Datasheet LM4652TF, LM4651N, LM4652TA Datasheet (NSC)

Page 1
August 2000
LM4651 & LM4652 Overture
LM4651 & LM4652
Overture
Audio Power Amplifier
170W Class D Audio Power Amplifier Solution
General Description
The IC combination of the LM4651 driver and the LM4652 power MOSFET provides a high efficiency, Class D sub­woofer amplifier solution.
The LM4651 is a fully integrated conventional pulse width modulator driver IC. The IC contains short circuit, under voltage, over modulation, and thermal shut down protection circuitry. It contains a standby function, which shuts down the pulse width modulation and minimizes supply current. The LM4652 is a fully integrated H-bridge power MOSFET IC in a TO-220 power package. Together, these two IC’s form a simple, compact high power audio amplifier solution complete with protection normally seen only in Class AB amplifiers. Few external components and minimal traces between the IC’s keep the PCB area small and aids in EMI control.
The near rail-to-rail switching amplifier substantially in­creases the efficiencycompared to Class AB amplifiers. This high efficiency solution significantly reduces the heat sink size compared to a Class AB IC of the same power level. This two-chip solution is optimum for powered subwoofers and self powered speakers.
Key Specifications
n Output power into 4with<10% THD. 170W (Typ) n THD at 10W, 4, 10 − 500Hz. n Maximum efficiency at 125W 85% (Typ) n Standby attenuation.
Features
n Conventional pulse width modulation. n Externally controllable switching frequency. n 50kHZ to 200kHz switching frequency range. n Integrated error amp and feedback amp. n Turn−on soft start and under voltage lockout. n Over modulation protection (soft clipping). n Short circuit current limiting and thermal shutdown
protection.
n 15 Lead TO−220 isolated package. n Self checking protection diagnostic.
Applications
n Powered subwoofers for home theater and PC’s n Car booster amplifier n Self-powered speakers
<
0.3% THD (Typ)
>
100dB (Min)
170W Class D Audio Power Amplifier Solution
Connection Diagrams
LM4651 Plastic Package
Top View
Order Number LM4651N
See NS Package Number N28B
DS101277-72
LM4652 Plastic Package (Note 8)
DS101277-73
Isolated TO-220 Package
Order Number LM4652TF
See NS Package Number TF15B
or
Non-Isolated TO-220 Package
Order Number LM4652TA
See NS Package Number TA15A
Overture®is a registered trademark of National Semiconductor Corporation.
© 2001 National Semiconductor Corporation DS101277 www.national.com
Page 2
Absolute Maximum Ratings (Notes 1, 2)
If Military/Aerospace specified devices are required, please contact the National Semiconductor Sales Office/ Distributors for availability and specifications.
Supply Voltage Output Current (LM4652) 10A
LM4651 & LM4652
Power Dissipation (LM4651) (Note 3) 1.5W Power Dissipation (LM4652) (Note 3) 32W
±
22V
Operating Ratings (Notes 1, 2)
Temperature Range −40˚C T Supply Voltage |V
Thermal Resistance LM4651 N Package
θJA 52˚C/W θJC 22˚C/W
+
|+|V−| 22V to 44V
ESD Susceptibility (LM4651) (Note 4) 2000V
LM4652 (pins 2,6,10,11) 500V
ESD Susceptibility (LM4651) (Note 5) 200V
LM4652 (pins 2,6,10,11) 100V
LM4652 TF, TO−220 Package
θJA 43˚C/W θJC 2.0˚C/W
Junction Temperature (Note 6) 150˚C Soldering Information
N, TA and TF Package (10 seconds) 260˚C
Storage Temperature −40˚C to + 150˚C
LM4652 T, TO−220 Package
θJA 37˚C/W θJC 1.0˚C/W
System Electrical Characteristics for LM4651 and LM4652 (Notes 1, 2)
The following specifications apply for +VCC= +20V, −VEE= −20V, fSW= 125kHz, fIN= 100Hz, RL=4Ω, unless otherwise specified. Typicals apply for T
Symbol Parameter Conditions
I
CQ
I
STBY
A
P
M
O
Total Quiescent Power Supply Current
Standby Current V Standby Attenuation V
Output Power (Continuous Average)
η Efficiency at P η
Pd
Efficiency (LM4651 & LM4652)
Power Dissipation (LM4651 + LM4652)
THD+N Total Harmonic Distortion Plus Noise
e
OUT
Output Noise A Weighted, no signal, RL=4 550 µV SNR Signal-to-Noise Ratio V
OS
Output Offset Voltage VIN= 0V, IO= 0mA, R PSRR Power Supply Rejection Ratio
= 25˚C. For specific circuit values, refer to Figure 1 (Typical Audio Application Circuit).
A
Typical Units
= 0V, LO= 0mA, |I
V
CIN
R
DLY
R
DLY
13 = 5V, Stby: On 17 mA
PIN
13 = 5V, Stby: On
PIN
R
=4Ω, 1% THD 125 W
L
R
=4Ω, 10% THD 155 W
L
R
=8Ω, 1% THD 75 W
L
R
=8Ω, 10% THD 90 W
L
f
= 75kHz, RL=4Ω, 1% THD 135 W
SW
f
= 75kHz, RL=4Ω, 10% THD 170 W
SW
=5W PO= 5W, R
O
= 125W, THD = 1% 85 %
P
O
= 125W, THD = 1% (max) 22 W
P
O
f
= 75kHz, PO= 135W,
SW
=0 = 10k
=5k 55 %
DLY
VCC+
|+|I
VEE−
|
THD = 1% (max) 10W, 10Hz f
500Hz, AV=18dB
IN
10Hz BW 80kHz
A-Wtg, P 22kHz BW, P
=4Ω, 10Hz BW 30kHz
R
L
+V
CC
= 125W, RL4 92 dB
out
= 125W, RL4 89 dB
out
=0 0.7 V
OFFSET
AC
=−V
=1V
EE
RMS,fAC
AC
= 120Hz
LM4651 & LM4652
237 124
>
115 dB
22 W
0.3 %
37 dB
+85˚C
A
mA mA
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Page 3
Electrical Characteristics for LM4651 (Notes 1, 2, 7)
The following specifications apply for +VCC= +20V, −VEE= −20V, fSW= 125kHz, unless otherwise specified. Limits apply for T
= 25˚C. For specific circuit values, refer to Figure 1 (Typical Audio Application Circuit).
A
Symbol Parameter Conditions
I
CQ
Standby V
IL
V
IH
f
SW
f
SWerror
T
dead
T
OverMod
Total Quiescent Current
Standby Low Input Voltage Not in Standby Mode 0.8 V Standby High Input Voltage In Standby Mode 2.5 2.0 V
Switching Frequency Range 50% Duty Cycle Error R
Dead Time R Over Modulation Protection Time Pulse Width Measured at 50% 310 ns
LM4652 not connected, I
|+|I
|I
VCC+
R
= 15k 65 kHz
OSC
R
=0 200 kHz
OSC
=4kΩ,fSW= 125kHz 1 3 %
OSC
=0 27 ns
DLY
VEE−
|, R
DLY
O
=0
= 0mA,
Min Typical Max Units
15 36 45 mA
LM4651
Electrical Characteristics for LM4652 (Notes 1, 2, 7)
The following specifications apply for +VCC= +20V, −VEE= −20V, unless otherwise specified. Limits apply for TA= 25˚C. For specific circuit values, refer to Figure 1 (Typical Audio Application Circuit).
Symbol Parameter Conditions
DSS
V
(BR)
I
DSS
VGS
th
R
DS(ON)
t
r
t
f
I
D
Note 1: Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is functional, but do not guarantee specific performance limits. Electrical Characteristics state DC and AC electrical specifications under particular test conditions which guarantee specific performance limits. This assumes that the device is within the Operating Ratings. Specifications are not guaranteed for parameters where no limit is given, however, the typical value is a good indication of device performance.
Note 2: All voltages are measured with respect to the GND pin unless otherwise specified. Note 3: For operating at case temperatures above 25˚C, the LM4651 must be de−rated based on a 150˚C maximum junction temperature and a thermal resistance
of θ
2.0 ˚C/W (junction to case) for the isolated package (TF) or a thermal resistance of θ
Note 4: Human body model, 100 pF discharged through a 1.5 kresistor. Note 5: Machine Model, 220pF-240pF discharge through all pins. Note 6: The operating junction temperature maximum, T Note 7: Limits are guaranteed to National’s AOQL (Average Outgoing Quality Level). Note 8: The LM4652TA package TA15A is a non-isolated package, setting the tab of the device and the heat sink at −V potential when the LM4652 is directly
mounted to the heat sink using only thermal compound. If a mica washer is used in addition to thermal compound, θ will be isolated from −V.
Drain−to−Source Breakdown Voltage
VGS = 0 55 V
Drain−to−Source Leakage Current VDS = 44VDC, VGS = 0V 1.0 mA Gate Threshold Voltage VDS = VGS, ID = 1mA Static Drain−to−Source On
Resistance Rise Time
Fall Time Maximum Saturation Drain
Current
= 62 ˚C/W (junction to ambient), while the LM4652 must be de−rated based on a 150˚C maximum junction temperature and a thermal resistance of θJC=
JA
VGS=6V VGD=6V
=0 VGD=6V
=0 VGS=6V
is 150˚C.
jmax
,ID=6A
DC
, VDS = 40VDC,R
DC
, VDS = 40VDC,R
DC
, VDS = 10V
DC
DC
DC
GATE
GATE
DC
= 1.0˚C/W (junction to case) for the non-isolated package (T).
JC
Min Typical Max Units
810 A
(case to sink) is increased, but the heat sink
CS
LM4652
0.85 V 200 300 m
25 ns
26 ns
LM4651 & LM4652
DC
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Electrical Characteristics for LM4652 (Notes 1, 2, 7) (Continued)
LM4651 & LM4652
FIGURE 1. Typical Application Circuit and Test Circuit
DS101277-68
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Page 5
LM4651 Pin Descriptions
Pin No. Symbol Description
1 OUT
2,27 BS
3HG 4HG
1
,BS
1
2 1 2
5,15 GND The ground pin for all analog circuitry.
6 +6V 7+V 8 −6V
9F 10 E 11 E
BYP
CC
BYP
BKVO
RRIN
RRVO
12 TSD The thermal shut down input pin for the thermal shut down output of the LM4652. 13 STBY Standby function input pin. This pin is CMOS compatible.
14 FBK
1
16 OSC 17 Delay The dead time setting pin.
18 SCKT Short circuit setting pin. Minimum setting is 10A. 19 FBK
20,21 −V 22,23 −V
2
DDBYP
EE
24 START
25 LG 26 LG 28 OUT
1 2
2
The reference pin of the power MOSFET output to the gate drive circuitry. The bootstrap pin provides extra bias to drive the upper gates, HG1,HG2. High−Gate#1 is the gate drive to a top side MOSFET in the H-Bridge. High−Gate#2 is the gate drive to a top side MOSFET in the H-Bridge.
The internally regulated positive voltage output for analog circuitry. This pin is available for internal regulator bypassing only.
The positive supply input for the IC. The internally regulated negative voltage output for analog circuitry. This pin is available
for internal regulator bypassing only. The feedback instrumentation amplifier output pin. The error amplifier inverting input pin. The input audio signal and the feedback signal are
summed at this input pin. The error amplifier output pin.
The feedback instrumentation amplifier pin. This must be connected to the feedback filter from V
(pin 15 on the LM4652 ).
O1
The switching frequency oscillation pin. Adjusting the resistor from 15.5kto 0 changes the switching frequency from 75kHz to 225kHz.
The feedback instrumentation amplifier pin. This must be connected to the feedback filter from V
(pin 7 on the LM4652 ).
O2
The regulator output for digital blocks. This pin is for bypassing only. The negative voltage supply pin for the IC. The start up capacitor input pin. This capacitor adjusts the start up time of the diagnostic
sequence for the modulator. Refer to Start up Sequence and Timing in the Application Information section.
Low−Gate#1 is the gate drive to a bottom side MOSFET in the H-Bridge. Low−Gate#2 is the gate drive to a bottom side MOSFET in the H-Bridge. The reference pin of the power MOSFET output to the gate drive circuitry.
LM4651 & LM4652
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Page 6
LM4652 Pin Descriptions
Pin No. Symbol Description
1 GND A ground reference for the thermal shut down circuitry.
LM4651 & LM4652
2LG 3−V
1
EE
4 TSD
Low−Gate#1 is the gate input to a bottom side MOSFET in the H-Bridge. The negative voltage supply input for the power MOSFET H-Bridge. The thermal shut down flag pin. This pin transitions to 6V when the die temperature
exceeds 150˚C. 5 NC No connection 6LG 7VO
2 2
Low−Gate#2 is the gate input to a bottom side MOSFET in the H-Bridge.
The switching output pin for one side of the H-Bridge. 8 NC No connection. 9 NC No connection.
10 HG
2
High−Gate#2 is the gate input to a top side MOSFET in the H-Bridge.
11 NC No connection. 12 NC No connection. 13 +V 14 HG 15 VO
CC
1
2
The positive voltage supply input for the power MOSFET H-Bridge.
High−Gate#1 is the gate input to a top side MOSFET in the H-Bridge.
The switching output pin for one side of the H-Bridge.
Note: NC, no connect pins are floating pins. It is best to connect the pins to GND to minimize any noise from being coupled into the pins.
External Components Description (Refer to Figure 1)
Components Functional Description
1. R
2. R
3. R
4. C
1
2
f
f
Works with R2,R
)/ R
R
)−(R2/R1) + .5].
fl2
fl2
See description above for R1.
Sets the gain and bandwidth of the system by creating a low pass filter for the Error
Amplifier’s feedback with C
See description above for Rf.
fl1
and R
to set the gain of the system. Gain = [(R2/R1) x ((R
fl2
. 3dB pole is at fC= 1/(2πRfCf) (Hz).
f
Provides a reduction in the feedback with R
5. R
fI1
reduce effects on the pole created by R
fI2
System Gain.
6. R
7. C
8. R
9. C
10. L
11. C
12. C
byp
and C
fI2
fI1
fI3
fI2
1
1
fI2
note for R
See description above for R
Establish the second pole for the low pass filter in the feedback path at fC=
1/(2πR
See description above for R
Combined with C
= 1/[2π(L12C
Filters high frequency noise from the amplifier’s output to ground. Recommended value
is 0.1µF to 1µF.
See description for L1.
creates a low pass filter with a pole at fC= 1/(2πR
fI1
for effect on System Gain.
1,R2
.
fI2
) (Hz).
fI3CfI2
.
fI3
creates a 2−pole, low pass output filter that has a −3dB pole at f
BYP
1
)
2
] (Hz).
BYP
R
Bypass capacitors for VCC,VEE, analog and digital voltages (VDD, +6V, −6V). See
13. C
B1−CB4
Supply Bypassing and High Frequency PCB Design in the Application Information
section for more information.
14. B
15. R
16. C
START
17. R
18. R
19. D
BT
DLY
SCKT
OSC
1
Provides the bootstrap capacitance for the boot strap pin.
Sets the dead time or break before make to T
Controls the startup time with T
Sets the output short circuit current with I
START
= (8.5x104)C
SCKT
Controls the switching frequency with fSW=1X109/ (4000 + R
Schottky diode to protect the output MOSFETs from fly back voltages.
should be 10 X R
fI2.RfI1
and C
. See also note for R1,R2for effect on
fI1
= (1.7x10
DLY
START
= (1x105)/ (10k\ R
fI2CfI1
−12
)(500+R
(seconds).
OSC
minimum to
fI2
) (Hz). See also
) (seconds).
DLY
) (A).
SCKT
) (Hz).
+
fl1
C
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Page 7
External Components Description (Refer to Figure 1) (Continued)
Components Functional Description
,
C
20.
21. R
SBY1,CSBY2
C
OFFSET
22. C
23. R
SBY3
IN
gate
Supply de-coupling capacitors. See Supply Bypassing in the Application Information section.
Provides a small DC voltage at the input to minimize the output DC offset seen by the load. This also minimize power on pops and clicks.
Blocks DC voltages from being coupled into the input and blocks the DC voltage created
OFFSET
from the source.
by R Slows the rise and fall time of the gate drive voltages that drive the output FET’s.
Typical Performance Characteristics
LM4651 & LM4652
Output Power vs. Supply Voltage
THD+N vs. Output Power R
=4
L
DS101277-4
Output Power vs. Supply Voltage
THD+N vs. Output Power R
=8
L
DS101277-5
DS101277-6
DS101277-7
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Page 8
Typical Performance Characteristics (Continued)
THD+N vs. Output Power R
=4
L
LM4651 & LM4652
THD+N vs. Frequency vs. Bandwidth R
=4
L
DS101277-8
THD+N vs. Output Power R
=8
L
THD+N vs. Frequency vs. Bandwidth R
=8
L
DS101277-9
DS101277-10
THD+N vs. Frequency vs. Bandwidth R
=4
L
DS101277-12
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THD+N vs. Frequency vs. Bandwidth R
=8
L
DS101277-11
DS101277-13
Page 9
Typical Performance Characteristics (Continued)
LM4651 & LM4652
Power Dissipation & Efficiency vs. Output Power
Frequency Response R
=4
L
DS101277-16
Clipping Power Point & Efficiency vs. Switching Frequency (f
SW
)
Supply Current vs. Switching Frequency (LM4651 & LM4652)
DS101277-17
Supply Current vs. Supply Voltage (LM4651 & LM4652)
DS101277-18
DS101277-21
R
DS
(ON)
DS101277-20
vs. Temperature
DS101277-23
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Page 10
Application Information
GENERAL FEATURES System Functional Information: The LM4651 is a conven-
tional pulse width modulator/driver. As Figure 2 shows the incoming audio signal is compared with a triangle waveform with a much higher frequency than the audio signal (not
LM4651 & LM4652
drawn to scale). The comparator creates a variable duty cycle squarewave. The squarewave has a duty cycle propor­tional to the audio signal level. The squarewave is then properly conditioned to drive the gates of power MOSFETs in an H-bridge configuration, such as the LM4652. The pulse train of the power MOSFETs are then fed into a low pass filter (usually a LC) which removes the high frequency and delivers an amplified replica of the audio input signal to the load.
DS101277-1
FIGURE 2. Conventional Pulse Width Modulation
Standby Function: The standby function of the LM4651 is
CMOS compatible, allowing the user to perform a muting of the music as well as turning off all power MOSFETs by shutting down the pulse width waveform. Standby has the added advantage of minimizing the quiescent current. Be­cause standby shuts down the pulse width waveform, the attenuation of the music is complete ( mized, and any output noise is eliminated since there is no modulation waveform. By placing a logic ’1’ or 5V at pin 13, the standby function will be enabled. A logic ’0’ or 0V at pin 13 will disable the standby function allowing modulation by the input signal.
>
120dB), EMI is mini-
The value of C
sets the time it takes for the IC to go
START
though the start-up sequence and the frequency that the diagnostic circuitry checks to see if an error condition has been corrected. An Error condition occurs if current limit, thermal shut down, under voltage detection, or standby are sensed. The self-diagnostic circuit checks to see if any one of these error flags has been removed at a frequency set by the C
capacitor. For example, if the value of C
START
START
10µF then the diagnostic circuitry will check approximately every second to see if an error condition has been corrected. If the error condition is no longer present, the LM4651/52 will return to normal operation.
DS101277-70
FIGURE 3. Startup Timing Diagram
Current Limiting and Short Circuit Protection: The resis-
tor value connected between the SCKT pin and GND deter­mines the maximum output current. Once the output current is higher than the set limit, the short circuit protection turns all power MOSFETsoff. The current limit is set to a minimum of 10A internally but can be increased by adjusting the value of the R
resistor.Equation (3) shows how to find R
SCKT
I
= 1X105/(10k\ R
SCKT
) (Amps) (3)
SCKT
SCKT
is
.
Under Voltage Protection: The under voltage protection disables the output driver section of the LM4651 while the supply voltage is below
±
10.5V. This condition can occur as power is first applied or when low line, changes in load resistance or power supply sag occurs. The under voltage protection ensures that all power MOSFETs are off, eliminat­ing any shoot-through current and minimizing pops or clicks during turn-on and turn-off. The under voltage protection gives the digital logic time to stabilize into known states providing a popless turn on.
Start Up Sequence and Self-Diagnostic Timing: The LM4651 has an internal soft start feature (see Figure 3) that ensures reliable and consistent start-up while minimizing turn-on thumps or pops. During the start-up cycle the system is in standby mode. This start-up time is controlled externally by adjusting the capacitance (C
) value connected to
START
the START pin. The start-up time can be controlled by the capacitor value connected to the START pin given by Equa­tion (1) or (2):
t
= (8.4x104)C
START
C
START=TSTART
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START
/(8.5x104) (Farads) (2)
(seconds) (1)
This feature is designed to protect the MOSFETs by setting the maximum output current limit under short circuit condi­tions. It is designed to be a fail-safe protection when the output terminals are shorted or a speaker fails and causes a short circuit condition.
Thermal Protection The LM4651 has internal circuitry (pin
12) that is activated by the thermal shutdown output signal from the LM4652 (pin 4). The LM4652 has thermal shut down circuitry that monitors the temperature of the die. The voltage on the TSD pin (pin 4 of the LM4652) goes high (6V) once the temperature of the LM4652 die reaches 150˚C. This pin should be connected directly to the TSD pin of the LM4651 (pin 12). The LM4651 disables the pulse width waveform when the LM4652 transmits the thermal shutdown flag. The pulse width waveform remains disabled until the TSD flag from the LM4652 goes low, signaling the junction temperature has cooled to a safe level.
Dead Time Setting The DELAY pin on the LM4651 allows the user to set the amount of dead time or break before make of the system. This is the amount of time one pair of FETs are off before another pair is switched on. Increased dead time will reduce the shoot through current but has the disadvantage of increasing THD. The dead time should be
Page 11
Application Information (Continued)
reduced as the desired bandwidth of operation increases. The dead time can be adjusted with the R Equation (4):
T
DLY
= 1.7x10
−12
(500 + R
) (Seconds) (4)
DLY
Currently, the recommended value is 5k.
Oscillator Control: The modulation frequency is set by an external resistor, R
, connected between pin 16 and
OSC
GND. The modulation frequency can be set within the range of 50kHz to 225kHz according to the design requirements. The values of R
OSC
and f
can be found by Equation (5)
OSC
and (6):
f
= 1x109/ (4000 + R
OSC
R
= (1x109/f
OSC
) − 4000 (Ω) (6)
OSC
) (Hz) (5)
OSC
DLY
resistor by
LM4651 & LM4652
Feedback Amplifier and Filter: The purpose of the feed-
back amplifier is to differentially sample the output and pro­vide a single-ended feedback signal to the error amplifier to close the feedback loop. The feedback is taken directly from the switching output before the demodulating LC filter to avoid the phase shift caused by the output filter. The signal fed back is first low pass filtered with a single pole or dual pole RC filter to remove the switching frequency and its harmonics. The differential signal, derived from the bridge output, goes into the high input impedance instrumentation amplifier that is used as the feedback amplifier. The instru­mentation amplifier has an internally fixed gain of 1. The use of an instrumentation amplifier serves two purposes. First, it’s input are high impedance so it doesn’t load down the output stage. Secondly, an IA has excellent common-mode rejection when its gain setting resistors are properly matched. This feature allows the IA to derive the true feed­back signal from the differential output, which aids in improv­ing the system performance.
Equations (5) and (6) are for R greater than zero will increase the value needed for R For R
DLY
=5kΩ,R
will need to be increased by about
OSC
= 0. Using a value of R
DLY
DLY
OSC
2k.As the graphs show, increasing the switching frequency will reduce the THD but also decreases the efficiency and maximum output power level before clipping. Increasing the switching frequency increases the amount of loss because switching currents lower the efficiency across the output power range. A higher switching frequency also lowers the maximum output power before clipping or the 1% THD point occur.
Over-Modulation Protection: The over-modulation protec­tion is an internally generated fixed pulse width signal that prevents any side of the H-bridge power MOSFETs from remaining active for an extended period of time. This condi­tion can result when the input signal amplitude is higher than the internal triangle waveform. Lack of an over modulation signal can increase distortion when the amplifier’s output is clipping. Figure 4 shows how the over modulation protection works.
DS101277-2
FIGURE 4. Over Modulation Protection
The over modulation protection also provides a ’soft clip’ type response on the top of a sine wave. This minimum pulse time is internally set and cannot be adjusted. As the switching frequency increases this minimum time becomes a higher percentage of the period (T
= 1/fSW). Because
PERIOD
the over modulation protection time is a higher percentage of the period, the peak output voltage is lower and, therefore, the output power at clipping is lower for the same given supply rails and load.
.
DS101277-3
FIGURE 5. Feedback instrumentation Amplifier
Schematic
Error Amplifier: The purpose of the error amplifier is to sum
the input audio signal with the feedback signal derived from the output. This inverting amplifier’s gain is externally con­figurable by resistors Rf and R1. The parallel feedback ca­pacitor and resistor form a low pass filter that limits the frequency content of the input audio signal and the feedback signal. The pole of the filter is set by Equation (7).
f
= 1/(2πRfCf) (Hz) (7)
IP
On-Board Regulators: The LM4651 has its own internal supply regulators for both analog and digital circuits. Sepa-
±
rate
6V regulators exist solely for the analog amplifiers, oscillator and PWM comparators. A separate voltage regu­lator powers the digital logic that controls the protection, level shifting, and high−/low−side driver circuits. System per­formance is enhanced by bypassing each regulator’s output.
±
The
6V regulator outputs, labeled +6V
−6V regulator output, −V passed to −V
(pin 8) should be bypassed to ground. The digital
BYP
DDBYP
(pins 22 & 23). The voltage level of −V
EE
(pins 20 & 21) should be by-
(pin 6) and
BYP
DDBYP
should be always be 6V closer to ground than the negative rail, −V
. As an example, if −VEE= −20V, then −V
EE
DDBYP
should equal −14V. Recommended capacitor values and type can be found in Figure 1, Typical audio Application
Circuit.
APPLICATIONS HINTS
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Page 12
Application Information (Continued)
Introduction
National Semiconductor (NSC) is committed to providing application information that assists our customers in obtain­ing the best performance possible from our products. The
LM4651 & LM4652
following information is provided in order to support this commitment. The reader should be aware that the optimiza­tion of performance was done using a reference PCB de­signed by NSC and shown in Figure 7 through 11. Variations in performance can occur because of physical changes in the printed circuit board and the application. Therefore, the designer should know that component value changes may be required in order to optimize performance in a given application. The values shown in this data sheet can be used as a starting point for evaluation purposes. When working with high frequency circuits, good layout practices are also critical to achieving maximum performance.
pin(s) using leads as short as possible. For supply stabiliz­ing, large electrolytic capacitors (3,300µF to 15,000µF) are needed. The value used is design and cost dependent.
High Frequency PCB Design
A double-sided PCB is recommended when designing a class D amplifier system. One side should contain a ground plane with the power traces on the other side directly over the ground plane. The advantage is the parasitic capaci­tance created between the ground plane and the power planes. This parasitic capacitance is very small (pF) but is the value needed for coupling high frequency noise to ground. At high frequencies, capacitors begin to act more like inductors because of lead and parasitic inductance in the capacitor. For this reason, bypassing capacitors should be surface mount because of their low parasitic inductance. Equation (8) shows how to determine the amount of power to ground plane capacitance.
Input Pre-Amplifier with Subwoofer Filter
The LM4651 and LM4652 Class D solution is designed for low frequency audio applications where low gain is required. This necessitates a pre−amplifier stage with gain and a low pass audio filter. An inexpensive input stage can be de­signed using National’s LM833 audio operational amplifier and a minimum number of external components. Again of 10 (20dB) is recommended for the pre−amplifier stage. For a subwoofer application, the pole of the low pass filter is normally set within the range of 60Hz − 180Hz. For a clean sounding subwoofer the filter should be at least a second-order filter to sharply roll off the high frequency audio signals.A higher order filter is recommended for stand-alone self-powered subwoofer applications. Figure 6 shows a simple input stage with a gain of 10 and a second-order low pass filter.
DS101277-77
FIGURE 6. Pre−amplifier Stage with Low Pass Filter
C=eoerA/d (Farads) (8)
where eo = 0.22479pF/in and er = 4.1
A is the common PCB area and d is the distance between the planes. The designer should target a value of 100pF or greater for both the positive supply to ground capacitance and negative supply to ground capacitance. Signal traces that cross over each other should be laid out at 90˚ to minimized any coupling.
Output Offset Voltage Minimization
The amount of DC offset voltage seen at the output with no input signal present is already quite good with the LM4651/
52. With no input signal present the system should be at 50% duty cycle.Any deviation from 50% duty cycle creates a DC offset voltage seen by the load. To completely eliminate the DC offset, a DC voltage divider can be used at the input to set the DC offset to near zero. This is accomplished by a simple resistor divider that applies a small DC voltage to the input. This forces the duty cycle to 50% when there is no input signal. The result is a LM4651 and LM4652 system with near zero DC offset. The divider should be a 1.8M from the +6V output (pin 6) to the input (other side of 25k, R
). R1acts like the second resistor in the divider. Also use
1
a 1µF input capacitor before R the source. R
and the 1µF capacitor create a high pass filter
1
with a 3dB point at 6.35Hz. The value of R
to block the DC voltage from
1
is set
OFFSET
according to the application. Variations in switching fre­quency and supply voltage will change the amount of offset voltage requiring a different value than stated above. The value above (1.8M)isfor
±
20V and a switching frequency
of 125kHz.
Supply Bypassing
Correct supply bypassing has two important goals. The first is to ensure that noise on the supply lines does not enter the circuit and become audible in the output. The second is to help stabilize an unregulated power supply and provide cur­rent under heavy current conditions. Because of the two different goals multiple capacitors of various types and val­ues are recommended for supply bypassing. For noise de-coupling, generally small ceramic capacitors (.001µF to .1µF) along with slightly larger tantalum or electrolytic ca­pacitors (1µF to 10µF) in parallel will do an adequate job of removing most noise from the supply rails. These capacitors should be placed as close as possible to each IC’s supply
www.national.com 12
Output Stage Filtering
As common with Class D amplifier design, there are many trade-offs associated with different circuit values. The output stage is not an exception. National has found good results with a 50µF inductor and a 5µF Mylar capacitor (see Figure 1, Typical Audio Application Circuit) used as the output LC filter. The two-pole filter contains three components; L and C output. The design formula for a bridge output filter is f 1/[2π(L
because the LM4651 and LM4652 have a bridged
BYP
1
)
2
12CBYP
].
C
A common mistake is to connect a large capacitor between ground and each output. This applies only to single-ended
1
=
Page 13
Application Information (Continued)
applications. In bridge operation, each output sees C This causes the extra factor of 2 in the formula. The alterna­tive to C V
, and V
O
size or cost efficient because each capacitor must be twice C
BYP
is a capacitor connected between each output,
BYP
, and ground. This alternative is, however, not
O
2
’s value to achieve the same filter cutoff frequency. The additional small value capacitors connected between each output and ground (C
) help filter the high frequency from the
1
output to ground . The recommended value for C 1µF or 2% to 20% of C
BYP
.’
Modulation Frequency Optimization
Setting the modulation frequency depends largely on the application requirements. To maximize efficiency and output power a lower modulation frequency should be used. The lower modulation frequency will lower the amount of loss caused by switching the output MOSFETs increasing the efficiency a few percent. A lower switching frequency will also increase the peak output power before clipping because the over modulation protection time is a smaller percentage of the total period. Unfortunately, the lower modulation fre­quency has worse THD+N performance when the output power is below 10 watts. The recommended switching fre­quency to balance the THD+N performance, efficiency and output power is 125kHz to 145kHz.
THD+N Measurements and Out of Audio Band Noise
THD+N (Total Harmonic Distortion plus Noise) is a very important parameter by which all audio amplifiers are mea­sured. Often it is shown as a graph where either the output power or frequency is changed over the operating range. A very important variable in the measurement of THD+N is the bandwidth limiting filter at the input of the test equipment.
Class D amplifiers, by design, switch their output power devices at a much higher frequency than the accepted audio range (20Hz - 20kHz). Switching the outputs makes the amplifier much more efficient than a traditional Class A/B amplifier. Switching the outputs at high frequency also in­creases the out-of-band noise. Under normal circumstances this out-of-band noise is significantly reduced by the output low pass filter. If the low pass filter is not optimized for a given switching frequency, there can be significant increase in out-of-band noise.
THD+N measurements can be significantly affected by out-of-band noise, resulting in a higher than expected THD+N measurement. To achieve a more accurate mea­surement of THD, the bandwidth at the input of the test equipment must be limited. Some common upper filter points are 22kHz, 30kHz, and 80kHz. The input filter limits the noise component of the THD+N measurement to a smaller bandwidth resulting in a more real-world THD+N value.
The output low pass filter does not remove all of the switch­ing fundamental and harmonics. If the switching frequency fundamental is in the measurement range of the test equip­ment, the THD+N measurement will include switching fre­quency energy not removed by the output filter.Whereas the switching frequency energy is not audible, it’s presence de­grades the THD+N measurement. Reducing the bandwidth to 30kHz and 22kHz reveals the true THD performance of
is 0.1µF to
1
BYP
LM4651 & LM4652
the Class D amplifier. Increasing the switching frequency or reducing the cutoff frequency of the output filter will also
.
reduce the level of the switching frequency fundamental and it’s harmonics present at the output. This is caused by a switching frequency that is higher than the output filter cutoff frequency and, therefore, more attenuation of the switching frequency.
In-band noise is higher in switching amplifiers than in linear amplifiers because of increased noise from the switching waveform. The majority of noise is out of band (as discussed above), but there is also an increase of audible noise. The output filter design (order and location of poles) has a large effect on the audible noise level. Power supply voltage also has an effect on noise level. The output filter removes a certain amount of the switching noise. As the supply in­creases, the attenuation by the output fiter is constant. How­ever, the switching waveform is now much larger resulting in higher noise levels.
THERMAL CONSIDERATIONS Heat Sinking
The choice of a heat sink for the output FETs in a Class D audio amplifier is made such that the die temperature does not exceed T
and activate the thermal protection cir-
JMAX
cuitry under normal operating conditions. The heat sink should be chosen to dissipate the maximum IC power which occurs at maximum output power for a given load. Knowing the maximum output power, the ambient temperature sur­rounding the device, the load and the switching frequency, the maximum power dissipation can be calculated. The ad­ditional parameters needed are the maximum junction tem­perature and the thermal resistance of the IC package (θ
JC
junction to case), both of which are provided in the Absolute Maximum Ratings and Operating Ratings sections above.
It should be noted that the idea behind dissipating the power within the IC is to provide the device with a low resistance to convection heat transfer such as a heat sink. Convection cooling heat sinks are available commercially and their manufacturers should be consulted for ratings. It is always safer to be conservative in thermal design.
Proper IC mounting is required to minimize the thermal drop between the package and the heat sink. The heat sink must also have enough metal under the package to conduct heat from the center of the package bottom to the fins without excessive temperature drop. A thermal grease such as Wakefield type 120 or Thermalloy Thermacote should be used when mounting the package to the heat sink. Without some thermal grease, the thermal resistance θ
CS
(case to sink) will be no better than 0.5˚C/W, and probably much worse. With the thermal grease, the thermal resistance will be 0.2˚C/W or less. It is important to properly torque the mounting screw. Over tightening the mounting screw will cause the package to warp and reduce the contact area with the heat sink. It can also crack the die and cause failure of the IC. The recommended maximum torque applied to the mounting screw is 40 inch-lbs. or 3.3 foot-lbs.
Determining Maximum Power Dissipation
Power dissipation within the integrated circuit package is a very important parameter. An incorrect maximum power dis­sipation (P
) calculation may result in inadequate heat sink-
D
ing, causing thermal shutdown circuitry to operate intermit­tently. There are two components of power dissipation in a class D amplifier. One component of power dissipation in the
,
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Page 14
Application Information (Continued)
LM4652 is the R current when operating at maximum output power.The other component of power dissipation in the LM4652 is the switch­ing loss. If the output power is high enough and the DC resistance of the filter coils is not minimized then significant loss can occur in the output filter. This will not affect the
LM4651 & LM4652
power dissipation in the LM4652 but should be checked to be sure that the filter coils with not over heat.
The first step in determining the maximum power dissipation is finding the maximum output power with a given voltage and load. Refer to the graph Output Power verses Supply Voltagetodetermine the output power for the given load and supply voltage. From this power, the RMS output current can be calculated as I dissipation caused by the output current is P (I
OUTRMS
2
)
*
(2*R found from the Electrical Characteristics for the LM4652 table above. The percentage of loss due to the switching is calculated by Equation (9):
%LOSS
SWITCH
t
and T
r,tf
OVERMOD
teristic for the LM4651 and Electrical Characteristic for the LM4652 sections above. The system designer deter-
mines the value for f pation caused by switching loss is found by Equation (10). P
OUTMAX
is the 1% output power for the given supply voltage
and the load impedance being used in the application. P
can be determined from the graph Output Power vs.
MAX
Supply Voltage in the Typical Performance Characteris­tics section above.
P
DSWITCH
(1−%LOSS
P
for the LM4652 is found by adding the two compo-
DMAX
nents (P
DSWITCH
Determining the Correct Heat Sink
Once the LM4652’s power dissipation known, the maximum thermal resistance (in ˚C/W) of a heat sink can be calculated. This calculation is made using Equation (11) and is based on the fact that thermal heat flow parameters are analogous to electrical current flow properties.
P
=(T
DMAX
JMAX−TAMBIENTMAX
Where θ
Since we know θJC, θCS, and T Maximum Ratings and Operating Ratings sections above (taking care to use the correct θ on which package type is being used in the application) and have calculated P the heat sink’s thermal resistance. The following equation is derived from Equation (11):
θ
= [(T
SA
JMAX−TAMBIENTMAX
of the FET times the RMS output
DS
(ON)
OUTRMS
= SQRT(P
). The value for R
DS
(ON)
=(tr+tf+T
OVERMOD
OUT/RL
)*f
SW
can be found in the Electrical Charac-
(switching frequency). Power dissi-
SW
= (%LOSS
+P
DOUT
SWITCH
) of power dissipation together.
*
SWITCH
P
OUTMAX
) (Watts) (10)
)/θJA(Watts) (11)
= θJC+ θCS+ θ
DMAX
JA
and T
JMAX
for the LM4652 depending
JC
AMBIENTMAX
SA
from the Absolute
, we only need θSA,
)/P
DMAX
). The power
DOUT
can be
DS
(ON)
(9)
OUT
)/
]−θJC− θ
CS
Again, it must be noted that the value of θSAis dependent upon the system designer’s application and its correspond­ing parameters as described previously. If the ambient tem­perature surrounding the audio amplifier is higher than T
AMBIENTMAX
, then the thermal resistance for the heat sink,
given all other parameters are equal, will need to be lower.
Example Design of a Class D Amplifier
The following is an example of how to design a class D amplifier system for a power subwoofer application utilizing the LM4651 and LM4652 to meet the design requirements listed below:
Output Power, 1% THD 125W
Load Impedance 4
=
Input Signal level 3V RMS (max)
Input Signal Bandwidth 10Hz − 150Hz
Ambient Temperature 50˚C (max)
Determine the Supply Voltage From the graph Output Power verses Supply voltage at
1% THD the supply voltage needed for a 125 watt, 4
application is found to be
Determine the Value for R
±
20V.
(Modulation Frequency)
OSC
The oscillation frequency is chosen to obtain a satisfactory efficiency level while also maintaining a reasonable THD
-
performance. The modulation frequency can be chosen us­ing the Clipping Power Point and Efficiency verses Switching Frequency graph. A modulation frequency of 125kHz is found to be a good middle ground for THD per­formance and efficiency.The value of the resistor for R
OSC
is
found from Equation (6) to be 3.9 k.
Determine the Value for R
(Circuit Limit)
SCKT
The current limit is internally set as a failsafe to 10 amps. The inductor ripple current and the peak output current must be lower than 10 amps or current limit protection will turn on. Atypical 4load driven by a filter using 50µH inductors does not require more than 10A. The current limit will have to be increased when loads less than 4are used to acheive higher output power. With R
equal to 100k, the current
SCKT
limit is 10A.
Determine the Value for R
(Dead Time Control)
DLY
The delay time or dead time is set to the recommended value so R is desired, R value for R
equals 5k. If a higher bandwidth of operation
DLY
should be a lower value resistor. If a zero
DLY
is desired, connect the LM4651’s pin 17 to
DLY
GND.
Determine the Value of L C
(the Output and Feedback Filters)
f
1,CBYP,C1,Rfl1Rfl2,Cfl1Cfl2,Rf
All component values show in
Figure 1
Typical Audio Ap-
,
plication Circuit, are optimized for a subwoofer application.
Use the following guidelines when changing any component values from those shown. The frequency response of the output filter is controlled by L
and C
1
. Refer to the Ap-
BYP
plication Information section titled Output Stage Filtering for a detailed explanation on calculating the correct values for L
and C
1
BYP
.
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Page 15
Application Information (Continued)
C
should be in the range of 0.1µF to 1µF or 2 - 20% of C
1
R
fl1
and R
are found by the ratio R
fl2
fl1
= 10R
fl2
Alower ratio can be used if the application is for lower output voltages than the 125Watt, 4solution show here.
The feedback RC filter’s pole location should be higher than the output filter pole. The reason for two capacitors in paral­lel instead of one larger capacitor is to reduce the possible EMI from the feedback traces. C
is placed close as pos-
fl1
sible to the output of the LM4652 so that an audio signal is present on the feedback trace instead of a high frequency square wave. C
is then placed as close as possible to the
fl2
feedback inputs (pins 14, 19) of the LM4651 to filter off any noise picked up by the feedback traces. The combination lowers EMI and provides a cleaner audio feedback signal to the LM4651. R
should be in range of 100kto1M.C
f
controls the bandwidth of the error signal and should be in the range of 100pF to 470pF.
BYP
.
LM4651 & LM4652
Equations (9) - (11) to calculate the amount of power dissi-
.
f
pation for the LM4652. The appropriate heat sink size, or thermal resistance in ˚C/W, will then be determined.
Equation (9) determines the percentage of loss caused by the switching. Use the typical values given in the Electrical
Characteristics for the LM4651 and Electrical Character­istics for the LM4652 tables for the rise time, fall time and
over modulation time:
*
%Loss = (25ns+26ns+350ns)
125kHz
%Loss = 5.0%
This switching loss causes a maximum power dissipation, using Equation (10), of:
P
DSWITCH
= (5.0%*125W) / (1−5.0%) P
DSWITCH
= 6.6W
Determine the Value for C
(Start Up Delay)
START
The start-up delay is chosen to be 1 second to ensure minimum pops or clicks when the amplifier is powered up. Using Equation (2), the value of C
is 11.7µF.Astandard
START
value of 10µF is used.
Determine the Value of Gain, R
, and R
1
2
The gain is set to produce a 125W output at no more than 1% distortion with a 3V 4load requires a 22.4V
input. A dissipation of 125W in a
RMS
signal. To produce this output
RMS
signal, the LM4651/LM4652 amplifier needs an overall closed-loop gain of 22.4V
RMS
/3V
, or 7.5V/V (17.5db).
RMS
Equation (12) shows all the variables that affect the system gain.
Gain = [(R
The values for R the Value of the Filters section above. Therefore, R 620k,R
fI2
also found as the first step in this example to be
2/R1
fI1,RfI2
) x ((R
fl1+Rfl2
, and Rfwere found in the Determine
)/ R
)−(R2/R1) + .5].(3)
fl2
fI1
= 62kand Rf= 390k. The value of VCCwas
±
20V. Inserting these values into equation (12) and reducing gives the equation below:
R
= .7R
2
1
The input resistance is desired to be 20kso R 20k.R
Lowering R ing R
is then found to be 14k.
2
direcly affects the noise of the system. Chang-
2
to increase gain with the lower value for R2has very
1
is set to
1
(4)
little affect on the noise level. The percent change in noise is about what whould be expected with a higher gain. The drawback to a lower R
value is a larger CINvalue, neces-
1
sary to properly couple the lowest desired signal frequen­cies. If a 20kinput impedance is not required, then the recommended values shown in Application Circuit should be used: with R
4.7kand R
’s value set to 3.5kfor a gain 7.5V/V.
2
Figure 1
, Typical Audio
’s value set to
1
Determine the Needed Heat Sink
The only remaining design requirement is a thermal design that prevents activating the thermal protection circuitry. Use
Next the power dissipation caused by the R
DS(ON)
of the output FETs is found by multiplying the output current times the R
. Again, the value for R
DS(ON)
is found from the
DS(ON)
Electrical Characteristics for the LM4652 table above. The value for R
at 100˚C is used since we are calcu-
DS(ON)
lating the maximum power dissipation.
I
OUTRMS
= SQRT(125watts/4) = 5.59 amps
2
P
RDS(ON)
= (5.59A)
P
RDS(ON)
*
(0.230*2)
= 14.4W
The total power dissipation in the LM4652 is the sum of these two power losses giving:
P
= 6.6W + 14.4W = 21W
DTOTAL
The value for Maximum Power Dissipation given in the Sys-
tem Electrical Characteristics for the LM4651 and
=
LM4652 is 22 watts. The difference is due to approximately 1 watt of power loss in the LM4651. The above calculations are for the power loss in the LM4652.
Lastly,use Equation (11) to determine the thermal resistance of the LM4652’s heat sink. The values for θ
JC
and T
JMAX
are found in the Operating Ratings and the Absolute Maxi- mum Ratings section above for the LM4652. The value of
θ
is 2˚C/W for the isolated (TF) package or 1˚C/W for the
JC
non-isolated (T) package. The value for T value for θ
is set to 0.2˚C/W since this is a reasonable
CS
is 150˚C. The
JMAX
value when thermal grease is used. The maximum ambient temperature from the design requirements is 50˚. The value of θ
for the isolated (TF) package is:
SA
θ
= [(150˚C − 50˚C)/21W] − 2˚C/W − 0.2˚C/W
SA
θ
= 2.5˚C/W
SA
and for the non-isolated (T) package without a mica washer to isolate the heat sink from the package:
θ
= [(150˚C − 50˚C)/21W] − 1˚C/W − 0.2˚C/W
SA
θ
= 3.5˚C/W
SA
www.national.com15
Page 16
Application Information (Continued)
To account for the use of a mica washer simply subtract the thermal resistance of the mica washer from θ
calculated
SA
above.
Recommendations for Critical External Components
LM4651 & LM4652
Circuit
Symbol
C
fI1
C
fI2
C
C
B2
C
B1&CBT
C
B3
C
1&CBYP
C
1&CBYP
D
L
L
L
f
1 1
1
1
Suggested
Value
Suggested Type Supplier/Contact Information
330pF Ceramic Disc 100pF Ceramic Disc 470pF Ceramic Disc
1µF Resin Dipped Solid Tantalum
0.1µF Monolithic Ceramic
0.001µF Monolithic Ceramic
5µF - 10µF Metalized Polypropylene or
Polyester Film
5µF - 10µF Metalized Polypropylene or
Polyester Film
3A, 50V Fast Schottky Diode
47µH, 5A High Saturation Open Core
(Vertical Mount Power Chokes)
50µH, 5.6A High Saturation Flux Density
Ferrite Rod
68µH, 7.3A High Saturation Flux Density
Ferrite Rod
Bishop Electronics Corp.
(562) 695 - 0446
http://www.bishopelectronics.com/
Nichicon Corp.
(847) 843-7500
http://www.nichicon-us.com/
CoilCraft
(847) 639-6400
http://www.coilcraft.com/
J.W. Miller
(310) 515-1720
http://www.jwmiller.com/
J.W. Miller
(310) 515-1720
http://www.jwmiller.com/
Supplier Part
#
BEC-9950 A11A-50V
QAF2Exx
or
QAS2Exx
PCV-0-
473-05
5504
5512
FIGURE 7. Reference PCB silkscreen layer
www.national.com 16
DS101277-29
Page 17
Application Information (Continued)
FIGURE 8. Reference PCB top layer
LM4651 & LM4652
DS101277-26
FIGURE 9. Reference PCB bottom layer
DS101277-27
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Page 18
Application Information (Continued)
LM4651 & LM4652
FIGURE 10. Reference PCB top layer solder mask
DS101277-28
FIGURE 11. Reference PCB bottom layer solder mask
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DS101277-78
Page 19
Physical Dimensions inches (millimeters) unless otherwise noted
Order Number LM4651N
NS Package Number N28B
LM4651 & LM4652
Order Number LM4652TF
NS Package Number TF15B
www.national.com19
Page 20
Notes
170W Class D Audio Power Amplifier Solution
LIFE SUPPORT POLICY
NATIONAL’S PRODUCTS ARE NOT AUTHORIZED FOR USE AS CRITICAL COMPONENTS IN LIFE SUPPORT DEVICES OR SYSTEMS WITHOUT THE EXPRESS WRITTEN APPROVAL OF THE PRESIDENT AND GENERAL COUNSEL OF NATIONAL SEMICONDUCTOR CORPORATION. As used herein:
LM4651 & LM4652 Overture
1. Life support devices or systems are devices or systems which, (a) are intended for surgical implant into the body, or (b) support or sustain life, and whose failure to perform when properly used in accordance with instructions for use provided in the labeling, can be reasonably expected to result in a significant injury to the user.
2. A critical component is any component of a life support device or system whose failure to perform can be reasonably expected to cause the failure of the life support device or system, or to affect its safety or effectiveness.
National Semiconductor Corporation
Americas Tel: 1-800-272-9959 Fax: 1-800-737-7018 Email: support@nsc.com
www.national.com
National does not assume any responsibility for use of any circuitry described, no circuit patent licenses are implied and National reserves the right at any time without notice to change said circuitry and specifications.
National Semiconductor Europe
Fax: +49 (0) 180-530 85 86
Email: europe.support@nsc.com Deutsch Tel: +49 (0) 69 9508 6208 English Tel: +44 (0) 870 24 0 2171 Français Tel: +33 (0) 1 41 91 8790
National Semiconductor Asia Pacific Customer Response Group
Tel: 65-2544466 Fax: 65-2504466 Email: ap.support@nsc.com
National Semiconductor Japan Ltd.
Tel: 81-3-5639-7560 Fax: 81-3-5639-7507
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