HTC LM5171D

1.5A, 280kHz, Boost Regulator
LM5171
FEATURES
• Integrated Power Switch 1.5A Guaranteed
• Wide Input Voltage Range 2.7V to 30V
• High Frequency Allows for Small Components
• Minimum External Components
• Easy External Synchronization
• Frequency Foldback Reduces Component
Stress During an Overcurrent Condition
• Thermal Shutdown with Hysteresis
• Shutdown Current is 50 uA Maximum
• Wide Ambient Temperature Range
• Moisture Sensitivity Level 3
SOP-8 PKG
ORDERING INFORMATION
APPLICATION
• LCD Monitor/TV LED Backlight Driver
• TFT-LCD Power Management
Device
Package
LM5171D
SOP-8
DESCRIPSION
The LM5171 product is 280kHz switching regulator with a high efficiency, 1.5A integrated switch. This part
operates over a wide input voltage range, from 2.7V to 30V. The flexibility of the design allows the chip to
operate in most power supply configurations, including boost, flyback, forward, inverting, and SEPIC.
This IC utilizes current mode architecture, which allows excellent load and line regulation, as well as a practical
means for limiting current. Combining high frequency operation with a highly integrated regulator circuit results
in an extremely compact power supply solution. The circuit design includes provisions for features such as
frequency synchronization, shutdown, and feedback control.
ABSOLUTE MAXIMUM RATINGS
RATING
SYMBOL
VALUE
UNIT
Junction Temperature Range
TJ
-40 to 125
℃
Storage Temperature Range
Tstg
-65 to 150
℃
Thermal Resistance, Junction to Ambient
RθJA
165
℃/W
Thermal Resistance, Junction to Case
RθJC
45
℃/W
-
230
℃
Lead Temperature (Soldering, 10 sec)
(Note 1)
Note 1. 60 second maximum above 183°C.
* Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Maximum ratings applied to the device are
individual stress limit value and are not valid simultaneously. If the limits are exceeded, device functional operation is not implied, damage
may occur and reliability may be affected.
Ordering Information
Package
Order No.
SOP-8
LM5171D
Dec. 2010 - Rev. 1.2.1
Description
1.5A, 280kHz
-1
-
Supply As
Status
Reel
Active
HTC
1.5A, 280kHz, Boost Regulator
LM5171
ABSOLUTE MAXIMUM RATINGS*
Pin Name
Pin Symbol
VMAX
VMIN
ISOURCE
ISINK
IC Power Input
Vcc
30 V
- 0.3 V
N/A
200 mA
Shutdown / Sync
SS
30 V
- 0.3 V
1.0 mA
1.0 mA
Loop Compensation
Vc
6.0 V
- 0.3 V
10 mA
10 mA
Voltage Feedback Input
FB
10 V
- 0.3 V
1.0 mA
1.0 mA
Test Pin
Test
6.0 V
- 0.3 V
1.0 mA
1.0 mA
Power Ground
PGND
0.3 V
- 0.3 V
4.0 A
1.0 mA
Analog Ground
AGND
0V
0V
N/A
10 mA
Switch Input
Vsw
40 V
- 0.3 V
10 mA
3.0 A
* Operating Ratings indicate conditions for which the device is intended to be but do not guarantee specific performance limits. For guaranteed
specifications, see the Electrical Characteristics.)
BLOCK DIAGRAM
VCC
Shutdown
2.0V
Regulator
Thermal
Shutdown
Switch
Delay
Timer
Oscillator
S
Driver
VSW
R
Sync
SS
Q
Frequency
Shift 5:1
x5
63mΩ
Test
PGND
0.4V Detector
-
-
FB
+
1.276V
+
Ramp
Summer
PWM
Comparator
Error Amp
AGND
VC
Dec. 2010 - Rev. 1.2.1
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HTC
1.5A, 280kHz, Boost Regulator
LM5171
PIN CONFIGURATION
VC
1
8
VSW
FB
2
7
PGND
Test
3
6
AGND
SS
4
5
VCC
SOP-8 PKG
PIN DESCRIPTION
Pin No.
Pin Name
Pin Function
1
VC
Loop compensation pin. The VC pin is the output of the error amplifier and is used for loop
compensation and current limit. Loop compensation can be implemented by a simple RC
network as shown in the application circuit on page 4 as R1 and C1.
2
FB
Feedback pin. This pin senses an output voltage and is referenced to 1.276V. When the
voltage at this pin falls below 0.4V, chip switching frequency reduces to 20% of the
nominal frequency.
3
Test
This pin is connected to internal test logic and should either be left floating or be used in
soft start circuit. Connection to a voltage between 9.5 V and 15 V shuts down the internal
oscillator and leaves the power switch running.
4
SS
Synchronization and shutdown pin. This pin may be used to synchronize the part to nearly
twice the base frequency. A TTL low will shut the part down and put it into low current
mode. If synchronization is not used, this pin should be either tied high or left floating for
normal operation.
5
VCC
Input power supply pin. This pin supplies power to the part and should have a bypass
capacitor connected to AGND.
6
AGND
Analog ground. This pin provides a clean ground for the controller circuitry and should not
be in the path of large currents. The output voltage sensing resistors should be connected
to this ground pin. This pin is connected to the IC substrate.
7
PGND
Power ground. This pin is the ground connection for the emitter of the power switching
transistor. Connection to a good ground plane is essential.
8
VSW
High current switch pin. This pin connects internally to the collector of the power switch.
The open voltage across the power switch can be as high as 40 V. To minimize radiation,
use a trace as short as practical.
Dec. 2010 - Rev. 1.2.1
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HTC
1.5A, 280kHz, Boost Regulator
LM5171
APPLICATION CIRCUIT
R2
3.72k
1
2
C1
0.01uF
3
4
SS
VSW
VC
FB
PGND
Test
AGND
SS
VCC
VOUT
D1
8
5V
MBRS120T3
7
6
L1
5
+
22uH
C3
22uF
3.3V
R1
5k
+ C2
R3
1.28k
22uF
ELECTRICAL CHARACTERISTICS
2.7V < Vcc < 30 V, 0°C < TJ < 125°C, unless otherwise stated.
Characteristics
Test Condition
Min
TYP
Max
Unit
FB Reference Voltage
Vc tied to FB : Measure at FB
1.246
1.276
1.300
V
FB Input Current
FB = VREF
-1.0
0.1
1.0
uA
FB Reference Voltage Line Regulation
Vc = FB
-
0.01
0.03
%/V
Error Amp Transconductance
Ivc = ± 25 uA
300
550
800
uMho
Error Amp Gain
(Note 2)
200
500
-
V/ V
Vc Source Current
FB = 1.0V, Vc = 1.25V
25
50
90
uA
Vc Sink Current
FB = 1.5V, Vc = 1.25V
200
625
1500
uA
Vc High Clamp Voltage
FB = 1.0V, Vc sources 25uA
1.5
1.7
1.9
V
Vc Low Clamp Voltage
FB = 1.5V, Vc sinks 25uA
0.25
0.50
0.65
V
Vc Threshold
Reduce Vc from 1.5V until
switching stops
200
625
1500
uA
Base Operating Frequency
FB = 1V
230
280
310
kHz
Reduced Operating Frequency
FB = 0V
30
52
120
kHz
90
94
-
%
0.36
0.40
0.44
V
Error Amplifier
Oscillator
Maximum Duty Cycle
FB Frequency Shift Threshold
Dec. 2010 - Rev. 1.2.1
Frequency drops to reduced
operating frequency
-4
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HTC
1.5A, 280kHz, Boost Regulator
LM5171
ELECTRICAL CHARACTERISTICS (Continued)
2.7V < Vcc < 30 V, 0°C < TJ < 125°C, unless otherwise stated.
Characteristics
Test Condition
Min
TYP
Max
Unit
320
-
500
kHz
Rise Time = 20 ns
2.5
-
-
V
SS = 0V
-15
-3
-
-
3
8
0.50
0.85
1.20
V
2.7V ≤ Vcc ≤ 12V
12
80
350
us
12V ≤ Vcc ≤ 30V
12
36
200
us
ISWITCH = 1.5A (Note 2)
-
0.8
1.4
V
ISWITCH = 1.0A, 0°C ≤ TA ≤ 70°C
-
0.55
1.00
V
ISWITCH = 10mA
-
0.09
0.45
V
50% duty cycle (Note 2)
1.6
1.9
2.4
A
(Note 2)
1.5
1.7
2.2
A
200
250
300
ns
2.7V ≤ VCC ≤ 12V, 10mA ≤ Isw ≤1.0A
-
10
30
mA/A
12V ≤ VCC ≤ 30V, 10mA ≤ Isw ≤ 1.0A
-
-
100
mA/A
-
17
30
mA/A
(Note2)
-
-
100
mA/A
Vsw = 40V, Vcc = 0V
-
2.0
100
uA
Isw = 0
-
5.5
8
mA
Vc < 0.8V, SS = 0V, 2.7V ≤ Vcc ≤ 12V
-
12
60
uA
Vc < 0.8V, SS = 0V, 12V ≤ Vcc ≤ 30V
-
-
100
uA
Minimum Operating Input Voltage
Vsw Switching, Maximum Isw = 10mA
-
2.45
2.70
V
Thermal Shutdown
(Note 2)
150
180
210
°C
Thermal Hysteresis
(Note 2)
-
25
-
°C
Sync / Shutdown
Sync Range
Sync Pulse Transition Threshold
SS Bias Current
SS = 3.0V
Shutdown Threshold
Shutdown Delay
uA
Power Switch
Switch Saturation Voltage
Switch Current Limit
Minimum Pulse Width
∆Icc/∆Ivsw
80% duty cycle
FB = 0V, Isw = 4.0A
(Note 2)
2.7V ≤ VCC ≤ 12V,10mA ≤ Isw ≤ 1.5A
(Note2)
12V ≤ VCC ≤ 30V, 10mA≤ Isw ≤ 1.5A
Switch Leakage
General
Operating Current
Shutdown Mode Current
Note 2. Guaranteed by design, not 100% tested in production.
Dec. 2010 - Rev. 1.2.1
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HTC
1.5A, 280kHz, Boost Regulator
LM5171
TYPICAL PERFORMANCE CHARCTERISTICS
Figure 3. ICC(No Switching) vs. Temperature
Figure 4. ∆Icc/∆Ivsw
Figure 5. VCE(SAT) vs. ISW
vs. Temperature
Figure 6. Minimum Input Voltage vs. Temperature
VCC = 12V
Figure 7. Switching Frequency vs. Temperature
Figure 8. Switching Frequency vs. VFB
Figure 9. Current Limit vs. Temperature
Dec. 2010 - Rev. 1.2.1
Figure 10. Maximum Duty Cycle vs. Temperature
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HTC
1.5A, 280kHz, Boost Regulator
LM5171
TYPICAL PERFORMANCE CHARCTERISTICS (Continued)
Figure 11. Vc Threshold and High Clamp
Figure 12. Shutdown Threshold vs. Temperature
Voltage vs. Temperature
Figure 13. Shutdown Delay vs. Temperature
Figure 14. ISS vs VSS
Figure 15. ICC vs. VIN During Shutdwon
Figure 16. Error Amplifier Transconductance
vs. Temperature
Figure 17. Switch Leakage vs. Temperature
Dec. 2010 - Rev. 1.2.1
Figure 18. Error Amplifier IOUT vs. VFB
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HTC
1.5A, 280kHz, Boost Regulator
LM5171
APPLICATION INFORMATION
Current Mode Control
VIN
Oscillator
VC
S
Q
-
L
Power Switch
R
D1
VSW
+
MBRS120T3
PWM
Comparator
C0
X5
RLoad
63mΩ
Figure 19. Current Mode Controle Scheme
The LM5171 is a current mode control scheme, in which the PWM ramp signal is derived from the power
switch current. This ramp signal is compared to the output of the error amplifier to control the on-time of the
power switch. The oscillator is used as a fixed-frequency clock to ensure a constant operational frequency.
The resulting control scheme features several advantages over conventional voltage mode control. First,
derived directly from the inductor, the ramp signal responds immediately to line voltage changes. This
eliminates the delay caused by the output filter and error amplifier, which is commonly found in voltage mode
controllers. The second benefit comes from inherent pulse−by−pulse current limiting by merely clamping the
peak switching current. Finally, since current mode commands an output current rather than voltage, the filter
offers only a single pole to the feedback loop. This allows both a simpler compensation and a higher
gain−bandwidth over a comparable voltage mode circuit.
Without discrediting its apparent merits, current mode control comes with its own peculiar problems, mainly,
sub harmonic oscillation at duty cycles over 50%. The LM5171 solves this problem by adopting a slope
compensation scheme in which a fixed ramp generated by the oscillator is added to the current ramp. A proper
slope rate is provided to improve circuit stability without sacrificing the advantages of current mode control.
Oscillator and Shutdown
Figure 20. Timing Diagram of Sync and Shutdown
Dec. 2010 - Rev. 1.2.1
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HTC
1.5A, 280kHz, Boost Regulator
LM5171
The oscillator is trimmed to guarantee 18% frequency accuracy. The output of the oscillator turns on the
power switch at a frequency of 280 kHz. The power switch is turned off by the output of the PWM Comparator.
A TTL−compatible sync input at the SS pin is capable of syncing up to 1.8 times the base oscillator frequency.
As shown in Figure 20, in order to sync to a higher frequency, a positive transition turns on the power switch
before the output of the oscillator goes high, thereby resetting the oscillator. The sync operation allows multiple
power supplies to operate at the same frequency.
A sustained logic low at the SS pin will shut down the IC and reduce the supply current.
An additional feature includes frequency shift to 20% of the nominal frequency when the FB pin trigger the
threshold. During power up, overload, or short circuit conditions, the minimum switch on−time is limited by the
PWM comparator minimum pulse width. Extra switch off−time reduces the minimum duty cycle to protect
external components and the IC itself.
As previously mentioned, this block also produces a ramp for the slope compensation to improve regulator
stability.
Error Amplifier
VC
LM5171
FB
120pF
+
1MΩ
Voltage
Clamp
1.276V
C1
0.01uF
R1
5kΩ
Error Amp
Figure 21. Error Amplifier Equivalent Circuit
The FB pin is directly connected to the inverting input of the positive error amplifier, whose non−inverting input
is fed by the 1.276 V reference. The amplifier is transconductance amplifiers with a high output impedance of
approximately 1 MΩ, as shown in Figure 21. The VC pin is connected to the output of the error amplifiers and
is internally clamped between 0.5 V and 1.7 V. A typical connection at the VC pin includes a capacitor in series
with a resistor to ground, forming a pole/zero for loop compensation.
An external shunt can be connected between the VC pin and ground to reduce its clamp voltage.
Consequently, the current limit of the internal power transistor current is reduced from its nominal value.
Switch Driver and Power Switch
The switch driver receives a control signal from the logic section to drive the output power switch. The
switch is grounded through emitter resistors (63mΩ total) to the PGND pin. PGND is not connected to the IC
substrate so that switching noise can be isolated from the analog ground. The peak switching current is
clamped by an internal circuit. The clamp current is guaranteed to be greater than 1.5A and varies with duty
cycle due to slope compensation. The power switch can withstand a maximum voltage of 40 V on the collector
(VSW pin). The saturation voltage of the switch is typically less than 1V to minimize power dissipation.
Dec. 2010 - Rev. 1.2.1
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HTC
1.5A, 280kHz, Boost Regulator
LM5171
Short Circuit Condition
When a short circuit condition happens in a boost circuit, the inductor current will increase during the whole
switching cycle, causing excessive current to be drawn from the input power supply. Since control ICs don’t
have the means to limit load current, an external current limit circuit (such as a fuse or relay) has to be
implemented to protect the load, power supply and ICs.
In other topologies, the frequency shift built into the IC prevents damage to the chip and external components.
This feature reduces the minimum duty cycle and allows the transformer secondary to absorb excess energy
before the switch turns back on.
Figure22. Startup Waveforms of Circuit Shown in the Application Circuit. Load = 400mA
The LM5171 can be activated by either connecting the VCC pin to a voltage source or by enabling the SS pin.
Startup waveforms shown in Figure 22 are measured in the boost converter demonstrated in the Application
circuit on the page 4 of this document. Recorded after the input voltage is turned on, this waveform shows the
various phases during the power up transition.
When the VCC voltage is below the minimum supply voltage, the VSW pin is in high impedance. Therefore,
current conducts directly from the input power source to the output through the inductor and diode. Once VCC
reaches approximately 1.5V, the internal power switch briefly turns on. This is a part of the LM5171 normal
operation. The turn−on of the power switch accounts for the initial current swing.
When the VC pin voltage rises above the threshold, the internal power switch starts to switch and a voltage
pulse can be seen at the VSW pin. Detecting a low output voltage at the FB pin, the built−in frequency shift
feature reduces the switching frequency to a fraction of its nominal value, reducing the minimum duty cycle,
which is otherwise limited by the minimum on−time of the switch. The peak current during this phase is
clamped by the internal current limit.
When the FB pin voltage rises above 0.4V, the frequency increases to its nominal value, and the peak current
begins to decrease as the output approaches the regulation voltage. The overshoot of the output voltage is
prevented by the active pull−on, by which the sink current of the error amplifier is increased once an
overvoltage condition is detected. The overvoltage condition is defined as when the FB pin voltage is 50mV
greater than the reference voltage.
Dec. 2010 - Rev. 1.2.1
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HTC
1.5A, 280kHz, Boost Regulator
LM5171
COMPONENT SELECTION
Frequency Compensation
The goal of frequency compensation is to achieve desirable transient response and DC regulation while
ensuring the stability of the system. A typical compensation network, as shown in Figure 23, provides a
frequency response of two poles and one zero. This frequency response is further illustrated in the Bode plot
shown in Figure 24.
VC
R1
LM5171
C2
C1
AGND
Figure 23. A Typical Compensation Network
The high DC gain in Figure 24 is desirable for achieving DC accuracy over line and load variations. The DC
gain of a transconductance error amplifier can be calculated as follows:
Gain DC = Gm × RO
where:
GM = error amplifier transconductance;
RO = error amplifier output resistance ≈ 1 MΩ.
The low frequency pole, fP1, is determined by the error amplifier output resistance and C1 as:
f P1 =
1
2 πC1RO
f Z1 =
1
2πC1R1
The first zero generated by C1 and R1 is:
The phase lead provided by this zero ensures that the loop has at least a 45° phase margin at the crossover
frequency. Therefore, this zero should be placed close to the pole generated in the power stage which can be
identified at frequency:
fp =
1
2πCO R LOAD
where:
CO = equivalent output capacitance of the error amplifier≈120pF;
RLOAD= load resistance.
Dec. 2010 - Rev. 1.2.1
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HTC
1.5A, 280kHz, Boost Regulator
LM5171
The high frequency pole, fP2, can be placed at the output filter’s ESR zero or at half the switching frequency.
Placing the pole at this frequency will cut down on switching noise. The frequency of this pole is determined by
the value of C2 and R1:
f p2 =
1
2πC2R1
Gain (dB)
One simple method to ensure adequate phase margin is to design the frequency response with a −20dB per
decade slope, until unity−gain crossover. The crossover frequency should be selected at the midpoint between
fZ1 and fP2 where the phase margin is maximized.
Frequency (Log)
Figure 24. Bode Plot of the Compensation Network shown in Figure 23.
VSW Voltage Limit
In the boost topology, VSW pin maximum voltage is set by the maximum output voltage plus the output diode
forward voltage. The diode forward voltage is typically 0.5V for Schottky diodes and 0.8V for ultra fast
recovery diodes
VSW(MAX) = VOUT(MAX) + VF
where:
VF = output diode forward voltage.
In the flyback topology, peak VSW voltage is governed by:
VSW(MAX) = VCC(MAX) + (VOUT + VF) ⅹ N
where:
N = transformer turns ratio, primary over secondary.
When the power switch turns off, there exists a voltage spike superimposed on top of the steady−state
voltage. Usually this voltage spike is caused by transformer leakage inductance charging stray capacitance
between the VSW and PGND pins. To prevent the voltage at the VSW pin from exceeding the maximum rating,
a transient voltage suppressor in series with a diode is paralleled with the primary windings. Another method
of clamping switch voltage is to connect a transient voltage suppressor between the VSW pin and ground.
Dec. 2010 - Rev. 1.2.1
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1.5A, 280kHz, Boost Regulator
LM5171
Magnetic Component Selection
When choosing a magnetic component, one must consider factors such as peak current, core and ferrite
material, output voltage ripple, EMI, temperature range, physical size and cost. In boost circuits, the average
inductor current is the product of output current and voltage gain (VOUT/VCC), assuming 100% energy transfer
efficiency. In continuous conduction mode, inductor ripple current is
I RIPPLE =
Vcc (VOUT - VCC )
(f)(L)(VOUT )
where:
f = 280 kHz
The peak inductor current is equal to average current plus half of the ripple current, which should not cause
inductor saturation. The above equation can also be referenced when selecting the value of the inductor based
on the tolerance of the ripple current in the circuits. Small ripple current provides the benefits of small input
capacitors and greater output current capability. A core geometry like a rod or barrel is prone to generating
high magnetic field radiation, but is relatively cheap and small. Other core geometries, such as toroids, provide
a closed magnetic loop to prevent EMI.
Input Capacitor Selection
In boost circuits, the inductor becomes part of the input filter, as shown in Figure 26. In continuous mode, the
input current waveform is triangular and does not contain a large pulsed current, as shown in Figure 25. This
reduces the requirements imposed on the input capacitor selection. During continuous conduction mode, the
peak to peak inductor ripple current is given in the previous section. As we can see from Figure 25, the product
of the inductor current ripple and the input capacitor’s effective series resistance (ESR) determine the VCC ripple.
In most applications, input capacitors in the range of 10µF to 100 µF with an ESR less than 0.3Ω work well up to
a full 1.5A switch current.
IIN
IL
CIN
VIN
+
-
RESR
Figure 25. Boost Input Voltage and Current Ripple
Waveforms
Figure 26. Boost Circuit Effective Input Filter
The situation is different in a flyback circuit. The input current is discontinuous and a significant pulsed
current is seen by the input capacitors. Therefore, there are two requirements for capacitors in a flyback
regulator: energy storage and filtering. To maintain a stable voltage supply to the chip, a storage capacitor
larger than 20 µF with low ESR is required. To reduce the noise generated by the inductor, insert a 1.0µF
ceramic capacitor between VCC and ground as close as possible to the chip.
By examining the waveforms shown in Figure 27, we can see that the output voltage ripple comes from two
Dec. 2010 - Rev. 1.2.1
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1.5A, 280kHz, Boost Regulator
LM5171
major sources, namely capacitor ESR and the charging/discharging of the output capacitor. In boost circuits,
when the power switch turns off, IL flows into the output capacitor causing an instant ΔV = IIN × ESR. At the same time,
current IL − IOUT charges the capacitor and increases the output voltage gradually.
VOUT Ripple
IL
Figure 27. Typical Output Voltage Ripple
VOUT(RIPPLE)=
(I IN - I OUT )(1 - D)
I OUT D
+
+ I × ESR
(COUT )(f)
(COUT )(f) IN
The equation can be expressed more conveniently in terms of VCC, VOUT and IOUT for design purposes as follows :
VOUT(RIPPLE) =
I OUT (VOUT -V CC )
(I OUT )(VOUT )(ESR)
1
×
+
(COUT )(f)
(COUT )(f)
V CC
The capacitor RMS ripple current is :
I RIPPLE = (I IN - I OUT )2 (1 - D) + (I OUT ) 2 (D) = I OUT
VOUT - VCC
VCC
Although the above equations apply only for boost circuits, similar equations can be derived for flyback circuits.
Reducing the Current Limit
In some applications, the designer may prefer a lower limit on the switch current than 1.5A. An external shunt
can be connected between the VC pin and ground to reduce its clamp voltage. Consequently, the current limit of
the internal power transistor current is reduced from its nominal value.
The voltage on the VC pin can be evaluated with the equation
VC = ISW RE AV
where:
RE=63mΩ, the value of the internal emitter resistor;
AV=5V/V, the gain of the current sense amplifier.
Since RE and AV cannot be changed by the end user, the only available method for limiting switch current below
1.5A is to clamp the VC pin at a lower voltage. If the maximum switch or inductor current is substituted into the
equation above, the desired clamp voltage will result.
A simple diode clamp, as shown in Figure 28 clamps the VC voltage to a diode drop above the voltage on
resistor R3. Unfortunately, such a simple circuit is not generally acceptable if VIN is loosely regulated.
Dec. 2010 - Rev. 1.2.1
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1.5A, 280kHz, Boost Regulator
LM5171
VIN
VCC
R2
VC
D1
R1
R3
C1
C2
Figure 28. Current Limiting using a Diode Clamp
Another solution to the current limiting problem is to externally measure the current through the switch using a
sense resistor. Such a circuit is illustrated in Figure 29.
VCC
PGND
VIN
AGND
VC
+
-
R1
C1
R2
Q1
C2
C3
Output
Ground
RSENSE
Figure 29. Current Limiting using a Current Sense Resistor
The switch current is limited to
I SWITCH(PEAK) =
VBE(Q1)
RSENSE
where:
VBE(Q1) =the base-emitter voltage drop of Q1, typically 0.65V.
The improved circuit does not require a regulated voltage to operate properly. Unfortunately, a price must be
paid for this convenience in the overall efficiency of the circuit. The designer should note that the input and
output grounds are no longer common. Also, the addition of the current sense resistor, RSENCE, results in a
considerable power loss which increases with the duty cycle. Resistor R2 and capacitor C3 form a low-pass
filter to remove noise.
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1.5A, 280kHz, Boost Regulator
LM5171
Subharmonic Oscillation
Subharmonic oscillation (SHM) is a problem found in current-mode control systems, where instability results
when duty cycle exceeds 50%. SHM only occurs in switching regulators with a continuous inductor current.
This instability is not harmful to the converter and usually does not affect the output voltage regulation. SHM will
increase the radiated EM noise from the converter and can cause, under certain circumstances, the inductor to
emit high-frequency audible noise.
SHM is an easily remedied problem. The rising slope of the inductor current is supplemented with internal
“slope compensation” to prevent any duty cycle instability from carrying through to the next switching cycle. In
the LM5171, slope compensation is added during the entire switch on-time, typically in the amount of 180mA/μs.
In some cases, SHM can rear its ugly head despite the presence of the onboard slope compensation. The
simple cure to this problem is more slope compensation to avoid the unwanted oscillation. In that case, an
external circuit, shown in Figure 30, can be added to increase the amount of slope compensation used. This
circuit requires only a few components and is “tacked on” to the compensation network.
VSW
VSW
VC
R1
R2
C1
C2
R3
C3
Figure 30. Technique for Increasing Slope Compensation
The dashed box contains the normal compensation circuitry to limit the bandwidth of the error amplifier.
Resistors R2 and R3 form a voltage divider off of the VSW pin. In normal operation, VSW looks similar to a
square wave, and is dependent on the converter topology. Formulas for calculating VSW in the boost and flyback
topologies are given in the section “VSW Voltage Limit.” The voltage on VSW charges capacitor C3 when the
switch is off, causing the voltage at the VC pin to shift upwards. When the switch turns on, C3 discharges
through R3, producing a negative slope at the VC pin. This negative slope provides the slope compensation.
The amount of slope compensation added by this circuit is
-(1 - D)
R3
f SW
ΔI
= VSW (
)(1 - e R3C3 f SW )(
)
ΔT
R 2 + R3
(1 - D)RE AV
where:
ΔI/ΔT = the amount of slope compensation added (A/s);
VSW = the voltage at the switch node when the transistor is turned off (V);
fSW = the switching frequency, typically 280 kHz;
D = the duty cycle;
RE = 63mΩ, the value of the internal emitter resistor;
AV = 5V/V, the gain of the current sense amplifier.
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In selecting appropriate values for the slope compensation network, the designer is advised to choose a
convenient capacitor, then select values for R2 and R3 such that the amount of slope compensation added is 100
mA/μs. Then R2 may be increased or decreased as necessary. Of course, the series combination of R2 and
R3 should be large enough to avoid drawing excessive current from VSW. Additionally, to ensure that the control
loop stability is improved, the time constant formed by the additional components should be chosen such that
R3 C 3 <
1- D
f SW
Finally, it is worth mentioning that the added slope compensation is a trade-off between duty cycle stability and
transient response. The more slope compensation a designer adds, the slower the transient response will be,
due to the external circuitry interfering with the proper operation of the error amplifier.
Soft−Start
Through the addition of an external circuit, a soft−start function can be added to the LM5171. Soft−start
circuitry prevents the VC pin from slamming high during startup, thereby inhibiting the inductor current from rising
at a high slope.
This circuit, shown in Figure 31, requires a minimum number of components and allows the soft−start circuitry
to activate any time the SS pin is used to restart the converter.
VIN
SS
SS
VCC
D1
4uA
Test
C3
Q
Test
VC
R1
C1
C2
Figure 31. Soft-Start
Resistor R1 and capacitors C1 and C2 form the compensation network. At turn on, the voltage at the VC pin
starts to come up, charging capacitor C3 through transistor Q, clamping the voltage at the VC pin such that
switching begins when VC reaches the VC threshold, typically 1.05V
Therefore, C3 slows the startup of the circuit by limiting the voltage on the VC pin. The soft−start time
increases with the size of C3.
Diode D1 discharges C3 when SS is low. If the shutdown function is not used with this part, the cathode of
D1 should be connected to VIN.
Calculating Junction Temperature
To ensure safe operation of the LM5171, the designer must calculate the on−chip power dissipation and
determine its expected junction temperature. Internal thermal protection circuitry will turn the part off once the
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LM5171
junction temperature exceeds 180°C±30°. However, repeated operation at such high temperatures will ensure a
reduced operating life.
Calculation of the junction temperature is an imprecise but simple task. First, the power losses must be
quantified. There are three major sources of power loss on the LM5171:
• biasing of internal control circuitry, PBIAS
• switch driver, PDRIVER
• switch saturation, PSAT
The internal control circuitry, including the oscillator and linear regulator, requires a small amount of power
even when the switch is turned off. The specifications section of this datasheet reveals that the typical operating
current, IQ, due to this circuitry is 5.5mA. Additional guidance can be found in the graph of operating current vs.
temperature. This graph shows that IQ is strongly dependent on input voltage, VIN, and temperature. Then
PBIAS = VIN IQ
Since the onboard switch is an NPN transistor, the base drive current must be factored in as well. This
current is drawn from the VIN pin, in addition to the control circuitry current. The base drive current is listed in the
specifications as ΔICC/ΔISW, or switch transconductance. As before, the designer will find additional guidance in
the graphs. With that information, the designer can calculate
PDRIVER = VIN I SW ×
I CC
×D
ΔI SW
where:
ISW = the current through the switch;
D = the duty cycle or percentage of switch on−time.
ISW and D are dependent on the type of converter. In a boost converter,
I SW(AVG) ≈ I LOAD × D ×
D≈
1
Efficiency
VOUT - V IN
VOUT
In a flyback converter,
I SW(AVG) ≈
D≈
VOUT I ILOAD
1
×
V IN
Efficiency
VOUT
NS
V
VOUT +
N P IN
The switch saturation voltage, V(CE)SAT, is the last major source of on−chip power loss. V(CE)SAT is the
collector−emitter voltage of the internal NPN transistor when it is driven into saturation by its base drive current.
The value for V(CE)SAT can be obtained from the specifications or from the graphs, as “Switch Saturation Voltage.”
Thus,
PSAT = V(CE)SAT ISW * D
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LM5171
Finally, the total on−chip power losses are
PD = PBIAS + PDRIVER + PSAT
Power dissipation in a semiconductor device results in the generation of heat in the junctions at the surface of
the chip. This heat is transferred to the surface of the IC package, but a thermal gradient exists due to the
resistive properties of the package molding compound. The magnitude of the thermal gradient is expressed in
manufacturers’ data sheets as θJA, or junction−to−ambient thermal resistance.
The on−chip junction
temperature can be calculated if θJA, the air temperature near the surface of the IC, and the on−chip power
dissipation are known.
TJ = TA + (PD • θJA)
where:
TJ = IC or FET junction temperature (°C);
TA = ambient temperature (°C);
PD = power dissipated by part in question (W);
θJA = junction–to–ambient thermal resistance (°C/W). For the LM5171 θJA=165°C/W.
Once the designer has calculated TJ, the question of whether the LM5171 can be used in an application is
settled. If TJ exceeds 150°C, the absolute maximum allowable junction temperature, the LM5171 is not suitable
for that application.
If TJ approaches 150°C, the designer should consider possible means of reducing the junction temperature.
Perhaps another converter topology could be selected to reduce the switch current. Increasing the airflow
across the surface of the chip might be considered to reduce TA.
Circuit Layout Guidelines
In any switching power supply, circuit layout is very important for proper operation. Rapidly switching currents
combined with trace inductance generates voltage transitions that can cause problems. Therefore the following
guidelines should be followed in the layout.
1. In boost circuits, high AC current circulates within the loop composed of the diode, output capacitor, and
on−chip power transistor. The length of associated traces and leads should be kept as short as possible.
In the flyback circuit, high AC current loops exist on both sides of the transformer. On the primary side, the
loop consists of the input capacitor, transformer, and on−chip power transistor, while the transformer, rectifier
diodes, and output capacitors form another loop on the secondary side. Just as in the boost circuit, all
traces and leads containing large AC currents should be kept short.
2. Separate the low current signal grounds from the power grounds. Use single point grounding or ground
plane construction for the best results.
3. Locate the voltage feedback resistors as near the IC as possible to keep the sensitive feedback wiring short.
Connect feedback resistors to the low current analog ground.
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