LINER LT1976IFE

LT1976
High Voltage 1.5A, 200kHz
Step-Down Switching Regulator
with 100µA Quiescent Current
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FEATURES
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DESCRIPTIO
The LT®1976 is a 200kHz monolithic buck switching
regulator that accepts input voltages up to 60V. A high
efficiency 1.5A, 0.2Ω 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.
Wide Input Range: 3.3V to 60V
1.5A 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
200kHz Switching Frequency
Saturating Switch Design: 0.2Ω 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
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 CSS pin to the output
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.
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APPLICATIO S
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High Voltage Power Conversion
14V and 42V Automotive Systems
Industrial Power Systems
Distributed Power Systems
Battery-Powered Systems
The LT1976 is available in a 16-pin TSSOP package with
exposed pad leadframe for low thermal resistance.
, LTC and LT are registered trademarks of Linear Technology Corporation.
Burst Mode is a registered trademark of Linear Technology Corporation.
*U.S. Patent 6,498,466 **See Burst Mode Operation section for conditions
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TYPICAL APPLICATIO
Supply Current vs
Input Voltage
14V to 3.3V Step-Down Converter with
100µA No Load Quiescent Current
VIN
BOOST
0.33µF 33µH
SHDN
SW
4148
0.1µF
LT1976
10MQ100N
VC
100pF
0.047µF
12.5k
1µF
CSS
VBIAS
CT
SYNC
GND
FB
PGFB
PG
27pF
165k
1%
100k
1%
100µF
6.3V
TANT
Efficiency vs Load Current
100
VOUT = 3.3V
TA = 25°C
90
125
80
100
EFFICIENCY (%)
4.7µF
100V
CER
VOUT
3.3V
1A
SUPPLY CURRENT (µA)
VIN
3.3V TO 60V
150
75
50
TA = 25°C
VOUT = 5V
VOUT = 3.3V
70
60
50
40
30
20
25
10
0
1976 TA01
0
10
30
40
20
INPUT VOLTAGE (V)
50
60
1976 F05
0
0.0001
0.001
0.1
0.01
LOAD CURRENT (A)
1
10
1976 TA02
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LT1976
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ABSOLUTE
AXI U RATI GS
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PACKAGE/ORDER I FOR ATIO
(Note 1)
VIN, SHDN, BIAS ..................................................... 60V
BOOST Pin Above SW ............................................ 35V
BOOST Pin Voltage ................................................. 68V
SYNC, CSS, PGFB, FB ................................................ 6V
Operating JunctionTemperature Range
LT1976EFE (Note 2) ........................ – 40°C to 125°C
LT1976IFE (Note 2) ......................... – 40°C to 125°C
Storage Temperature Range ................. – 65°C to 150°C
Lead Temperature (Soldering, 10 sec).................. 300°C
TOP VIEW
NC
1
16 PGOOD
SW
2
15 SHDN
NC
3
14 SYNC
VIN
4
NC
5
12 FB
BOOST
6
11 VC
TCAP
7
10 BIAS
GND
8
9
17
ORDER PART
NUMBER
LT1976EFE
LT1976IFE
13 PGFB
CSS
FE PACKAGE
16-LEAD PLASTIC TSSOP
TJMAX = 125°C, θJA = 45°C/W, θJC(PAD) = 10°C/W
EXPOSED PAD IS GND (PIN 17)
MUST BE SOLDERED TO GND (PIN 8)
Consult LTC Marketing for parts specified with wider operating temperature ranges.
ELECTRICAL CHARACTERISTICS
The ● denotes the specifications which apply over the full operating
temperature range, otherwise specifications are at TJ = 25°C. VIN = 12V, SHDN = 12V, BOOST = 15.3V, BIAS = 5V, FB/PGFB = 1.25V,
CSS/SYNC = 0V unless otherwise noted.
SYMBOL
PARAMETER
VSHDN
SHDN Threshold
ISHDN
SHDN Input Current
CONDITIONS
SHDN = 12V
Minimum Input Voltage (Note 3)
IVINS
IVIN
MIN
TYP
MAX
UNITS
1.2
1.3
1.4
V
●
5
20
µA
●
2.4
3
V
0.1
2
µA
170
45
230
75
µA
µA
3.2
2.6
4.10
3.25
mA
mA
●
Supply Shutdown Current
SHDN = 0V, BOOST = 0V, FB/PGFB = 0V
Supply Sleep Current (Note 4)
BIAS = 0V, FB = 1.35V
FB = 1.35V
Supply Quiescent Current
BIAS = 0V, FB = 1.15V, VC = 0.8V
BIAS = 5V, FB = 1.15V, VC = 0.8V
●
●
Minimum BIAS Voltage (Note 5)
●
2.7
3
V
IBIASS
BIAS Sleep Current (Note 4)
●
110
180
µA
IBIAS
BIAS Quiescent Current
SYNC = 3.3V
700
800
µA
Minimum Boost Voltage (Note 6)
ISW = 1.5A
1.8
2.5
V
Input Boost Current (Note 7)
ISW = 0.5A
ISW = 1.5A
10
40
15
50
mA
mA
VREF
Reference Voltage (VREF)
3.3V < VVIN < 60V
1.25
1.275
V
IFB
FB Input Bias Current
75
200
nA
EA Voltage Gain (Note 8)
900
●
1.225
EA Voltage gm
dI(VC)= ±10µA
500
650
800
µMho
EA Source Current
FB = 1.15V
25
40
55
µA
EA Sink Current
FB = 1.35V
20
30
40
µA
2.1
2.2
2.4
V
1.5
2.4
3.5
A
VC to SW gm
3
VC High Clamp
IPK
V/V
SW Current Limit
●
A/V
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LT1976
ELECTRICAL CHARACTERISTICS
The ● denotes the specifications which apply over the full operating
temperature range, otherwise specifications are at TJ = 25°C. VIN = 12V, SHDN = 12V, BOOST = 15.3V, BIAS = 5V, FB/PGFB = 1.25V,
CSS/SYNC = 0V unless otherwise noted.
SYMBOL
PARAMETER
CONDITIONS
MIN
Switch On Resistance (Note 9)
●
Switching Frequency
●
Maximum Duty Cycle
180
90
MAX
UNITS
0.2
0.4
Ω
200
230
kHz
92
Minimum SYNC Amplitude
1.5
SYNC Frequency Range
600
SYNC Input Impedance
CSS Current Threshold (Note 10)
IPGFB
PGFB Input Current
VPGFB
PGFB Voltage Threshold (Note 11)
●
88
ICT
CT Source Current (Note 11)
●
3
10
CT Sink Current (Note 11)
CT Voltage Threshold (Note 11)
PGFB = 1V, PG = 400mV
Note 1: Absolute Maximum Ratings are those values beyond which the life of
a device may be impaired.
Note 2: The LT1976EFE 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
LT1976IFE 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 LT1976. With the BIAS pin at 0V, all of the quiescent current
required to operate the LT1976 will be provided by the VIN pin. With the
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.
V
kHz
kΩ
13
16
µA
25
100
nA
90
92
%
3.6
5.5
µA
1
2
1.16
1.2
1.24
V
0.1
1
µA
PG Leakage (Note 11)
PG Sink Current (Note 11)
%
2.0
85
ICSS
VCT
TYP
120
200
mA
µA
Note 5: Minimum BIAS voltage is the voltage on the BIAS pin when IBIAS is
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 VC swing from 1.15V to 750mV.
Note 9: Switch on resistance is calculated by dividing VIN to SW voltage by the
forced current (1.5A). See Typical Performance Characteristics for the graph
of switch voltage at other currents.
Note 10: The CSS threshold is defined as the value of current sourced into the
CSS pin which results in an increase in sink current from the VC pin. See the
Soft-Start section in Applications Information.
Note 11: The PGFB threshold is defined as the percentage of VREF voltage
which causes the current source output of the CT pin to change from
sinking (below threshold) to sourcing current (above threshold). When
sourcing current, the voltage on the CT pin rises until it is clamped
internally. When the clamp is activated, the output of the PG pin will be set
to a high impedance state. When the CT clamp is inactive the PG pin will
be set active low with a current sink capability of 200µA.
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TYPICAL PERFOR A CE CHARACTERISTICS
Oscillator Frequency
1.29
240
1.28
230
1.27
220
1.26
1.25
1.24
1.23
190
160
100
50
25
0
75
TEMPERATURE (°C)
100
1.00
–50 –25
125
Shutdown Supply Current
200
180
20
4.5
3.0
2.5
140
CURRENT (µA)
CURRENT (µA)
CURRENT (µA)
4.0
3.5
VBIAS = 0V
160
VIN = 60V
15
10
2.0
120
100
80
VBIAS = 5V
60
1.5
5
40
VIN = 42V
1.0
0
10
30
40
20
SHDN VOLTAGE (V)
0
–50 –25
60
50
VIN = 12V
50
25
0
75
TEMPERATURE (°C)
100
0
–50 –25
125
1.18
160
1.16
140
1.14
100
80
1.08
40
1.04
20
1.02
100
125
1976 G07
200
1.10
1.06
1.00
–50 –25
125
PG Sink Current
1.12
60
100
250
CURRENT (µA)
180
VOLTAGE (V)
1.20
120
50
25
0
75
TEMPERATURE (°C)
1976 G06
PGFB Threshold
Bias Sleep Current
200
50
25
0
75
TEMPERATURE (°C)
20
1976 G05
1976 G04
0
–50 –25
125
Sleep Mode Supply Current
25
TJ = 25°C
100
1976 G03
5.0
0
50
25
0
75
TEMPERATURE (°C)
1976 G02
SHDN Pin Current
CURRENT (µA)
0.15
1.05
1976 G01
5.5
1.20
1.10
150
–50 –25
125
1.25
180
1.21
50
25
0
75
TEMPERATURE (°C)
1.30
200
170
–25
1.35
210
1.22
1.20
–50
SHDN Threshold
1.40
VOLTAGE (V)
250
FREQUENCY (kHz)
VOLTAGE (V)
FB Voltage
1.30
150
100
50
50
25
0
75
TEMPERATURE (°C)
100
125
1976 G08
0
–50 –25
50
25
0
75
TEMPERATURE (°C)
100
125
1976 G08
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TYPICAL PERFOR A CE CHARACTERISTICS
Soft-Start Current Threshold
vs FB Voltage
Switch Peak Current Limit
3.5
50
250
TJ = 25°C
45
40
3.0
FREQUENCY (kHz)
2.5
SOFT-START
DEFEATED
30
25
20
15
2.0
TJ = 25°C
200
35
CURRENT (µA)
PEAK SWITCH CURRENT (A)
Oscillator Frequency
vs FB Voltage
10
150
100
50
5
1.5
–50 –25
–0
25
50
75
TEMPERATURE (°C)
100
0
125
0
0
0.2
0.6
0.8
0.4
FB VOLTAGE (V)
1976 G10
Switch On Voltage (VCESAT)
0.2
TJ = 125°C
250
TJ = 25°C
200
150
100
VOUT = 3.3V
TA = 25°C
VOUT = 5V
7.0
START-UP
6.5
100
75
50
0.5 0.7 0.9 1.1
LOAD CURRENT (A)
1.3
5.5
VOUT = 3.3V
START-UP
5.0
RUNNING
4.5
4.0
3.5
0
0.3
RUNNING
6.0
25
TJ = –50°C
50
1.2
Minimum Input Voltage
INPUT VOLTAGE (V)
SUPPLY CURRENT (µA)
300
1.0
7.5
125
400
350
0.6
0.8
0.4
FB VOLTAGE (V)
1976 G12
Supply Current vs Input Voltage
150
450
VOLTAGE (mV)
0
1976 G11
500
0
–0.1 0.1
1.2
1.0
1.5
3.0
0
10
30
40
20
INPUT VOLTAGE (V)
50
60
0
0.25
0.50 0.75 1.00
LOAD CURRENT (A)
1976 F05
1976 G13
1.25
1.50
1976 G19
Burst Mode Operation
Burst Mode Operation
VOUT
50mV/DIV
VOUT
50mV/DIV
ISW
100mA/DIV
ISW
100mA/DIV
0A
0A
VIN = 12V
VOUT = 3.3V
IQ = 100µA
TIME (5ms/DIV)
1976 G14
VIN = 12V
TIME (10µs/DIV)
VOUT = 3.3V
IQ = 100µA
1976 G15
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TYPICAL PERFOR A CE CHARACTERISTICS
No Load 1A Step Response
Step Response
VOUT
100mV/DIV
VOUT
100mV/DIV
1A
IOUT
500mA/DIV
0A
1A
IOUT
500mA/DIV
0A
VIN = 12V
TIME (1ms/DIV)
VOUT = 3.3V
COUT = 47µF
1976 G17
TIME (1ms/DIV)
VIN = 12V
VOUT = 3.3V
COUT = 47µF
IDC = 250mA
1976 G18
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NC (Pins 1, 3, 5): No Connection.
SW (Pin 2): 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.
VIN (Pin 4): This is the collector of the on-chip power NPN
switch. VIN powers the internal control circuitry when 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
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 0.2Ω FET
structure, but with much smaller die area.
CT (Pin 7): A capacitor on the CT pin determines the amount
of delay time between the PGFB pin exceeding its threshold (VPGFB) and the PG pin set to a high impedance state.
When the PGFB pin rises above VPGFB, current is sourced
from the CT pin into the external capacitor. When the voltage on the external capacitor reaches an internal clamp
(VCT), the PG pin becomes a high impedance node. The
resultant PG delay time is given by t = CCT • VCT/ICT. If the
voltage on the PGFB pin drops below VPGFB, CCT will be
discharged rapidly to 0V and PG will be active low with a
200µA sink capability. If the CT pin is clamped (Power Good
condition) during normal operation and SHDN is taken low,
the CT pin will be discharged and a delay period will occur
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).
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LT1976
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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 CSS capacitor exceeds the CSS threshold (ICSS), the voltage ramp of
the output is limited. The CSS threshold is proportional to
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.
PGFB (PIN 13): The PGFB pin is the positive input to a
comparator whose negative input is set at VPGFB. When
PGFB is taken above VPGFB, current (ICSS) is sourced into
the CT pin starting the PG delay period. When the voltage
on the PGFB pin drops below VPGFB, the CT pin is rapidly
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.
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.
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
20% and 80% 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.
VC (Pin 11): The VC pin is the output of the error amplifier
and the input of the peak switch current comparator. It is
normally used for frequency compensation, but can also
serve as a current clamp or control loop override. VC sits
at about 0.45V for light loads and 2.2V at maximum load.
During the sleep portion of Burst Mode operation, the VC
pin is held at a voltage slightly below the burst threshold
for better transient response. Driving the VC pin to ground
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 CSS pin. See the Feedback 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 1.2V with a typical
source current of 3µA 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 CT pin is below its clamp level and
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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BLOCK DIAGRA
4
VIN
INTERNAL REF
UNDERVOLTAGE
LOCKOUT
10
14
15
BIAS
THERMAL
SHUTDOWN
2.4V
SLOPE
COMP
Σ
200kHz
OSCILLATOR
+
CURRENT
COMP
–
SYNC
SHDN
BOOST
ANTISLOPE
COMP
+
R
SHDN
COMP
S
–
SWITCH
Q
LATCH
DRIVER
CIRCUITRY
SW
1.3V
9
12
CSS
FB
SOFT-START
BURST MODE
DETECT
FOLDBACK
DETECT
VC
CLAMP
6
2
+
ERROR
AMP
1.25V
11
13
–
VC
PG
PGFB
16
+
PG
COMP
1.12V
1.2V CT
CLAMP
–
GND 17
7
PGND 8
CT
1976 BD
Figure 1. LT1976 Block Diagram
The LT1976 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
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 LT1976 operates from an
internal 2.4V bias line. The bias regulator normally draws
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BLOCK DIAGRA
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.
To further optimize efficiency, the LT1976 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 LT1976 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.
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APPLICATIO S I FOR ATIO
FEEDBACK PIN FUNCTIONS
Table 1
The feedback (FB) pin on the LT1976 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.
OUTPUT
VOLTAGE
(V)
R2
(kΩ, 1%)
R1
NEAREST (1%)
(kΩ)
OUTPUT
ERROR
(%)
2.5
100
100
0
Referring to Figure 2, the output voltage is determined by
a voltage divider from VOUT to ground which generates
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.
R1 = R2 •
VOUT – 1.25
1.25 + R2 • 50nA
3
100
140
0
3.3
100
165
0.38
5
100
300
0
6
100
383
0.63
8
100
536
– 0.63
10
100
698
– 0.25
12
100
866
0.63
VOUT
LT1976
SW 2
SOFT-START
200kHz
OSCILLATOR
CSS
C1
9
FOLDBACK
DETECT
R1
+
FB
12
ERROR
AMP
R2
–
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
1.25V
VC
11
1976 F02
Figure 2. Feedback Network
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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 2A for the LT1976). Minimum switch on time
limitations would prevent the switcher from attaining a
sufficiently low duty cycle if switching frequency were
maintained at 200kHz, 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 VC pin, due to minimum switch on time, the
LT1976 will skip the next switch cycle. As the feedback
voltage rises, the switching frequency increases to 200kHz
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 CSS pin to the output determines the maximum output
dV/dt. When the feedback voltage is below 0.4V, the VC pin
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 ICSS the VC voltage is
reduced resulting in a constant dV/dt at the output. As the
feedback voltage increases ICSS increases, resulting in an
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.
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 LT1976 and force the
switching current into a tight local loop, thereby minimizing EMI. The RMS ripple current can be calculated from:
IRIPPLE(RMS) =
IOUT
VOUT ( VIN – VOUT )
VIN
Ceramic capacitors are ideal for input bypassing. At 200kHz
switching frequency input capacitor values in the range of
4.7µF to 20µF are suitable for most applications. If operation is required close to the minimum input required by the
LT1976 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 LT1976 to a pre-powered source such
as a wall adapter can exceed maximum VIN ratings. The
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 LT1976. All input voltage
transient sequences should be observed at the VIN pin of
the LT1976 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 0.5Ω to 2Ω 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
1976f
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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
Output capacitor ripple current (RMS)
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 LT1976 applications is 0.05Ω to 0.2Ω. A
typical output capacitor is an AVX type TPS, 100µF at 10V,
with a guaranteed ESR less than 0.1Ω. 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
AVX TPS
ESR MAX (Ω)
RIPPLE CURRENT (A)
0.1 to 0.3
0.7 to 1.1
0.1 to 0.3
0.7 to 1.1
0.2
0.5
D CASE SIZE
AVX TPS
C CASE SIZE
AVX TPS
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 200mARMS. The formula
to calculate this is:
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.
IRIPPLE(RMS) =
0.29( VOUT )( VIN – VOUT ) IP-P
=
12
(L)( f)( VIN )
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 RC can be placed in series
with the VC compensation capacitor CC (Figure 10). Care
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 CF in parallel with the RC/CC network, along
with a small feedforward capacitor CFB, is suggested to
control possible ripple at the VC pin. The LT1976 can be
stabilized using a 47µF ceramic output capacitor and VC
component values of CC = 0.047µF, RC = 12.5k, CF = 100pF
and CFB = 27pF.
OUTPUT RIPPLE VOLTAGE
Figure 3 shows a typical output ripple voltage waveform
for the LT1976. 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:
IP-P =
VOUT ( VIN – VOUT )
( VIN )(L)( f)
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converters, the LT1976 maximum switch current limit
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.)
VOUT
20mV/DIV
47µF TANTALUM
ESR 100mΩ
VOUT
20mV/DIV
47µF CERAMIC
VSW
5V/DIV
VIN = 12V
VOUT = 3.3V
ILOAD = 1A
L = 33µH
1µs/DIV
1976 F03
Figure 3. LT1976 Ripple Voltage Waveform
For high frequency switchers the ripple current slew rate
is also relevant and can be calculated from:
di VIN
=
dt 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.
VRIPPLE = (IP-P )(ESR) + (ESL)
di
dt
Example: with VIN = 12V, VOUT = 3.3V, L = 33µH, ESR =
0.08Ω, ESL = 10nH:
(3.3)(12 – 3.3) = 0.362A
IP-P =
(12)(33e − 6)(200e3)
di
12
=
= 3.63e5
dt 3.3e – 5
VRIPPLE = (0.362A)(0.08) + (10e – 9)(363e3)
= 0.0289 + 0.003 = 32mVP-P
MAXIMUM OUTPUT LOAD CURRENT
Maximum load current for a buck converter is limited by
the maximum switch current rating (IPK). The current
rating for the LT1976 is 1.5A. Unlike most current mode
The LT1976 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 (IP-P/2) is less than IOUT.
IOUT(MAX) = IPK –
( VOUT )( VIN – VOUT ) = I – IP-P
PK
2(L)( f)( VIN )
2
Discontinuous operation occurs when:
IOUT(DIS) ≤
VOUT ( VIN – VOUT )
2(L)( f)( VIN )
For VOUT = 5V, VIN = 8V and L = 20µH:
IOUT(MAX) = 1.5 –
(5)(8 – 5)
2(20e – 6)(200e3)(8)
= 1.5 – 0.24 = 1.26 A
Note that there is less load current available at the higher
input voltage because inductor ripple current increases. At
VIN = 15V, duty cycle is 33% and for the same set of
conditions:
IOUT(MAX) = 1.5 –
(5)(15 – 5)
2(20e – 6)(200e3)(15)
= 1.5 – 0.42 = 1.08 A
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To calculate actual peak switch current in continuous
mode with a given set of conditions, use:
ISW (PK) = IOUT +
(
VOUT VIN – VOUT
( )( )( )
)
2 L f VIN
If a small inductor is chosen which results in discontinous
mode operation over the entire load range, the maximum
load current is equal to:
IPK 2( f)(L)( VIN )
2( VOUT )( VIN – VOUT )
2
IOUT(MAX) =
CHOOSING THE INDUCTOR
Table 3. Inductor Selection Criteria
VENDOR/
PART NUMBER
VALUE (µH)
IRMS(A)
DCR (Ω) HEIGHT (mm)
UP2B-150
15
2.4
0.041
6
UP2B-330
33
1.7
0.062
6
UP2B-470
47
1.4
0.139
6
Coiltronics
UP2B-680
68
1.2
0.179
6
UP2B-101
100
0.95
0.271
6
UP3B-150
15
3.9
0.032
6.8
UP3B-330
33
2.4
0.069
6.8
UP3B-470
47
1.9
0.101
6.8
UP3B-680
68
1.6
0.156
6.8
UP3B-101
100
1.4
0.205
6.8
Sumida
For most applications the output inductor will fall in the
range of 15µH to 100µH. 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 LT1976 switch, which has a 1.5A limit. Higher
values also reduce output ripple voltage and reduce core
loss.
CDRH8D28-150M
15
2.2
0.053
3
CDRH124-150M
15
3.2
0.05
4.5
CDRH127-150M
15
4.5
0.02
8
CDRH8D28-330M
33
1.4
0.122
3
CDRH124-330M
33
2.7
0.97
4.5
CDRH127-330M
33
3.0
0.048
8
CDRH8D28-470M
47
1.25
0.150
3
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.
CDRH125-470M
47
1.8
0.058
6
CDRH127-470M
47
2.5
0.076
8
CDRH124-680M
68
1.5
0.228
4.5
1. Choose a value in microhenries from the graph of
maximum load current. Choosing a small inductor with
lighter loads may result in discontinuous mode of
operation, but the LT1976 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 0.5A, for instance, a 0.5A inductor
may not survive a continuous 2A overload condition.
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.
CDRH127-680M
68
2.1
0.1
8
CDRH124-101M
100
1.2
0.30
4.5
CDRH127-101M
100
1.7
0.17
8
DT3308P-153
15
2.0
0.1
3
DT3308P-333
33
1.4
0.3
3
DT3308P-473
47
1
0.47
3
Coilcraft
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.
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VOUT ( VIN – VOUT )
IPEAK = IOUT +
2( f)(L)( VIN )
VIN = maximum input voltage
f = switching frequency, 200kHz
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 LT1976 is a current mode controller. It uses the VC
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 VC
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 prod}m could occur under shortcircuit conditions. If the power supply output is short
circuited, the feedback amplifier responds to the low
output voltage by raising the control voltage, VC, to its
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
tON(MIN). When combined with the large ratio of VIN to
(VF + 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:
f • tON ≤
VF + I • R
VIN
where:
f = switching frequency
tON = switch on time
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 IPK but will cycle-by-cycle ratchet up to some
higher value. Using the nominal LT1976 clock frequency
of 200kHz, a VIN of 40V and a (VF + I • R) of say 0.7V, the
maximum tON to maintain control would be approximately
90ns, 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 200kHz 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 LT1976 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 LT1976 to
maintain current control.
SOFT-START
For applications where [VIN/(VOUT + VF)] ratios > 10 or
large input surge currents can’t be tolerated, the LT1976
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
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limits the switch current via the VC pin to maintain a
constant voltage ramp rate (dV/dt) at the output capacitor.
A capacitor (C1 in Figure 2) from the CSS pin to the
regulated output voltage determines the output voltage
ramp rate. When the current through the CSS capacitor
exceeds the CSS threshold (ICSS), the voltage ramp of the
output capacitor is limited by reducing the VC pin voltage.
The CSS threshold is proportional to the FB voltage (see
Typical Performance Characteristics) and is defeated for
FB voltages greater than 0.9V (typical). The output dV/dt
can be approximated by:
The minimum average input current depends on the VIN to
VOUT ratio, VC frequency compensation, feedback divider
network and Schottky diode leakage. It can be approximated by the following equation:
 V  (IBIASS + IFB + IS )
IIN(AVG) ≅ IVINS + ISHDN +  OUT 
 VIN 
( η)
where
IVINS = input pin current in sleep mode
VOUT = output voltage
dV ICSS
=
dt CSS
but actual values will vary due to start-up load conditions,
compensation values and output capacitor selection.
VOUT
0.5V/DIV
average input current is greatly reduced resulting in higher
efficiency.
CSS = GND
CSS = 0.1µF
VIN = input voltage
IBIASS = BIAS pin current in sleep mode
IFB = feedback network current
IS = catch diode reverse leakage at VOUT
η = low current efficiency (non Burst Mode operation)
Example: For VOUT = 3.3V, VIN = 12V
CSS = 0.1µF
 3.3  (125µA + 12.5µA + 0.5µA )
IIN(AVG) = 45µA + 5µA +  
 12 
(0.8)
= 45µA + 5µA + 44µA = 99µA
150
TIME (1ms/DIV)
VOUT = 3.3V
TA = 25°C
1976 F04
Figure 4. VOUT dV/dt
Burst Mode OPERATION
To enhance efficiency at light loads, the LT1976 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 LT1976 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, VIN and BIAS quiescent
currents are reduced to typically 45µA and 125µA respectively during the sleep time. As the load current decreases
towards a no load condition, the percentage of time that
the LT1976 operates in sleep mode increases and the
125
SUPPLY CURRENT (µA)
COUT = 47µF
ILOAD = 200mA
VIN = 12V
100
75
50
25
0
0
10
30
40
20
INPUT VOLTAGE (V)
50
60
1976 F05
Figure 5. IQ vs VIN
During the sleep portion of the Burst Mode cycle, the VC
pin voltage is held just below the level needed for normal
operation to improve transient response. See the Typical
Performance Characteristics section for burst and transient response waveforms.
1976f
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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. VOUT
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 CT capacitor discharge when SHDN is taken low. See the Power
Good section for further information.
LEAKAGE
VOUT = 3.3V
VF AT 1A
IQ at 125°C EFFICIENCY
VIN =12V
VIN =12V
VOUT = 3.3 VOUT = 3.3V
DIODE
25°C
125°C
25°C
125°C
IL = 0A
IL = 1A
IR 10BQ100
0.0µA
59µA
0.72V
0.58V
125µA
74.1%
Diodes Inc.
B260SMA
0.1µA
242µA 0.48V
0.41V
215µA
82.8%
Diodes Inc.
B360SMB
0.2µA
440µA 0.45V
0.36V
270µA
83.6%
1µA
1.81mA 0.42V
0.34V
821µA
83.7%
1.7µA 2.64mA 0.40V
0.32V
1088µA
84.5%
IR
MBRS360TR
VOUT
50mV/DIV
IR 30BQ100
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.
VSHDN
2V/DIV
ISW
100mA/DIV
Table 4. Catch Diode Selection Criteria
VIN = 12V
VOUT = 3.3V
IQ = 15µA
TIME (50ms/DIV)
1976 G16
Figure 6. Burst Mode with Shutdown Pin
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 IPEAK at maximum duty cycle.
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
LT1976 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
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 VIN current into the diode in an
attempt to get it to recover. Then, when the diode has
finally turned off, some tens of nanoseconds later, the VSW
node voltage ramps up at an extremely high dV/dt, perhaps 5V to even 10V/ns! With real world lead inductances
the VSW node can easily overshoot the VIN rail. This can
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 VOUT above VIN to drive the output
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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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 (VBOOST = VIN • 2) from
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 VIN or an
independent supply may reduce efficiency but it will reduce the minimum VIN required to start-up with light
loads. If the generated BOOST voltage dissipates too
much power at maximum load, the BOOST voltage the
LT1976 sees can be reduced by placing a Zener diode in
series with the BOOST diode (Figure 7a option).
OPTIONAL
VIN
VIN BOOST
VOUT
LT1976
GND
SW
VBOOST – VSW = VOUT
VBOOST(MAX) = VIN + VOUT
(7a)
VIN
VIN BOOST
LT1976
GND
VOUT
SW
(7b)
VIN BOOST
VDC
LT1976
GND
SHUTDOWN FUNCTION AND UNDERVOLTAGE
LOCKOUT
The SHDN pin on the LT1976 controls the operation of the
IC. When the voltage on the SHDN pin is below the 1.2V
shutdown threshold the LT1976 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 LT1976 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 VIN to VOUT ratios refer to Figure 8 and
the following:
V
V

VUVLO = R1 SHDN + SHDN + ISHDN + VSHDN
R2
 R3

VBOOST – VSW = VIN
VBOOST(MAX) = 2VIN
VIN
A 0.33µF boost capacitor is recommended for most applications. Almost any type of film or ceramic capacitor is
suitable but the ESR should be <1Ω to ensure it can be fully
recharged during the off time of the switch. The capacitor
value is derived from worst-case conditions of 4700ns on
time, 42mA 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.
VHYST =
VOUT (R1)
R3
VOUT
SW
DSS
1976 F07
VBOOST – VSW = VDC
VBOOST(MAX) = VDC + VIN
(7c)
Figure 7. BOOST Pin Configurations
R1 should be chosen to minimize quiescent current during
normal operation by the following equation:
R1 =
VIN – 2V
(1.5) ISHDN(MAX)
(
)
1976f
17
LT1976
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APPLICATIO S I FOR ATIO
Example:
R1 =
12 – 2
= 1.3MΩ
1.5(5µA )
5(1.3MΩ)
= 6.5MΩ (Nearest 1% 6.49MΩ)
1
1.3
R2 =
7 – 1.3
1.3
– 1µA –
1.3MΩ
6.49MΩ
= 408k (Nearest 1% 412k)
R3 =
See the Typical Performance Characteristics section for
graphs of SHDN and VIN currents verses input voltage.
VIN
+
VIN
COMP
–
2.4V
ENABLE
R1
VOUT
R3
15
R2
SHDN
+
SHDN
COMP
3µA
–
1.3V
1976 F08
Figure 8. Undervoltage Lockout
SYNCHRONIZING
Oscillator synchronization to an external input is achieved
by connecting a TTL logic-compatible square wave with a
duty cycle between 20% and 80% to the LT1976 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 (230kHz), not the typical operating frequency of 200kHz. Caution should be used when
synchronizing above 230kHz 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
18
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 no synchronization is required this pin should be connected to ground.
POWER GOOD
The LT1976 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.
LT1976
4
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.
Referring to Figure 2, the PGFB pin is the positive input to
a comparator whose negative input is set at VPGFB. When
PGFB is taken above VPGFB, current (ICSS) is sourced into
the CT pin starting the delay period. When the voltage on
the PGFB pin drops below VPGFB the CT pin is rapidly
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 CT pin determines the amount of
delay time between the PGFB pin exceeding its threshold
(VPGFB) and the PG pin set to a high impedance state.
When the PGFB pin rises above VPGFB current is sourced
(ICT) from the CT pin into the external capacitor. When the
voltage on the external capacitor reaches an internal clamp
(VCT), the PG pin becomes a high impedance node. The
resultant PG delay time is given by t = CCT •␣ (VCT)/(ICT). If
the voltage on the PGFB pin drops below its VPGFB, CCT will
be discharged rapidly and PG will be active low with a
200µA sink capability. If the SHDN pin is taken below its
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 CT = 0.1µF. Figure 10 shows
several different configurations for the LT1976 Power
Good circuitry.
1976f
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LAYOUT CONSIDERATIONS
VOUT
500mV/DIV
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
100k TO VIN
VCT
500mV/DIV
VSHDN
2V/DIV
TIME (10ms/DIV)
1976 F09
Figure 9. Power Good
PG at 80% VOUT with 100ms Delay
PG at VIN > 4V with 100ms Delay
VIN
VIN
200k
200k
PG
VOUT = 3.3V
LT1976
153k
COUT
PGFB
PG
LT1976
PGFB
511k
VOUT = 3.3V
200k
12k
165k
FB
COUT
FB
100k
CT
100k
CT
0.27µF
0.27µF
VOUT Disconnect at 80% VOUT
with 100ms Delay
VOUT Disconnect 3.3V Logic Signal
with 100µs Delay
VIN
VIN
200k
200k
PG
PG
VOUT = 3.3V
LT1976
153k
PGFB
VOUT = 12V
LT1976
COUT
COUT
PGFB
12k
FB
866k
FB
100k
CT
100k
CT
0.27µF
270pF
1976 F10
Figure 10. Power Good Circuits
1976f
19
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parasitic inductance produces a flyback spike across the
LT1976 switch. When operating at higher currents and
input voltages, with poor layout, this spike can generate
voltages across the LT1976 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 VC and FB components should be kept as far away as
possible from the switch and boost nodes. The LT1976
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
LT1976
4 VIN
+
VIN
C2
L1
SW 2
HIGH
FREQUENCY
CIRCULATION
PATH
VOUT
D1
C1
LOAD
continuous copper plate that runs under the LT1976 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 LT1976. 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 LT1976 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:
RSW (IOUT ) ( VOUT )
=
VIN + tEFF (1/2)(IOUT )( VIN )( f)
2
PSW
1976 F11
Figure 11. High Speed Switching Path
C2
CONNECT PIN 8 GND TO THE
PIN 17 EXPOSED PAD GND
VOUT
L1
C1
D1
MINIMIZE
D1-C3
LOOP
GND
Boost current loss:
D2
PLACE VIA's UNDER EXPOSED
PAD TO A BOTTOM PLANE TO
ENHANCE THERMAL
CONDUCTIVITY
PGOOD 16
1 NC
SHDN 15
2 SW
3 NC
C3
LT1976
5 NC
FB 12
R2
6 BOOST
VC 11
C2
C4
7 TCAP
BIAS 10
8 GND
CSS 9
VIN
Quiescent current loss:
RSW = switch resistance (≈0.3 when hot )
tEFF = effective switch current/voltage overlap time
(tr + tf + tIR + tIF)
tr = (VIN/1.7)ns
tf = (VIN/1.2)ns
tIR = tIF = (IOUT/0.05)ns
f = switch frequency
SYNC 14
R1
PBOOST
PQ = VIN (0.0015) + VOUT (0.003)
R3
PGFB 13
4 VIN
VIN
KELVIN SENSE
FEEDBACK
TRACE AND
KEEP SEPARATE
FROM BIAS TRACE
2
VOUT ) (IOUT / 36)
(
=
C5
GND
1976 F12
Figure 12. Suggested Layout
1976f
20
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Example: with VIN = 40V, VOUT = 5V and IOUT = 1A:
PSW
2
0.3)(1) (5)
(
=
+
(97e – 9)(1/2)(1)(40)(200e3)
40
0.04 + 0.388 = 0.43W
PBOOST
2
5) (1/36)
(
=
= 0.02W
40
PQ = 40(0.0015) + 5(0.003) = 0.08W
Total power dissipation is:
PTOT = 0.43 + 0.02 + 0.08 = 0.53W
Thermal resistance for the LT1976 package is influenced
by the presence of internal or backside planes. With a full
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:
TJ = TA + QJA (PTOT)
With the FE16 package (QJA = 45°C/W) at an ambient
temperature of 70°C:
TJ = 70 + 45(0.53) = 94°C
Input Voltage vs Operating Frequency Considerations
The absolute maximum input supply voltage for the LT1976
is specified at 60V. This is based solely on internal semiconductor junction breakdown effects. Due to internal
power dissipation the actual maximum VIN achievable in a
particular application may be less than this.
A detailed theoretical basis for estimating internal power
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 VIN = 40V, VOUT =
5V at 1A and fOSC = 200kHz may be easily achievable,
simultaneously raising VIN to 60V and fOSC to 700kHz is
not possible. Nevertheless, input voltage transients up to
60V can usually be accommodated, assuming the result-
ing increase in internal dissipation is of insufficient time
duration to raise die temperature significantly.
A second consideration is controllability. A potential limitation occurs with a high step-down ratio of VIN to VOUT,
as this requires a correspondingly narrow minimum switch
on time. An approximate expression for this (assuming
continuous mode operation) is given as follows:
tON(MIN) = VOUT + VF/VIN(fOSC)
where:
VIN = input voltage
VOUT = output voltage
VF = Schottky diode forward drop
fOSC = switching frequency
A potential controllability problem arises if the LT1976 is
called upon to produce an on time shorter than it is able to
produce. Feedback loop action will lower then reduce the
VC control voltage to the point where some sort of cycleskipping or Burst Mode behavior is exhibited.
In summary:
1. Be aware that the simultaneous requirements of high
VIN, high IOUT and high fOSC may not be achievable in
practice due to internal dissipation. The Thermal Considerations section offers a basis to estimate internal
power. In questionable cases a prototype supply should
be built and exercised to verify acceptable operation.
2. The simultaneous requirements of high VIN, low VOUT
and high fOSC can result in an unacceptably short
minimum switch on time. Cycle skipping and/or Burst
Mode behavior will result although correct output voltage is usually maintained.
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
1976f
21
LT1976
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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 LT1976 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 LT1976 can be considered as two gm blocks, the error
amplifier and the power stage.
Figure 13 shows the overall loop response with a 330pF VC
capacitor and a typical 100µF tantalum output capacitor.
The response is set by the following terms:
Error amplifier: DC gain is set by gm and RO:
Ω
EA Gain = 650µ • 1.5M = 975
The pole set by CF and RL:
EA Pole = 1/(2π • 1.5M • 330pF) = 322Hz
Unity gain frequency is set by CF and gm:
EA Unity Gain Frequency = 650µF/(2π • 330pF)
= 313kHz
Powerstage: DC gain is set by gm and RL (assume 10Ω):
PS DC Gain = 3 • 10 = 30
Pole set by COUT and RL:
LT1976
CURRENT MODE
POWER STAGE
Ω
gm = 3
gm = 650µ
11
VC
1.6M
Ω
FB
+
12
ESR
R2
–
1.26V
COUT
CC
1976 F13
Figure 13. Model for Loop Response
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 VC 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. If needed, an additional capacitor (CF) can be added to form a pole at
typically one-fifth the switching frequency (if RC = 10k,
CF = 0.047µF)
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.
100
PS Unity Gain Freq = 3/(2π • 100µF) = 4.7kHz.
100
VOUT = 3.3V
COUT = 100µF, 0.1Ω
CC = 330pF
RL/CL = NC
ILOAD = 330µA
135
GAIN (dB)
50
90
0
PHASE (DEG)
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 (RC) in series with the compensation
capacitor. As the value of RC is increased, transient
response will generally improve but two effects limit its
CFB
R1
CF
Unity gain set by COUT and gm:
Output Capacitor Zero = 1/(2π • 100µF • 0.1) = 15.9kHz
OUTPUT
2
ERROR
AMP
RC
PS Pole = 1/(2π • 100µF • 10) = 159Hz
Tantalum output capacitor zero is set by COUT and COUT
ESR
SW
45
–50
10
100
1k
10k
FREQUENCY (Hz)
100k
0
1M
1976 F14
Figure 14. Overall Loop Response
1976f
22
LT1976
U
PACKAGE DESCRIPTIO
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)
3.58
(.141)
16 1514 13 12 1110
6.60 ±0.10
9
2.94
(.116)
4.50 ±0.10
SEE NOTE 4
2.94 6.40
(.116) BSC
0.45 ±0.05
1.05 ±0.10
0.65 BSC
1 2 3 4 5 6 7 8
RECOMMENDED SOLDER PAD LAYOUT
1.10
(.0433)
MAX
4.30 – 4.50*
(.169 – .177)
0° – 8°
0.09 – 0.20
(.0036 – .0079)
0.45 – 0.75
(.018 – .030)
NOTE:
1. CONTROLLING DIMENSION: MILLIMETERS
MILLIMETERS
2. DIMENSIONS ARE IN
(INCHES)
3. DRAWING NOT TO SCALE
0.65
(.0256)
BSC
0.195 – 0.30
(.0077 – .0118)
0.05 – 0.15
(.002 – .006)
FE16 (BC) TSSOP 0203
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
1976f
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.
23
LT1976
RELATED PARTS
PART NUMBER
DESCRIPTION
COMMENTS
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4.4A (IOUT), 100kHz, High Efficiency Step-Down DC/DC Converters
VIN: 7.3V to 45V/64V, VOUT(MIN): 2.21V, IQ: 8.5mA,
ISD: 10µA, DD5/7, TO220-5/7
LT1076/LT1076HV
1.6A (IOUT), 100kHz, High Efficiency Step-Down DC/DC Converters
VIN: 7.3V to 45V/64V, VOUT(MIN): 2.21V, IQ: 8.5mA,
ISD: 10µA, DD5/7, TO220-5/7
LT1676
60V, 440mA (IOUT), 100kHz, High Efficiency Step-Down DC/DC
Converter
VIN: 7.4V to 60V, VOUT(MIN): 1.24V, IQ: 3.2mA, ISD: 2.5µA,
S8
LT1765
25V, 3A (IOUT), 1.25MHz, High Efficiency Step-Down DC/DC
Converter
VIN: 3V to 25V, VOUT(MIN): 1.20V, IQ: 1mA, ISD: 15µA,
SO-8, TSSOP16E
LT1766
60V, 1.2A (IOUT), 200kHz, High Efficiency Step-Down DC/DC
Converter
VIN: 5.5V to 60V, VOUT(MIN): 1.20V, IQ: 2.5mA, ISD: 25µA,
TSSOP16/E
LT1767
25V, 1.5A (IOUT), 1.25MHz, High Efficiency Step-Down DC/DC
Converter
VIN: 3V to 25V, VOUT(MIN): 1.20V, IQ: 1mA, ISD: 6µA,
MS8/E
LT1776
40V, 550mA (IOUT), 200kHz, High Efficiency Step-Down DC/DC
Converter
VIN: 7.4V to 40V, VOUT(MIN): 1.24V, IQ: 3.2mA, ISD: 30µA,
N8, S8
LTC®1875
1.5A (IOUT), 550kHz, Synchronous Step-Down DC/DC Converter
VIN: 2.7V to 6V, VOUT(MIN): 0.8V, IQ: 15µA, ISD: <1µA,
TSSOP16
LT1940
Dual 1.2A (IOUT), 1.1MHz, High Efficiency Step-Down DC/DC
Converter
VIN: 3V to 25V, VOUT(MIN): 1.2V, IQ: 3.8mA, MS10
LT1956
60V, 1.2A (IOUT), 500kHz, High Efficiency Step-Down DC/DC
Converter
VIN: 5.5V to 60V, VOUT(MIN): 1.20V, IQ: 2.5mA, ISD: 25µA,
TSSOP16/E
LT3010
80V, 50mA, Low Noise Linear Regulator
VIN: 1.5V to 80V, VOUT(MIN): 1.28V, IQ: 30µA, ISD: <1µA,
MS8E
LTC3407
Dual 600mA (IOUT), 1.5MHz, High Efficiency Step-Down DC/DC
Converter
VIN: 2.5V to 5.5V, VOUT(MIN): 0.6V, IQ: 40µA MS10
LTC3412
2.5A (IOUT), 4MHz, Synchronous Step-Down DC/DC Converter
VIN: 2.5V to 5.5V, VOUT(MIN): 0.8V, IQ: 60µA, ISD: <1µA,
TSSOP16E
LTC3414
4A (IOUT), 4MHz, Synchronous Step-Down DC/DC Converter
VIN: 2.25V to 5.5V, VOUT(MIN): 0.8V, IQ: 64µA, ISD: <1µA,
TSSOP20E
LT3430
60V, 2.5A (IOUT), 200kHz, High Efficiency Step-Down DC/DC
Converter
VIN: 5.5V to 60V, VOUT(MIN): 1.20V, IQ: 2.5mA, ISD: 30µA,
TSSOP16E
LT3431
60V, 2.5A (IOUT), 500kHz, High Efficiency Step-Down DC/DC
Converter
VIN: 5.5V to 60V, VOUT(MIN): 1.20V, IQ: 2.5mA, ISD: 30µA,
TSSOP16E
LT3433
60V, 400mA (IOUT), 200kHz, Buck-Boost DC/DC Converter
VIN: 5V to 60V, VOUT: 3.3V to 20V, IQ: 100µA, TSSOP-16E
LTC3727/LTC3727-1 36V, 500kHz, High Efficiency Step-Down DC/DC Controllers
VIN: 4V to 36V, VOUT(MIN): 0.8V, IQ: 670µA, ISD: 20µA,
QFN-32, SSOP-28
1976f
24
Linear Technology Corporation
LT/TP 0803 1K PRINTED IN USA
1630 McCarthy Blvd., Milpitas, CA 95035-7417
(408) 432-1900 ● FAX: (408) 434-0507
●
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