Voltage Gain (Note 8) 900 V/V
EA Voltage g
m
) 3.3V < V
REF
dI(VC)= ±10µA 400 650 900 µMho
VIN
< 60V
1.225 1.25 1.275 V
520 µA
2.4 3 V
170 250 µA
45 75 µA
2.7 3.1 V
125 180 µA
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LT3435
ELECTRICAL CHARACTERISTICS
temperature range, otherwise specifications are at T
The ● denotes the specifications which apply over the full operating
= 25°C. VIN = 12V, SHDN = 12V, BIAS = 5V, FB/PGFB = 1.25V, CSS/SYNC = 0V
J
unless otherwise noted.
SYMBOL PARAMETER CONDITIONS MIN TYP MAX UNITS
EA Source Current FB = 1.15V 20 40 55 µA
EA Sink Current FB = 1.35V 15 30 40 µA
I
PK
I
CSS
I
PGFB
V
PGFB
I
CT
V
CT
VC to SW g
VC High Clamp FB = 1.15V 2.1 2.2 2.4 V
SW Current Limit
Switch On Resistance (Note 9)
Switching Frequency
Maximum Duty Cycle 86 92 %
Minimum SYNC Amplitude 1.5 2.0 V
SYNC Frequency Range 575 700 kHz SYNC Input Impedance 45 k
CSS Current Threshold (Note 10) FB = 0V 7 13 20 µA
PGFB Input Current 25 100 nA
PGFB Voltage Threshold (Note 11)
CT Source Current (Note 11) 2 3.6 5.5 µA
CT Sink Current (Note 11) 1 2 mA
CT Voltage Threshold (Note 11) 1.16 1.2 1.26 V
PG Leakage (Note 11) 0.1 1 µA
PG Sink Current (Note 11) PGFB = 1V, PG = 400mV 100 200 µA
m
3 5.2 6.5 A
425 500 575 kHz
88 90 92 %
6A/V
0.1 0.25
Note 1: Stresses beyond those listed under Absolute Maximum Ratings may cause permanent damage to the device. Exposure to any Absolute Maximum Rating condition for extended periods may affect device reliability and lifetime.
Note 2: The LT3435EFE is guaranteed to meet performance specifications from 0°C to 125°C junction temperature. Specifications over the –40°C to 125°C operating junction temperature range are assured by design, characterization and correlation with statistical process controls. The LT3435IFE is guaranteed and tested over the full –40°C to 125°C operating junction temperature range.
Note 3: Minimum input voltage is defined as the voltage where switching starts. Actual minimum input voltage to maintain a regulated output will depend upon output voltage and load current. See Applications Information.
Note 4: Supply input current is the quiescent current drawn by the input pin. Its typical value depends on the voltage on the BIAS pin and operating state of the LT3435. With the BIAS pin at 0V, all of the quiescent current required to operate the LT3435 will be provided by the V BIAS voltage above its minimum input voltage, a portion of the total quiescent current will be supplied by the BIAS pin. Supply sleep current is defined as the quiescent current during the “sleep” portion of Burst Mode operation. See Applications Information for determining application supply currents.
pin. With the
IN
Note 5: Minimum BIAS voltage is the voltage on the BIAS pin when I sourced into the pin.
Note 6: This is the minimum voltage across the boost capacitor needed to guarantee full saturation of the internal power switch.
Note 7: Boost current is the current flowing into the BOOST pin with the pin held 3.3V above input voltage. It flows only during switch on time.
Note 8: Gain is measured with a V Note 9: Switch on resistance is calculated by dividing V
the forced current (3A). See Typical Performance Characteristics for the graph of switch voltage at other currents.
Note 10: The C
pin which results in an increase in sink current from the VC pin.
the C
SS
See the Soft-Start section in Applications Information. Note 11: The PGFB threshold is defined as the percentage of V
which causes the current source output of the C sinking (below threshold) to sourcing current (above threshold). When sourcing current, the voltage on the C internally. When the clamp is activated, the output of the PG pin will be set to a high impedance state. When the C be set active low with a current sink capability of 200µA.
threshold is defined as the value of current sourced into
SS
swing from 1.15V to 750mV.
C
to SW voltage by
IN
pin to change from
T
pin rises until it is clamped
T
clamp is inactive the PG pin will
T
REF
BIAS
voltage
is
3435fa
3
LT3435
UW
TYPICAL PERFOR A CE CHARACTERISTICS
FB Voltage Oscillator Frequency SHDN Threshold
1.30
1.29
1.28
1.27
1.26
1.25
1.24
VOLTAGE (V)
1.23
1.22
1.21
1.20 –50 0
–25
50
25
TEMPERATURE (°C)
100
125
3435 G01
75
550
540
530
520
510
500
490
FREQUENCY (kHz)
480
470
460
450
–50
–25
50
25
0
TEMPERATURE (°C)
1.40
1.35
1.30
1.25
1.20
VOLTAGE (V)
0.15
1.10
1.05
100
125
3435 G02
75
1.00 –50 0
–25
TEMPERATURE (°C)
50
25
75
100
125
3435 G03
SHDN Pin Current
5.5 TJ = 25°C
5.0
4.5
4.0
3.5
3.0
2.5
CURRENT (µA)
2.0
1.5
1.0
0
10
0
Bias Sleep Current
200
180
160
140
120
100
80
CURRENT (µA)
60
40
20
0
–50 0
–25
30 40
20
SHDN VOLTAGE (V)
50
25
TEMPERATURE (°C)
Shutdown Supply Current Sleep Mode Supply Current
25
20
15
10
CURRENT (µA)
5
0
50
60
3435 G04
–50 0
VIN = 42V VIN = 12V
–25
TEMPERATURE (°C)
VIN = 60V
50
25
75
100
125
3435 G05
PGFB Threshold
1.20
1.18
1.16
1.14
1.12
1.10
1.08
VOLTAGE (V)
1.06
1.04
1.02
1.00
100
125
3435 G07
75
–50 0
–25
TEMPERATURE (°C)
50
25
75
100
125
3435 G08
200
180
160
140
120
100
80
CURRENT (µA)
60
40
20
0
–50 0
–25
PG Sink Current
250
200
150
100
CURRENT (µA)
50
0
–50 0
–25
V
= 0V
BIAS
V
= 5V
BIAS
50
25
TEMPERATURE (°C)
50
25
TEMPERATURE (°C)
100
100
125
3435 G06
125
3435 G09
75
75
4
3435fa
UW
FB VOLTAGE (V)
0
0
NORMALIZED FREQUENCY (%)
20
30
40
50
60
70
80
90
10
0.25 0.50 0.75
3435 G12
1.00
100
1.25
SWITCH CURRENT (mA)
0
0
BOOST CURRENT (mA)
10
30
2000
70
60
3435 G18
20
1000
500
2500
1500 3000
40
50
TYPICAL PERFOR A CE CHARACTERISTICS
LT3435
Switch Peak Current Limit
6.0
5.5
5.0
4.5
4.0
PEAK SWITCH CURRENT (A)
3.5
3.0
–25 –0 25 50
–50
TEMPERATURE (°C)
Switch On Voltage (V
500
450
400
350
300
250
200
VOLTAGE (mV)
150
100
50
0
0.5
1.0 2.0 3.0
1.5
LOAD CURRENT (A)
Soft-Start Current Threshold vs FB Voltage
50
TJ = 25°C
45
40
35
30
25
20
CURRENT (µA)
15
10
5
0
0
START-UP
0
0.2
RUNNING
START-UP
RUNNING
0.5
75 100 125
3435 G10
) Minimum Input Voltage
CESAT
TJ = 125°C
TJ = 25°C
TJ = –40°C
2.5
3435 G13
8.0
7.5
7.0
6.5
6.0
5.5
5.0
INPUT VOLTAGE (V)
4.5
4.0
3.5
3.0
0.6 0.8
0.4 FB VOLTAGE (V)
V
= 5V
OUT
V
OUT
1.0
1.5 3.0
LOAD CURRENT (A)
2.0
SOFT-START DEFEATED
1.0
3435 G11
= 3.3V
2.5
3435 G15
1.2
1000
900
800
700
600
500
400
300
LOAD CURRENT (mA)
200
100
Oscillator Frequency vs FB Voltage
Burst Mode Threshold vs Input Voltage
V
= 3.3V
0
5
OUT
L = 15µH
= 100µF
C
OUT
= 25°C
T
A
BURST MODE EXIT (INCREASING LOAD)
BURST MODE ENTER (DECREASING LOAD)
10 20
INPUT VOLTAGE (V)
15
3435 G16
Minimum On-Time for Continuous Mode Operation
600
LOAD CURRENT = 1A
550
500
450
400
350
300
ON TIME (ns)
250
200
150
100
–50
–25
50
25
0
TEMPERATURE (°C)
Maximum Synchronization Frequency vs Temperature Boost Current vs Switch Current
1000
950
900
850
800
750
700
FREQUENCY (kHz)
650
600
550
500
100
125
3435 G17
75
–50
0
–25
TEMPERATURE (°C)
50
25
75
100
125
3435 G14
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5
LT3435
UW
TYPICAL PERFOR A CE CHARACTERISTICS
4.0
3.5
3.0
2.5
2.0
1.5
OUTPUT VOLTAGE (V)
1.0
0.5
V
OUT
50mV/DIV
AC-COUPLED
I
SW
500mA/DIV
Dropout Operation Dropout Operation
6
V
V
= 3.3V
OUT
BOOST DIODE = DIODES INC DFLS160
LOAD CURRENT = 2.5A
LOAD CURRENT = 250mA
0
2 2.5 3 3.5 4 4.5 5 5.5 6
INPUT VOLTAGE (V)
Burst Mode Operation
3435 G19
V
OUT
200mV/DIV
AC-COUPLED
I
OUT
1A/DIV
= 5V
OUT
BOOST DIODE = DIODES INC DFLS160
5
4
3
2
OUTPUT VOLTAGE (V)
1
0
2 2.5 3 3.5 4 4.5 5 5.5 6.5 7 7.56
LOAD CURRENT = 250mA
INPUT VOLTAGE (V)
No Load 2A Step Response Step Response
LOAD CURRENT = 2.5A
3435 G20
V
OUT
50mV/DIV
AC-COUPLED
I
SW
500mA/DIV
V
OUT
200mV/DIV
AC-COUPLED
I
OUT
1A/DIV
Burst Mode Operation
V
= 12V 10ms/DIV
IN
V
= 3.3V
OUT
3435 G21
V
V
= 12V 10µs/DIV
IN
V
= 3.3V
OUT
U
3435 G22
UU
= 12V 500µs/DIV
IN
V
= 3.3V
OUT
= 100µF
C
OUT
PI FU CTIO S
NC (Pin 1): No Connection.
SW (Pins 2, 5): The SW pin is the emitter of the on-chip
power NPN switch. This pin is driven up to the input pin voltage during switch on time. Inductor current drives the SW pin negative during switch off time. Negative voltage is clamped with the external catch diode. Maximum nega­tive switch voltage allowed is –0.8V.
(Pins 3, 4): This is the collector of the on-chip power
V
IN
NPN switch. V a voltage on the BIAS pin is not present. High di/dt edges occur on this pin during switch turn on and off. Keep the path short from the VIN pin through the input bypass capacitor, through the catch diode back to SW. All trace
powers the internal control circuitry when
IN
3435 G23
= 12V 500µs/DIV
V
IN
V
= 3.3V
OUT
C
= 100µF
OUT
= 500mA
I
LOAD(DC)
3435 G24
inductance on this path will create a voltage spike at switch off, adding to the VCE voltage across the internal NPN.
BOOST (Pin 6): The BOOST pin is used to provide a drive voltage, higher than the input voltage, to the internal bipolar NPN power switch. Without this added voltage, the typical switch voltage loss would be about 1.5V. The additional BOOST voltage allows the switch to saturate and its voltage loss approximates that of a 0.1 FET structure.
CT (Pin 7): A capacitor on the CT pin determines the amount of delay time between the PGFB pin exceeding its thresh­old (V
) and the PG pin set to a high impedance state.
PGFB
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6
LT3435
U
UU
PI FU CTIO S
When the PGFB pin rises above V from the C
pin into the external capacitor. When the volt-
T
age on the external capacitor reaches an internal clamp (V
), the PG pin becomes a high impedance node. The
CT
resultant PG delay time is given by t = C voltage on the PGFB pin drops below V discharged rapidly to 0V and PG will be active low with a 200µA sink capability. If the C
pin is clamped (Power Good
T
condition) during normal operation and SHDN is taken low, the C
pin will be discharged and a delay period will occur
T
when SHDN is returned high. See the Power Good section in Applications Information for details.
GND (Pins 8, 17): The GND pin connection acts as the reference for the regulated output, so load regulation will suffer if the “ground” end of the load is not at the same voltage as the GND pin of the IC. This condition will occur when load current or other currents flow through metal paths between the GND pin and the load ground. Keep the path between the GND pin and the load ground short and use a ground plane when possible. The GND pin also acts as a heat sink and should be soldered (along with the exposed leadframe) to the copper ground plane to reduce thermal resistance (see Applications Information).
CSS (Pin 9): A capacitor from the CSS pin to the regulated output voltage determines the output voltage ramp rate during start-up. When the current through the C tor exceeds the C the output is limited. The C
threshold (I
SS
threshold is proportional to
SS
the FB voltage (see Typical Performance Characteristics) and is defeated for FB voltage greater than 0.9V (typical). See Soft-Start section in Applications Information for details.
BIAS (Pin 10): The BIAS pin is used to improve efficiency when operating at higher input voltages and light load current. Connecting this pin to the regulated output volt­age forces most of the internal circuitry to draw its operating current from the output voltage rather than the input supply. This architecture increases efficiency espe­cially when the input voltage is much higher than the output. Minimum output voltage setting for this mode of operation is 3V.
(Pin 11): The VC pin is the output of the error amplifier
V
C
and the input of the peak switch current comparator. It is
, current is sourced
PGFB
• VCT/ICT. If the
CT
, CCT will be
PGFB
SS
), the voltage ramp of
CSS
capaci-
normally used for frequency compensation, but can also serve as a current clamp or control loop override. V
sits
C
at about 0.45V for light loads and 2.2V at maximum load. During the sleep portion of Burst Mode operation, the V
C
pin is held at a voltage slightly below the burst threshold for better transient response. Driving the V
pin to ground
C
will disable switching and place the IC into sleep mode.
FB (Pin 12): The feedback pin is used to determine the output voltage using an external voltage divider from the output that generates 1.25V at the FB pin . When the FB pin drops below 0.9V, switching frequency is reduced, the SYNC function is disabled and output ramp rate control is enabled via the C
pin. See the Feedback section in
SS
Applications Information for details.
PGFB (PIN 13): The PGFB pin is the positive input to a comparator whose negative input is set at V PGFB is taken above V the C
pin starting the PG delay period. When the voltage
T
on the PGFB pin drops below V
, current (I
PGFB
PGFB
) is sourced into
CSS
, the CT pin is rapidly
PGFB
. When
discharged resetting the PG delay period. The PGFB volt­age is typically generated by a resistive divider from the regulated output or input supply. See Power Good section in Applications Information for details.
SYNC (Pin 14): The SYNC pin is used to synchronize the internal oscillator to an external signal. It is directly logic compatible and can be driven with any signal between 5% and 75% duty cycle. The synchronizing range is equal to maximum initial operating frequency up to 700kHz. When the voltage on the FB pin is below 0.9V the SYNC function is disabled. See the Synchronizing section in Applications Information for details.
SHDN (Pin 15): The SHDN pin is used to turn off the regulator and to reduce input current to less than 1µA. The SHDN pin requires a voltage above 1.3V with a typical source current of 5µA to take the IC out of the shutdown state.
PG (Pin 16): The PG pin is functional only when the SHDN pin is above its threshold, and is active low when the internal clamp on the C
pin is below its clamp level and
T
high impedance when the clamp is active. The PG pin has a typical sink capability of 200µA. See the Power Good section in Applications Information for details.
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7
LT3435
BLOCK DIAGRA
V
IN
4
BIAS
10
SYNC
14
SHDN
15
+
SHDN COMP
1.3V
INTERNAL REF
UNDERVOLTAGE
W
LOCKOUT
THERMAL
SHUTDOWN
2.4V
SLOPE
COMP
500kHz
OSCILLATOR
ANTISLOPE
COMP
Σ
CURRENT
COMP
R
S
+
SWITCH
LATCH
Q
DRIVER
CIRCUITRY
BOOST
SW
6
2
C
SS
9
FB
12
1.25V
V
C
11
PGFB
13
1.12V
C
T
7
SOFT-START
FOLDBACK
DETECT
ERROR
AMP
+
+
PG
COMP
BURST MODE
DETECT
V
C
CLAMP
1.2V C
T
CLAMP
GND
PGND
PG
16
17
8
3435 BD
Figure 1. LT3435 Block Diagram
The LT3435 is a constant frequency, current mode buck converter. This means that there is an internal clock and two feedback loops that control the duty cycle of the power switch. In addition to the normal error amplifier, there is a current sense amplifier that monitors switch current on a cycle-by-cycle basis. A switch cycle starts with an oscilla­tor pulse which sets the RS latch to turn the switch on. When switch current reaches a level set by the current compara­tor the latch is reset and the switch turns off. Output volt­age control is obtained by using the output of the error amplifier to set the switch current trip point. This technique means that the error amplifier commands current to be
8
delivered to the output rather than voltage. A voltage fed system will have low phase shift up to the resonant fre­quency of the inductor and output capacitor, then an abrupt 180° shift will occur. The current fed system will have 90° phase shift at a much lower frequency, but will not have the additional 90° shift until well beyond the LC resonant fre­quency. This makes it much easier to frequency compen­sate the feedback loop and also gives much quicker tran­sient response.
Most of the circuitry of the LT3435 operates from an internal 2.4V bias line. The bias regulator normally draws
3435fa
BLOCK DIAGRA
LT3435
W
power from the VIN pin, but if the BIAS pin is connected to an external voltage higher than 3V bias power will be drawn from the external source (typically the regulated output voltage). This improves efficiency.
High switch efficiency is attained by using the BOOST pin to provide a voltage to the switch driver which is higher than the input voltage, allowing switch to be saturated. This boosted voltage is generated with an external capaci­tor and diode.
WUUU
APPLICATIO S I FOR ATIO
FEEDBACK PIN FUNCTIONS
The feedback (FB) pin on the LT3435 is used to set output voltage and provide several overload protection features. The first part of this section deals with selecting resistors to set output voltage and the remaining part talks about frequency foldback and soft-start features. Please read both parts before committing to a final design.
Referring to Figure 2, the output voltage is determined by a voltage divider from V
1.25V at the FB pin. Since the output divider is a load on the output care must be taken when choosing the resistor divider values. For light load applications the resistor values should be as large as possible to achieve peak efficiency in Burst Mode operation. Extremely large values for resistor R1 will cause an output voltage error due to the 50nA FB pin input current. The suggested value for the output divider resistor (see Figure 2) from FB to ground (R2) is 100k or less. A formula for R1 is shown below. A table of standard 1% values is shown in Table 1 for common output voltages.
to ground which generates
OUT
To further optimize efficiency, the LT3435 automatically switches to Burst Mode operation in light load situations. In Burst Mode operation, all circuitry associated with controlling the output switch is shut down reducing the input supply current to 45µA.
The LT3435 contains a power good flag with a program­mable threshold and delay time. A logic-level low on the SHDN pin disables the IC and reduces input suppy current to less than 1µA.
Table 1
OUTPUT R1 OUTPUT
VOLTAGE R2 NEAREST (1%) ERROR
(V) (kΩ, 1%) (kΩ)(%)
2.5 100 100 0
3 100 140 0
3.3 100 165 0.38
5 100 301 0.25
6 100 383 0.63
8 100 536 – 0.63
10 100 698 – 0.25
12 100 866 0.63
V
LT3435
OSCILLATOR
500kHz
SOFT-START
FOLDBACK
DETECT
SW
2
C
C1
SS
9
OUT
R1
RR
12
=+•
V
125 2 50
.•
125
–.
OUT
RnA
More Than Just Voltage Feedback
The FB pin is used for more than just output voltage sensing. It also reduces switching frequency and con­trols the soft-start voltage ramp rate when output voltage is below the regulated level (see the Frequency Foldback
ERROR
AMP
+
1.25V
Figure 2. Feedback Network
FB
12
R2
V
C
11
3435 F02
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APPLICATIO S I FOR ATIO
and Soft-Start Current graphs in Typical Performance Characteristics).
Frequency foldback is done to control power dissipation in both the IC and in the external diode and inductor during short-circuit conditions. A shorted output requires the switching regulator to operate at very low duty cycles. As a result the average current through the diode and induc­tor is equal to the short-circuit current limit of the switch (typically 4.7A for the LT3435). Minimum switch on time limitations would prevent the switcher from attaining a sufficiently low duty cycle if switching frequency were maintained at 500kHz, so frequency is reduced by about 4:1 when the FB pin voltage drops below 0.4V (see Frequency Foldback graph). In addition, if the current in the switch exceeds 1.5 times the current limitations speci­fied by the V LT3435 will skip the next switch cycle. As the feedback voltage rises, the switching frequency increases to 500kHz with 0.95V on the FB pin. During frequency foldback, external syncronization is disabled to prevent interference with foldback operation. Frequency foldback does not affect operation during normal load conditions.
In addition to lowering switching frequency the soft-start ramp rate is also affected by the feedback voltage. Large capacitive loads or high input voltages can cause a high input current surge during start-up. The soft-start func­tion reduces input current surge by regulating switch current via the VC pin to maintain a constant voltage ramp rate (dV/dt) at the output. A capacitor (C1 in Figure 2) from the C dV/dt. When the feedback voltage is below 0.4V, the V will rise, resulting in an increase in switch current and output voltage. If the dV/dt of the output causes the current through the CSS capacitor to exceed I reduced resulting in a constant dV/dt at the output. As the feedback voltage increases I increased dV/dt until the soft-start function is defeated with 0.9V present at the FB pin. The soft-start function does not affect operation during normal load conditions. However, if a momentary short (brown out condition) is present at the output which causes the FB voltage to drop below 0.9V, the soft-start circuitry will become active.
pin to the output determines the maximum output
SS
pin, due to minimum switch on time, the
C
pin
C
the VC voltage is
CSS
increases, resulting in an
CSS
INPUT CAPACITOR
Step-down regulators draw current from the input supply in pulses. The rise and fall times of these pulses are very fast. The input capacitor is required to reduce the voltage ripple this causes at the input of LT3435 and force the switching current into a tight local loop, thereby minimiz­ing EMI. The RMS ripple current can be calculated from:
I
I
RIPPLE RMS
Ceramic capacitors are ideal for input bypassing. At 500kHz switching frequency input capacitor values in the range of
4.7µF to 20µF are suitable for most applications. If opera- tion is required close to the minimum input required by the LT3435 a larger value may be required. This is to prevent excessive ripple causing dips below the minimum operat­ing voltage resulting in erratic operation.
Input voltage transients caused by input voltage steps or by hot plugging the LT3435 to a pre-powered source such as a wall adapter can exceed maximum V sudden application of input voltage will cause a large surge of current in the input leads that will store energy in the parasitic inductance of the leads. This energy will cause the input voltage to swing above the DC level of input power source and it may exceed the maximum voltage rating of the input capacitor and LT3435. All input voltage transient sequences should be observed at the V the LT3435 to ensure that absolute maximum voltage ratings are not violated.
The easiest way to suppress input voltage transients is to add a small aluminum electrolytic capacitor in parallel with the low ESR input capacitor. The selected capacitor needs to have the right amount of ESR to critically damp the resonant circuit formed by the input lead inductance and the input capacitor. The typical values of ESR will fall in the range of 0.5 to 2 and capacitance will fall in the range of 5µF to 50µF.
If tantalum capacitors are used, values in the 22µF to 470µF range are generally needed to minimize ESR and meet ripple current and surge ratings. Care should be
OUT
VVV
V
OUT IN OUT()
IN
=
()
ratings. The
IN
pin of
IN
10
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I
VVV
VLf
OUT IN OUT
IN
P-P
=
()
()()()
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APPLICATIO S I FOR ATIO
LT3435
taken to ensure the ripple and surge ratings are not exceeded. The AVX TPS and Kemet T495 series are surge rated AVX recommends derating capacitor operating volt­age by 2:1 for high surge applications.
OUTPUT CAPACITOR
The output capacitor is normally chosen by its effective series resistance (ESR) because this is what determines output ripple voltage. To get low ESR takes volume, so physically smaller capacitors have higher ESR. The ESR range for typical LT3435 applications is 0.05 to 0.2. A typical output capacitor is an AVX type TPS, 100µF at 10V, with a guaranteed ESR less than 0.1. This is a “D” size surface mount solid tantalum capacitor. TPS capacitors are specially constructed and tested for low ESR, so they give the lowest ESR for a given volume. The value in microfarads is not particularly critical and values from 22µF to greater than 500µF work well, but you cannot cheat Mother Nature on ESR. If you find a tiny 22µF solid tantalum capacitor, it will have high ESR and output ripple voltage could be unacceptable. Table 2 shows some typical solid tantalum surface mount capacitors.
Table 2. Surface Mount Solid Tantalum Capacitor ESR and Ripple Current
E CASE SIZE ESR MAX () RIPPLE CURRENT (A)
AVX TPS 0.1 to 0.3 0.7 to 1.1
D CASE SIZE
AVX TPS 0.1 to 0.3 0.7 to 1.1
C CASE SIZE
AVX TPS 0.2 0.5
Unlike the input capacitor RMS, ripple current in the output capacitor is normally low enough that ripple cur­rent rating is not an issue. The current waveform is triangular with a typical value of 200mA to calculate this is:
Output capacitor ripple current (RMS)
VVV
029
.–
OUT IN OUT
I
RIPPLE RMS
CERAMIC CAPACITORS
Higher value, lower cost ceramic capacitors are now becoming available. They are generally chosen for their good high frequency operation, small size and very low ESR (effective series resistance). Low ESR reduces output ripple voltage but also removes a useful zero in the loop frequency response, common to tantalum capacitors. To compensate for this a resistor R with the V must be taken however since this resistor sets the high frequency gain of the error amplifier including the gain at the switching frequency. If the gain of the error amplifier is high enough at the switching frequency output ripple voltage (although smaller for a ceramic output capacitor) may still affect the proper operation of the regulator. A filter capacitor C with a small feedforward capacitor C control possible ripple at the V
OUTPUT RIPPLE VOLTAGE
=
()
compensation capacitor CC (Figure 10). Care
C
F
()( )
LfV
()()( )
in parallel with the RC/CC network, along
IN
can be placed in series
C
pin.
C
. The formula
RMS
I
P-P
=
12
, is suggested to
FB
Many engineers have heard that solid tantalum capacitors are prone to failure if they undergo high surge currents. This is historically true and type TPS capacitors are specially tested for surge capability but surge ruggedness is not a critical issue with the output capacitor. Solid tantalum capacitors fail during very high turn-on surges which do not occur at the output of regulators. High discharge surges, such as when the regulator output is dead shorted, do not harm the capacitors.
Figure 3 shows a typical output ripple voltage waveform for the LT3435. Ripple voltage is determined by the impedance of the output capacitor and ripple current through the inductor. Peak-to-peak ripple current through the inductor into the output capacitor is:
3435fa
11
LT3435
II
VVV
LfV
I
I
OUT MAX PK
OUT IN OUT
IN
PK
P
()
=
()( )
()()( )
=
2
-P
2
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APPLICATIO S I FOR ATIO
V
OUT
20mV/DIV AC-COUPLED C
= 100µF
OUT
TANTALUM
ESR 100m
V
OUT
20mV/DIV AC-COUPLED
= 100µF
C
OUT
CERAMIC
V
SW
5V/DIV
= 12V 500ns/DIV
V
IN
V
= 3.3V
OUT
= 1A
I
LOAD
L = 15µH
Figure 3. LT3435 Ripple Voltage Waveform
3435 F03
For high frequency switchers the ripple current slew rate is also relevant and can be calculated from:
didtV
IN
=
L
Peak-to-peak output ripple voltage is the sum of a triwave created by peak-to-peak ripple current times ESR and a square wave created by parasitic inductance (ESL) and ripple current slew rate. Capacitive reactance is assumed to be small compared to ESR or ESL.
V I ESR ESL
RIPPLE
Example: with V
=
P-P
()( )
= 12V, V
IN
+
di
()
dt
= 3.3V, L = 15µH, ESR =
OUT
0.08, ESL = 10nH:
33 12 33
.–.
I
P-P
()( )
=
ee
12 15 6 500 3
()
()()
=
0 319
.
A
does not fall off at high duty cycles. Most current mode converters suffer a drop off of peak switch current for duty cycles above 50%. This is due to the effects of slope compensation required to prevent subharmonic oscilla­tions in current mode converters. (For detailed analysis, see Application Note 19.)
The LT3435 is able to maintain peak switch current limit over the full duty cycle range by using patented circuitry to cancel the effects of slope compensation on peak switch current without affecting the frequency compensation it provides.
Maximum load current would be equal to maximum switch current for an infinitely large inductor, but with finite inductor size, maximum load current is reduced by one-half peak-to-peak inductor current. The following formula assumes continuous mode operation, implying that the term on the right (I
/2) is less than I
P-P
OUT
.
Discontinuous operation occurs when:
I
OUT DIS
()
For V
OUT
I
OUT MAX()
VVV
OUT IN OUT
2
= 5V, V
IN
=
3
–. .
==
3 0 125 2 875
()
LfV
()()( )
IN
= 8V and L = 15µH:
58 5
()( )
ee
2 15 6 500 3 8
()()()
A
di
dt e
V
RIPPLE
12
==
15 6
= (0.319A)(0.08) + (10e – 9)(0.8e6)
= 0.026 + 0.008 = 34mV
MAXIMUM OUTPUT LOAD CURRENT
Maximum load current for a buck converter is limited by the maximum switch current rating (I rating for the LT3435 is 3A. Unlike most current mode converters, the LT3435 maximum switch current limit
12
.
e
08 6
Note that there is less load current available at the higher input voltage because inductor ripple current increases. At
= 15V, duty cycle is 33% and for the same set of
V
IN
conditions:
P-P
515 5
I
OUT MAX()
). The current
PK
=
3
–. .
==
3 0 22 2 88
()( )
ee
2 15 6 500 3 15
()()()
A
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LT3435
To calculate actual peak switch current in continuous mode with a given set of conditions, use:
VVV
II
SW PK OUT
=+
()
OUT IN OUT
2
()
LfV
()()( )
IN
If a small inductor is chosen which results in discontinous mode operation over the entire load range, the maximum load current is equal to:
2
2
IfLV
PK IN
I
()
OUT MAX
=
2
()( )( )
VVV
OUT IN OUT
()( )
CHOOSING THE INDUCTOR
For most applications the output inductor will fall in the range of 5µH to 33µH. Lower values are chosen to reduce physical size of the inductor. Higher values allow more output current because they reduce peak current seen by the LT3435 switch, which has a 3A limit. Higher values also reduce output ripple voltage and reduce core loss.
When choosing an inductor you might have to consider maximum load current, core and copper losses, allow­able component height, output voltage ripple, EMI, fault current in the inductor, saturation and of course cost. The following procedure is suggested as a way of han­dling these somewhat complicated and conflicting requirements.
1. Choose a value in microhenries such that
the maximum load current plus half of the inductor ripple current is less than the minimum peak switch current (IPK). Choosing a small inductor with lighter loads may result in discontinuous mode of operation, but the LT3435 is designed to work well in either mode.
Assume that the average inductor current is equal to load current and decide whether or not the inductor must withstand continuous fault conditions. If maxi­mum load current is 1A, for instance, a 1A inductor may not survive a continuous 4A overload condition.
Table 3. Inductor Selection Criteria
VENDOR/ VALUE I
µ
PART NO. (
Sumida
CDRH104R-4R7 4.7 6 0.013 4
CDRH104R-100 10 4.4 0.035 4
CDRH104R-150 15 3.6 0.050 4
CDRH104R-220 22 2.9 0.073 4
CDRH104R-330 33 2.3 0.093 4
CDRH124-4R7 4.7 5.7 0.015 4.5
CDRH124-100 10 4.5 0.026 4.5
CDRH124-220 22 2.9 0.066 4.5
CDRH124R-330 33 2.7 0.097 4.5
CDRH127-330 33 3.0 0.065 8
CEI122-220 22 2.3 0.085 34
Coiltronics
UP3B-4R7 4.7 6.5 0.0083 6.8
UP3B-4R7 10 4.3 0.026 6.8
UP3B-330 33 3 0.069 6.8
H) (Amps) (Ohms) (mm)
DC(MAX)
DCR HEIGHT
For applications with a duty cycle above 50%, the inductor value should be chosen to obtain an inductor ripple current of less than 40% of the peak switch current.
2. Calculate peak inductor current at full load current to ensure that the inductor will not saturate. Peak current can be significantly higher than output current, especially with smaller inductors and lighter loads, so don’t omit this step. Powdered iron cores are forgiving because they saturate softly, whereas ferrite cores saturate abruptly. Other core materials fall somewhere in between. The following formula assumes continuous mode of opera­tion, but it errs only slightly on the high side for discon­tinuous mode, so it can be used for all conditions.
II
=+
PEAK OUT
VVV
OUT IN OUT
2
()
fLV
()( )( )
IN
VIN = maximum input voltage
f = switching frequency, 500kHz
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3. Decide if the design can tolerate an “open” core geom­etry like a rod or barrel, which have high magnetic field radiation, or whether it needs a closed core like a toroid to prevent EMI problems. This is a tough decision because the rods or barrels are temptingly cheap and small and there are no helpful guidelines to calculate when the magnetic field radiation will be a problem.
4. After making an initial choice, consider the secondary things like output voltage ripple, second sourcing, etc. Use the experts in the Linear Technology’s applications department if you feel uncertain about the final choice. They have experience with a wide range of inductor types and can tell you about the latest developments in low profile, surface mounting, etc.
Short-Circuit Considerations
The LT3435 is a current mode controller. It uses the V
C
node voltage as an input to a current comparator which turns off the output switch on a cycle-by-cycle basis as this peak current is reached. The internal clamp on the V
C
node, nominally 2.2V, then acts as an output switch peak current limit. This action becomes the switch current limit specification. The maximum available output power is then determined by the switch current limit.
A potential controllability problem could occur under short-circuit conditions. If the power supply output is short circuited, the feedback amplifier responds to the low output voltage by raising the control voltage, V
, to its
C
peak current limit value. Ideally, the output switch would be turned on, and then turned off as its current exceeded the value indicated by VC. However, there is finite response time involved in both the current comparator and turn-off of the output switch. These result in a minimum on time t
ON(MIN).
(V
F
When combined with the large ratio of VIN to
+ I • R), the diode forward voltage plus inductor I • R voltage drop, the potential exists for a loss of control. Expressed mathematically the requirement to maintain control is:
VIR
•≤+
ft
ON
F
V
IN
where:
f = switching frequency
= switch on time
t
ON
VF = diode forward voltage VIN = Input voltage I • R = inductor I • R voltage drop
If this condition is not observed, the current will not be limited at I
but will cycle-by-cycle ratchet up to some
PK
higher value. Using the nominal LT3435 clock frequency of 500kHz, a V maximum t
of 12V and a (VF + I • R) of say 0.7V, the
IN
to maintain control would be approximately
ON
116ns, an unacceptably short time.
The solution to this dilemma is to slow down the oscillator to allow the current in the inductor to drop to a sufficiently low value such that the current doesn’t continue to ratchet higher. When the FB pin voltage is abnormally low thereby indicating some sort of short-circuit condition, the oscil­lator frequency will be reduced. Oscillator frequency is reduced by a factor of 4 when the FB pin voltage is below
0.4V and increases linearly to its typical value of 500kHz at a FB voltage of 0.95V (see Typical Performance Character­istics). In addition, if the current in the switch exceeds 1.5
• IPK current demanded by the VC pin, the LT3435 will skip the next on cycle effectively reducing the oscillator fre­quency by a factor of 2. These oscillator frequency reduc­tions during short-circuit conditions allow the LT3435 to maintain current control.
SOFT-START
For applications where [V
IN
/(V
+ VF)] ratios > 10 or
OUT
large input surge currents can’t be tolerated, the LT3435 soft-start feature should be used to control the output capacitor charge rate during start-up, or during recovery from an output short circuit thereby adding additional control over peak inductor current. The soft-start function limits the switch current via the V
pin to maintain a
C
constant voltage ramp rate (dV/dt) at the output capacitor. A capacitor (C1 in Figure 2) from the C
pin to the
SS
regulated output voltage determines the output voltage
14
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LT3435
ramp rate. When the current through the CSS capacitor exceeds the C
threshold (I
SS
output capacitor is limited by reducing the V The C
threshold is proportional to the FB voltage (see
SS
), the voltage ramp of the
CSS
pin voltage.
C
Typical Performance Characteristics) and is defeated for FB voltages greater than 0.9V (typical). The output dV/dt can be approximated by:
dVdtI
CSS
=
C
SS
but actual values will vary due to start-up load conditions, compensation values and output capacitor selection.
C
= 1000pF
CSS
C
= 0.01µF
CSS
V
OUT
1V/DIV
V
= 12V 1ms/DIV
IN
V
= 3.3V
OUT
I
= 500mA
L
Figure 4. V
OUT
C
CSS
dV/dt
= 0.1µF
3435 F04
Burst Mode OPERATION
To enhance efficiency at light loads, the LT3435 automati­cally switches to Burst Mode operation which keeps the output capacitor charged to the proper voltage while minimizing the input quiescent current. During Burst Mode operation, the LT3435 delivers short bursts of current to the output capacitor followed by sleep periods where the output power is delivered to the load by the output capacitor. In addition, V
and BIAS quiescent
IN
currents are reduced to typically 45µA and 125µA respec- tively during the sleep time. As the load current decreases towards a no load condition, the percentage of time that the LT3435 operates in sleep mode increases and the average input current is greatly reduced resulting in higher efficiency.
The minimum average input current depends on the VIN to
ratio, VC frequency compensation, feedback divider
V
OUT
network and Schottky diode leakage. It can be approxi­mated by the following equation:
III
IN AVG VINS SHDN
++
()
⎛ ⎜
V
BIASS FB S
()
OUT
V
IN
η
()
++
III
where
= input pin current in sleep mode
I
VINS
V
= output voltage
OUT
V
input voltage
IN =
I
= BIAS pin current in sleep mode
BIASS
IFB = feedback network current IS = catch diode reverse leakage at V
OUT
η = low current efficiency (non Burst Mode operation)
Example: For V
45 5
IAA
IN AVG()
=µ+µ+
=µ+µ+µ=µ
45 5 44 99
150
125
100
SUPPLY CURRENT (µA)
During the sleep portion of the Burst Mode Cycle, the V
= 3.3V, VIN = 12V
OUT
3312125 12 5 0 5
.( . . )
⎜ ⎝
µ+ µ+ µ
AAA
⎟ ⎠
AA A A
V
OUT
T
A
75
50
25
0
0
10
Figure 5. I
30 40
20
INPUT VOLTAGE (V)
vs V
Q
IN
(.)
= 3.3V
= 25°C
50
3435 F05
08
60
C
pin voltage is held just below the level need for normal operation to improve transient response. See the Typical Performance Characteristics section for burst and tran­sient response waveforms.
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If a no load condition can be anticipated, the supply current can be further reduced by cycling the SHDN pin at a rate higher than the natural no load burst frequency. Figure 6 shows Burst Mode operation with the SHDN pin. V
OUT
burst ripple is maintained while the average supply current drops to 15µA. The PG pin will be active low during the “on” portion of the SHDN waveform due to the C
capaci-
T
tor discharge when SHDN is taken low. See the Power Good section for further information.
V
OUT
50mV/DIV
AC-COUPLED
V
SHDN
2V/DIV
I
SW
1A/DIV
VIN = 12V 100ms/DIV V
= 3.3V
OUT
= 15µA
I
Q
Figure 6. Burst Mode with Shutdown Pin
3435 F06
CATCH DIODE
The catch diode carries load current during the SW off time. The average diode current is therefore dependent on the switch duty cycle. At high input to output voltage ratios the diode conducts most of the time. As the ratio ap­proaches unity the diode conducts only a small fraction of the time. The most stressful condition for the diode is when the output is short circuited. Under this condition the diode must safely handle I
at maximum duty cycle.
PEAK
To maximize high and low load current efficiency a fast switching diode with low forward drop and low reverse leakage should be used. Low reverse leakage is critical to maximize low current efficiency since its value over tem­perature can potentially exceed the magnitude of the LT3435 supply current. Low forward drop is critical for high current efficiency since the loss is proportional to forward drop.
These requirements result in the use of a Schottky type diode. DC switching losses are minimized due to its low forward voltage drop and AC behavior is benign due to its
Table 4. Catch Diode Selection Criteria
IQ at 125°C EFFICIENCY
LEAKAGE V
V
= 3.3V VF AT 1A V
OUT
DIODE 25°C 125°C25°C 125°CIL = 0A IL = 1A
IR 10BQ100 0.0µA59µA 0.72V 0.58V 125µA 74.7%
Diodes Inc. 0.1µA 242µA 0.48V 0.41V 215µA 81.7% B260SMA
Diodes Inc. 0.2µA 440µA 0.45V 0.36V 270µA 82.4% B360SMB
IR 1µA 1.81mA 0.42V 0.34V 821µA 82.7% MBRS360TR
IR 30BQ100 1.7µA 2.64mA 0.40V 0.32V 1088µA 81.1%
=12V VIN =12V
IN
= 3.3 V
OUT
OUT
= 3.3V
lack of a significant reverse recovery time. Schottky diodes are generally available with reverse voltage ratings of 60V and even 100V and are price competitive with other types.
The effect of reverse leakage and forward drop on effi­ciency for various Schottky diodes is shown in Table 4. As can be seen these are conflicting parameters and the user must weigh the importance of each specification in choos­ing the best diode for the application.
The use of so-called “ultrafast” recovery diodes is gener­ally not recommended. When operating in continuous mode, the reverse recovery time exhibited by “ultrafast” diodes will result in a slingshot type effect. The power internal switch will ramp up V
current into the diode in an
IN
attempt to get it to recover. Then, when the diode has finally turned off, some tens of nanoseconds later, the V
SW
node voltage ramps up at an extremely high dV/dt, per­haps 5V to even 10V/ns! With real world lead inductances the V
node can easily overshoot the VIN rail. This can
SW
result in poor RFI behavior and, if the overshoot is severe enough, damage the IC itself.
BOOST PIN
For most applications the boost components are a 0.33µF capacitor and a MMSD914 diode. The anode is typically connected to the regulated output voltage to generate a voltage approximately V
above VIN to drive the output
OUT
stage (Figure 7a). However, the output stage discharges the boost capacitor during the on time of the switch. The output driver requires at least 2.5V of headroom through­out this period to keep the switch fully saturated. If the
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LT3435
output voltage is less than 3.3V it is recommended that an alternate boost supply is used. The boost diode can be connected to the input (Figure 7b) but care must be taken to prevent the boost voltage (V
= VIN • 2) from
BOOST
exceeding the BOOST pin absolute maximum rating. The additional voltage across the switch driver also increases power loss and reduces efficiency. If available, an inde­pendent supply can be used to generate the required BOOST voltage (Figure 7c). Tying BOOST to V
or an
IN
independent supply may reduce efficiency but it will re­duce the minimum V
required to start-up with light
IN
loads. If the generated BOOST voltage dissipates too much power at maximum load, the BOOST voltage the LT3435 sees can be reduced by placing a Zener diode in series with the BOOST diode (Figure 7a option).
OPTIONAL
BOOST
V
IN
V
IN
V
V
BOOST
V
BOOST(MAX)
V
IN
LT3435
– VSW = V
= VIN + V
BOOST
IN
LT3435
SWGND
OUT
OUT
(7a)
SWGND
V
OUT
V
OUT
A 0.33µF boost capacitor is recommended for most appli- cations. Almost any type of film or ceramic capacitor is suitable but the ESR should be <1 to ensure it can be fully recharged during the off time of the switch. The capacitor value is derived from worst-case conditions of 1700ns on time, TBD boost current and 0.7V discharge ripple. The boost capacitor value could be reduced under less de­manding conditions but this will not improve circuit opera­tion or efficiency. Under low input voltage and low load conditions a higher value capacitor will reduce discharge ripple and improve start-up operation.
SHUTDOWN FUNCTION AND UNDERVOLTAGE LOCKOUT
The SHDN pin on the LT3435 controls the operation of the IC. When the voltage on the SHDN pin is below the 1.2V shutdown threshold the LT3435 is placed in a “zero” supply current state. Driving the SHDN pin above the shutdown threshold enables normal operation. The SHDN pin has an internal sink current of 3µA.
In addition to the shutdown feature, the LT3435 has an undervoltage lockout function. When the input voltage is below 2.4V, switching will be disabled. The undervoltage lockout threshold doesn’t have any hysteresis and is mainly used to insure that all internal voltages are at the correct level before switching is enabled. If an undervolt­age lockout function with hysteresis is needed to limit input current at low V
IN
to V
ratios refer to Figure 8 and
OUT
the following:
V
– VSW = V
BOOST
V
BOOST(MAX)
V
IN
Figure 7. BOOST Pin Configurations
V
V
BOOST
V
BOOST(MAX)
IN
LT3435
– VSW = V
= 2V
BOOST
SWGND
= VDC + V
IN IN
(7b)
DC
(7c)
D
SS
IN
3435 F07
V
VR
V
DC
V
V
OUT
=++
UVLO
=
HYST
SHDN SHDN
1
R
VR
OUT
()
R
3
V
32
R
1
IV
SHDN SHDN
+
⎟ ⎠
R1 should be chosen to minimize quiescent current during normal operation by the following equation:
VV
2
R
1
=
IN
.
I
15
SHDN MAX
()( )
()
3435fa
17
LT3435
WUUU
APPLICATIO S I FOR ATIO
Example:
12 2
=
1
R
3
R
µ
155
.
()
513
.
()
=
13
M
=
.
A
M
65
= ΩΩ
(Nearest 1% 6.49M )
M
.
1
R2 =
7 – 1.3
1.3M 408
=
k
1.3 13
649
.
.
M
1
A
––
µ
(Nearest 1% 412k)
See the Typical Performance Characteristics section for graphs of SHDN and V
LT3435
V
IN
4
R1
R3
V
OUT
SHDN
15
R2
3µA
Figure 8. Undervoltage Lockout
currents verses input voltage.
IN
+
V
IN
COMP
2.4V
+
SHDN COMP
1.3V
ENABLE
3435 F08
SYNCHRONIZING
Oscillator synchronization to an external input is achieved by connecting a TTL logic-compatible square wave with a duty cycle between
5%
and
75%
to the LT3435 SYNC pin. The synchronizing range is equal to initial operating frequency up to
700kHz
. This means that minimum practical sync frequency is equal to the worst-case high self-oscillating frequency ( ating frequency of
300kHz
synchronizing above
575kHz
), not the typical oper-
. Caution should be used when
575kHz
because at higher sync frequencies the amplitude of the internal slope compen­sation used to prevent subharmonic switching is re­duced. This type of subharmonic switching only occurs at input voltages less than twice output voltage. Higher
inductor values will tend to eliminate this problem. See Frequency Compensation section for a discussion of an entirely different cause of subharmonic switching before assuming that the cause is insufficient slope compensa­tion. Application Note 19 has more details on the theory of slope compensation.
If the FB pin voltage is below 0.9V (power-up or output short-circuit conditions) the sync function is disabled. This allows the frequency foldback to operate to avoid and hazardous conditions for the SW pin.
If the synchronization signal is present during Burst Mode operation, synchronization will occur during the burst portion of the output waveform. Synchronizing the LT3435 during Burst Mode operation may alter the natural burst frequency which can lead to jitter and increased ripple in the burst waveform.
If no synchronization is required this pin should be con­nected to ground.
POWER GOOD
The LT3435 contains a power good block which consists of a comparator, delay timer and active low flag that allows the user to generate a delayed signal after the power good threshold is exceeded.
Referring to Figure 2, the PGFB pin is the positive input to a comparator whose negative input is set at V PGFB is taken above V the C
pin starting the delay period. When the voltage on
T
the PGFB pin drops below V
, current (I
PGFB
) is sourced into
CSS
the CT pin is rapidly
PGFB
PGFB
. When
discharged resetting the delay period. The PGFB voltage is typically generated by a resistive divider from the regu­lated output or input supply.
The capacitor on the C
pin determines the amount of
T
delay time between the PGFB pin exceeding its threshold (V When the PGFB pin rises above V (I
) and the PG pin set to a high impedance state.
PGFB
current is sourced
PGFB
) from the CT pin into the external capacitor. When the
CT
voltage on the external capacitor reaches an internal clamp (V
), the PG pin becomes a high impedance node. The
CT
resultant PG delay time is given by t = C the voltage on the PGFB pin drops below its V
•(VCT)/(ICT). If
CT
, CCT will
PGFB
be discharged rapidly and PG will be active low with a 200µA sink capability. If the SHDN pin is taken below its
3435fa
18
WUUU
APPLICATIO S I FOR ATIO
LT3435
threshold during normal operation, the CT pin will be discharged and PG inactive, resulting in a non Power Good cycle when SHDN is taken above its threshold. Figure 9 shows the power good operation with PGFB connected to FB and the capacitance on C
= 0.1µF. The PGOOD pin has
T
a limited amount of drive capability and is susceptible to noise during start-up and Burst Mode operation. If erratic
V
OUT
500mV/DIV
PG
100k TO V
IN
V
CT
500mV/DIV
V
SHDN
2V/DIV
TIME (10ms/DIV)
Figure 9. Power Good
PG at 80% V
LT3435
V
PG
PGFB
OUT
IN
FB
C
T
with 100ms Delay
200k
153k
12k
100k
0.27µF
3435 F09
V
= 3.3V
OUT
C
OUT
operation occurs during these conditions a small filter capacitor from the PGOOD pin to ground will ensure proper operation. Figure 10 shows several different con­figurations for the LT3435 Power Good circuitry. Figure 10 shows several different configurations for the LT3435 Power Good circuitry.
LAYOUT CONSIDERATIONS
As with all high frequency switchers, when considering layout, care must be taken in order to achieve optimal electrical, thermal and noise performance. For maximum efficiency switch rise and fall times are typically in the nanosecond range. To prevent noise both radiated and conducted the high speed switching current path, shown in Figure 11, must be kept as short as possible. This is implemented in the suggested layout of Figure 12. Short­ening this path will also reduce the parasitic trace induc­tance of approximately 25nH/inch. At switch off, this
PG at VIN > 4V with 100ms Delay
V
LT3435
PGFB
PG
IN
FB
C
T
511k
200k
0.27µF
200k
165k
100k
V
= 3.3V
OUT
C
OUT
V
Disconnect at 80% V
OUT
with 100ms Delay
V
IN
PG
LT3435
PGFB
FB
C
T
200k
0.27µF
153k
12k
100k
OUT
V
= 3.3V
OUT
C
OUT
V
OUT
Figure 10. Power Good Circuits
Disconnect 3.3V Logic Signal
with 100µs Delay
V
IN
PG
LT3435
PGFB
FB
C
200k
C
OUT
866k
T
100k
270pF
3435 F10
V
= 12V
OUT
3435fa
19
LT3435
P
RI V
V
tIVf
SW
SW OUT OUT
IN
EFF OUT IN
=
()( )
+
()( )()()
2
12/
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APPLICATIO S I FOR ATIO
parasitic inductance produces a flyback spike across the LT3435 switch. When operating at higher currents and input voltages, with poor layout, this spike can generate voltages across the LT3435 that may exceed its absolute maximum rating. A ground plane should always be used under the switcher circuitry to prevent interplane coupling and overall noise.
The V
and FB components should be kept as far away as
C
possible from the switch and boost nodes. The LT3435 pinout has been designed to aid in this. The ground for these components should be separated from the switch current path. Failure to do so will result in poor stability or subharmonic like oscillation.
Board layout also has a significant effect on thermal resistance. Pin 8 and the exposed die pad, Pin 17, are a
LT3435
V
42
IN
V
IN
+
C2
SW
HIGH
FREQUENCY
CIRCULATION
PATH
L1
D1
V
OUT
LOAD
C1
continuous copper plate that runs under the LT3435 die. This is the best thermal path for heat out of the package. Reducing the thermal resistance from Pin 8 and exposed pad onto the board will reduce die temperature and in­crease the power capability of the LT3435. This is achieved by providing as much copper area as possible around the exposed pad. Adding multiple solder filled feedthroughs under and around this pad to an internal ground plane will also help. Similar treatment to the catch diode and coil terminations will reduce any additional heating effects.
THERMAL CALCULATIONS
Power dissipation in the LT3435 chip comes from four sources: switch DC loss, switch AC loss, boost circuit current, and input quiescent current. The following formu­las show how to calculate each of these losses. These formulas assume continuous mode operation, so they should not be used for calculating efficiency at light load currents.
Switch loss:
GND
Figure 11. High Speed Switching Path
V
OUT
C1
C3
GND
C2 D2
MINIMIZE
D1-C3
LOOP
V
IN
CONNECT PIN 8 GND TO THE
PIN 17 EXPOSED PAD GND
L1
PLACE VIA's UNDER EXPOSED
PAD TO A BOTTOM PLANE TO
D1
C4
ENHANCE THERMAL
1
NC
SW
2
V
3
IN
4
V
IN
SW
5
6
BOOST
C
7
T
GND
8
CONDUCTIVITY
PGOOD
SHDN
LT3435
SYNC
PGFB
FB
V
BIAS
C
SS
Figure 12. Suggested Layout
3435 F11
Boost current loss:
2
VI
()
P
KELVIN SENSE
FEEDBACK
TRACE AND
KEEP SEPARATE
16
15
14
13
12
11
C
10
9
FROM BIAS TRACE
R3
R1
R2
C2
C5
BOOST
Quiescent current loss:
P
= VIN (0.0026) + V
Q
= switch resistance (0.15 when hot )
R
SW
t
= effective switch current/voltage overlap time
EFF
(tr + tf + tIR + tIF) tr = (VIN/1.2)ns
OUT OUT
=
V
46/
()
IN
(0.001)
OUT
tf = (VIN/1.7)ns tIR = tIF = (I
OUT
/0.2)ns
f = switch frequency
3435 F12
20
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WUUU
APPLICATIO S I FOR ATIO
LT3435
Example: with VIN = 25V, V
= 5V and I
OUT
OUT
= 2A:
increase in internal dissipation is of insufficient time dura­tion to raise die temperature significantly.
.
015 2 5
Pee
PW
PW
( )()()
=
SW
+=
.. .
012 0962 108
BOOST
Q
=
=
40 0 0026 5 0 001 0 11
()
Total power dissipation is:
P
= 1.08 + 0.03+ 0.11 = 1.22W
TOT
Thermal resistance for the LT3435 package is influenced
2
9
25
2
/
5240
()
()
+
77 12 2 25 500 3
()
=
.
003
/
()( )( )
()
40
...
+
()
=
A second consideration is controllability. A potential limi­tation occurs with a high step-down ratio of V as this requires a correspondingly narrow minimum switch on time. An approximate expression for this (assuming continuous mode operation) is given as follows:
t
ON(MIN)
where:
V
= input voltage
IN
V
= output voltage
OUT
VF = Schottky diode forward drop
by the presence of internal or backside planes. With a full
f
= switching frequency
plane under the FE16 package, thermal resistance will be about 45°C/W. No plane will increase resistance to about 150°C/W. To calculate die temperature, use the proper thermal resistance number for the desired package and add in worst-case ambient temperature:
= TA + QJA (P
T
J
With the FE16 package (Q
TOT
)
= 45°C/W) at an ambient
JA
temperature of 70°C:
= 70 + 45(1.22) = 125°C
T
J
Input Voltage vs Operating Frequency Considerations
OSC
A potential controllability problem arises if the LT3435 is called upon to produce an on time shorter than it is able to produce. Feedback loop action will lower then reduce the V
control voltage to the point where some sort of cycle-
C
skipping or Burst Mode behavior is exhibited.
In summary:
1. Be aware that the simultaneous requirements of high V
, high I
IN
practice due to internal dissipation. The Thermal Con­siderations section offers a basis to estimate internal power. In questionable cases a prototype supply should
The absolute maximum input supply voltage for the LT3435
be built and exercised to verify acceptable operation.
is specified at 60V. This is based solely on internal semi­conductor junction breakdown effects. Due to internal power dissipation the actual maximum V
achievable in a
IN
particular application may be less than this.
2. The simultaneous requirements of high V high f
OSC
switch on time. Cycle skipping and/or Burst Mode be­havior will result causing an increase in output voltage
A detailed theoretical basis for estimating internal power
ripple while maintaining the correct output voltage.
loss is given in the section Thermal Considerations. Note that AC switching loss is proportional to both operating frequency and output current. The majority of AC switch­ing loss is also proportional to the square of input voltage.
For example, while the combination of V 5V at 2A and f multaneously raising V
= 500kHz may be easily achievable, si-
OSC
to 60V and f
IN
= 40V, V
IN
to 700kHz is not
OSC
OUT
possible. Nevertheless, input voltage transients up to 60V can usually be accommodated, assuming the resulting
FREQUENCY COMPENSATION
Before starting on the theoretical analysis of frequency response the following should be remembered—the worse
=
the board layout, the more difficult the circuit will be to stabilize. This is true of almost all high frequency analog circuits. Read the Layout Considerations section first. Common layout errors that appear as stability problems are distant placement of input decoupling capacitor and/or
to V
IN
OUT
= V
+ VF/VIN(f
OUT
and high f
OUT
)
OSC
may not be achievable in
OSC
, low V
IN
OUT
and
can result in an unacceptably short minimum
,
3435fa
21
LT3435
WUUU
APPLICATIO S I FOR ATIO
catch diode and connecting the VC compensation to a ground track carrying significant switch current. In addi­tion the theoretical analysis considers only first order non­ideal component behavior. For these reasons, it is important that a final stability check is made with production layout and components.
The LT3435 uses current mode control. This alleviates many of the phase shift problems associated with the inductor. The basic regulator loop is shown in Figure 12. The LT3435 can be considered as two gm blocks, the error amplifier and the power stage.
Figure 13 shows the overall loop response with a 330pF V
C
capacitor and a typical 100µF tantalum output capacitor. The response is set by the following terms:
Error amplifier: DC gain is set by g
and RO:
m
EA Gain = 650µ • 1.5M = 975
The pole set by CF and RL:
EA Pole = 1/(2π • 1.5M • 470pF) = 220Hz
Unity gain frequency is set by C
and gm:
F
EA Unity Gain Frequency = 650µF/(2π • 470pF)
= 220kHz
Powerstage: DC gain is set by gm and RL (assume 10Ω):
PS DC Gain = 6 • 10 = 60
LT3435
CURRENT MODE
POWER STAGE
= 6
g
m
V
C
11
C
C
F
C
C
gm = 650µ
1.5MR
ERROR
AMP
SW
2
R1
FB
12
R2
OUTPUT
C
FB
ESR
+
1.25V
3435 F13
C
OUT
Figure 13. Model for Loop Response
capacitor. As the value of R
is increased, transient re-
C
sponse will generally improve but two effects limit its value. First, the combination of output capacitor ESR and a large RC may stop loop gain rolling off altogether. Second, if the loop gain is not rolled off sufficiently at the switching frequency output ripple will perturb the V
C
pin enough to cause unstable duty cycle switching similar to subharmonic oscillation. This may not be apparent at the output. Small-signal analysis will not show this since a continuous time system is assumed.
When checking loop stability the circuit should be oper­ated over the application’s full voltage, current and tem­perature range. Any transient loads should be applied and the output voltage monitored for a well-damped behavior.
Pole set by C
OUT
and RL:
PS Pole = 1/(2π • 100µF • 10) = 159Hz
Unity gain set by C
OUT
and gm:
PS Unity Gain Freq = 6/(2π • 100µF) = 94kHz.
Tantalum output capacitor zero is set by C
OUT
and C
OUT
ESR
Output Capacitor Zero = 1/(2π • 100µF • 0.1) = 15.9kHz
The zero produced by the ESR of the tantalum output capacitor is very useful in maintaining stability. If better transient response is required, a zero can be added to the loop using a resistor (R
) in series with the compensation
C
22
100
80
40
GAIN (dB)
0
–40
–80
100 1k 10k 100k
V
OUT
C
OUT
= 470pF
C
F
= 10k
R
C
= 4700pF
C
C
I
LOAD
FREQUENCY (Hz)
= 3.3V = 100µF, 0.1
= 1A
Figure 14. Overall Loop Response
3435 F14
1M10
180
160
PHASE (DEG)
120
80
40
0
3435fa
PACKAGE DESCRIPTIO
(.141)
3.58
U
FE Package
16-Lead Plastic TSSOP (4.4mm)
(Reference LTC DWG # 05-08-1663)
Exposed Pad Variation BC
4.90 – 5.10* (.193 – .201)
3.58
(.141)
16 1514 13 12 11
LT3435
10 9
6.60 ±0.10
4.50 ±0.10
RECOMMENDED SOLDER PAD LAYOUT
0.09 – 0.20
(.0035 – .0079)
NOTE:
1. CONTROLLING DIMENSION: MILLIMETERS
2. DIMENSIONS ARE IN
3. DRAWING NOT TO SCALE
SEE NOTE 4
0.65 BSC
4.30 – 4.50* (.169 – .177)
0.50 – 0.75
(.020 – .030)
MILLIMETERS
(INCHES)
(.116)
0.45 ±0.05
2.94
1.05 ±0.10
1345678
2
0.25 REF
0° – 8°
0.65
(.0256)
BSC
0.195 – 0.30
(.0077 – .0118)
TYP
4. RECOMMENDED MINIMUM PCB METAL SIZE FOR EXPOSED PAD ATTACHMENT
*DIMENSIONS DO NOT INCLUDE MOLD FLASH. MOLD FLASH SHALL NOT EXCEED 0.150mm (.006") PER SIDE
2.94
(.116)
1.10
(.0433)
MAX
0.05 – 0.15
(.002 – .006)
FE16 (BC) TSSOP 0204
6.40
(.252)
BSC
Information furnished by Linear Technology Corporation is believed to be accurate and reliable. However, no responsibility is assumed for its use. Linear Technology Corporation makes no represen­tation that the interconnection of its circuits as described herein will not infringe on existing patent rights.
3435fa
23
LT3435
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Converter
LT1977 60V, 1.5A (ISW), 500kHz, High Efficiency Step-Down DC/DC VIN: 3.3V to 60V, IQ = 100µA, ISD < 1µA
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LTC3412 2.5A (I
LTC3414 4A (I
LT3430 60V, 3A (ISW), 200kHz, High Efficiency Step-Down DC/DC VIN: 5.5V to 60V, V
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LT3434 60V, 3A (ISW), 200kHz, High Efficiency Step-Down DC/DC VIN: 3.3V to 60V, IQ = 100µA, ISD < 1µA
Converter
LTC3727/LTC3727-1 36V, 500kHz, High Efficiency Step-Down DC/DC Controllers VIN: 4V to 36V, V
), 100kHz, High Efficiency Step-Down DC/DC Converters VIN: 7.3V to 45V/64V, V
OUT
), 100kHz, High Efficiency Step-Down DC/DC Converters VIN: 7.3V to 45V/64V, V
OUT
), 550kHz, Synchronous Step-Down DC/DC Converter VIN: 2.7V to 6V, V
OUT
< 10µA, DD5/7, TO220-5/7
I
SD
< 10µA, DD5/7, TO220-5/7
I
SD
< 2.5µA, S8
SD
< 25µA, TSSOP16/E
SD
< 30µA, N8, S8
SD
TSSOP16
), 1.1MHz, High Efficiency Step-Down DC/DC VIN: 3V to 25V, V
OUT
< 25µA, TSSOP16/E
SD
MS8E
), 1.5MHz, High Efficiency Step-Down DC/DC VIN: 2.5V to 5.5V, V
OUT
), 4MHz, Synchronous Step-Down DC/DC Converter VIN: 2.5V to 5.5V, V
OUT
TSSOP16E
), 4MHz, Synchronous Step-Down DC/DC Converter VIN: 2.25V to 5.5V, V
OUT
TSSOP20E
< 30µA, TSSOP16E
SD
< 30µA, TSSOP16E
SD
), 200kHz, Buck-Boost DC/DC Converter VIN: 5V to 60V, V
OUT
QFN-32, SSOP-28
= 2.21V, IQ = 8.5mA,
OUT(MIN)
= 2.21V, IQ = 8.5mA,
OUT(MIN)
= 1.24V, IQ = 3.2mA,
OUT(MIN)
= 1.20V, IQ = 1mA, I
OUT(MIN)
= 1.20V, IQ = 2.5mA,
OUT(MIN)
= 1.20V, IQ = 1mA, I
OUT(MIN)
= 1.24V, IQ = 3.2mA,
OUT(MIN)
= 0.8V, IQ = 15µA, ISD < 1µA,
OUT(MIN)
= 1.2V, IQ = 3.8mA, MS10
OUT(MIN)
= 1.20V, IQ = 2.5mA,
OUT(MIN)
= 1.28V, IQ = 30µA, ISD < 1µA,
OUT(MIN)
= 0.6V, IQ = 40µA, MS10
OUT(MIN)
= 0.8V, IQ = 60µA, ISD < 1µA,
OUT(MIN)
= 0.8V, IQ = 64µA, ISD < 1µA,
OUT(MIN)
= 1.20V, IQ = 2.5mA,
OUT(MIN)
= 1.20V, IQ = 2.5mA,
OUT(MIN)
: 3.3V to 20V, IQ = 100µA, TSSOP-16E
OUT
= 0.8V, IQ = 670µA, ISD < 20µA,
OUT(MIN)
SD
SD
< 15µA,
< 6µA,
24
Linear Technology Corporation
1630 McCarthy Blvd., Milpitas, CA 95035-7417
(408) 432-1900 ● FAX: (408) 434-0507
www.linear.com
3435fa
LT 0306 REV A • PRINTED IN USA
© LINEAR TECHNOLOGY CORPORATION 2005
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