NSC LM4991LD

LM4991
3W Audio Power Amplifier with Shutdown Mode
General Description
Key Specifications
The LM4991 is a mono bridged audio power amplifier capable of delivering 3W of continuous average power into a
3Ω load with less than 10% THD when powered by a 5V
power supply (Note 1). To conserve power in portable applications, the LM4991’s micropower shutdown mode (ISD =
0.1µA, typ) is activated when VDD is applied to the SHUTDOWN pin.
n Improved PSRR at 217kHz and 1kHz
64dB (typ)
n PO at VDD = 5.0V, 10% THD, 1kHz
n
LM4991LD (only), 3Ω, 4Ω
3W (typ), 2.5W (typ)
n
All packages, 8Ω load
1.5W (typ)
n Shutdown current
0.1µA (typ)
Boomer audio power amplifiers are designed specifically to
provide high power, high fidelity audio output. They require
few external components and operate on low supply voltages from 2.2V to 5.5V. Since the LM4991 does not require
output coupling capacitors, bootstrap capacitors, or snubber
networks, it is ideally suited for low-power portable systems
that require minimum volume and weight.
Additional LM4991 features include thermal shutdown protection, unity-gain stability, and external gain set.
Note 1: An LM4991LD that has been properly mounted to a circuit board will
deliver 3W into 3Ω (at 10% THD). The other package options for the LM4991
will deliver 1.5W into 8Ω (at 10% THD). See the Application Information
sections for further information concerning the LM4991LD and LM4991M.
Features
Available in space-saving LLP and MA packages
Ultra low current shutdown mode
Can drive capacitive loads up to 500pF
Improved pop & click circuitry reduces noises during
turn-on and turn-off transitions
n 2.2 - 5.5V operation
n No output coupling capacitors, snubber networks,
bootstrap capacitors or gain-setting resistors required
n Unity-gain stable
n
n
n
n
Applications
n
n
n
n
Wireless and cellular handsets
PDA’s
Portable computers
Desktop computers
Connection Diagrams
Small Outline Package
LLP Package
20074002
Top View
Order Number LM4991MA
See NS Package Number M08A
20074039
Top View
Order Number LM4991LD
See NS Package Number LDC08A
Boomer ® is a registered trademark of National Semiconductor Corporation.
© 2003 National Semiconductor Corporation
DS200740
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LM4991 3W Audio Power Amplifier with Shutdown Mode
May 2003
LM4991
Typical Application
20074001
FIGURE 1. Typical Audio Amplifier Application Circuit
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2
Thermal Resistance
(Note 2)
If Military/Aerospace specified devices are required,
please contact the National Semiconductor Sales Office/
Distributors for availability and specifications.
Supply Voltage
6.0V
Supply Temperature
θJC (LD) (Note 9)
4.3˚C/W
θJA (LD)
56˚C/W
θJC (MA)
35˚C/W
θJA (MA)
140˚C/W
−65˚C to +150˚C
−0.3V to VDD to +0.3V
Input Voltage
Power Dissipation (Note 4)
Internally Limited
ESD Susceptibility (Note 5)
2000V
ESD Susceptibility (Note 6)
200V
Junction Temperature
Operating Ratings
Temperature Range
TMIN ≤ TA ≤ TMAX
−40˚C ≤ TA ≤ +85˚C
2.2V ≤ VDD ≤ 5.5V
Supply Voltage
150˚C
Electrical Characteristics VDD = 5V (Notes 2, 3)
The following specifications apply for VDD = 5V and RL = 8Ω unless otherwise specified. Limits apply for TA = 25˚C.
LM4991
Symbol
Parameter
Conditions
Typical
(Note 7)
Limit
(Note 8)
IDD
Quiescent Power Supply
Current
VIN = 0V, no Load
3
7
VIN = 0V, RL = 8Ω
4
10
ISD
Shutdown Current
VSHUTDOWN = VDD
0.1
2.0
VSDIH
Shutdown Voltage
mA (max)
µA (max)
1.5
VSDIL
VOS
Units
(Limits)
V
1.3
Output Offset Voltage
V
5
35
LM4991LD, RL = 3Ω (Note 10)
LM4991LD, RL = 4Ω (Note 10)
LM4991, RL = 8Ω
2.38
2.1
1.3
0.9
THD+N = 10%, f = 1kHz
LM4991LD, RL = 3Ω (Note 10)
LM4991LD, RL = 4Ω (Note 10)
LM4991, RL = 8Ω
3
2.5
1.5
mV (max)
THD = 1% (max), f = 1kHz
Po
THD+N
PSRR
Output Power
Total Harmonic
Distortion+Noise
Power Supply Rejection
Ratio
PO = 0.5W, f = 1kHz
VRIPPLE = 200mV sine p-p,
Input terminated with 10Ω,
f = 1kHz
W (min)
W
0.2
%
64
55
dB (min)
Electrical Characteristics VDD = 3V (Notes 2, 3)
The following specifications apply for VDD = 3V and RL = 8Ω unless otherwise specified. Limits apply for TA = 25˚C.
LM4991
Symbol
Parameter
Conditions
Typical
(Note 7)
Limit
(Note 8)
IDD
Quiescent Power Supply
Current
VIN = 0V, no Load
3
7
VIN = 0V, RL = 8Ω
4
7
VSHUTDOWN = VDD
0.1
2.0
ISD
Shutdown Current
VSDIH
Shutdown Voltage Input High
1.1
VSDIL
Shutdown Voltage Input Low
0.9
VOS
Output Offset Voltage
Po
Output Power
5
Total Harmonic
Distortion+Noise
mA (max)
µA (max)
V
V
35
mV (max)
THD = 1% (max), f = 1kHz
RL = 4Ω
RL = 8Ω
THD+N
Units
(Limits)
600
425
PO = 0.25W, f = 1kHz
3
0.1
mW
%
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LM4991
Absolute Maximum Ratings
LM4991
Electrical Characteristics VDD = 3V (Notes 2, 3)
The following specifications apply for VDD = 3V and RL = 8Ω unless otherwise specified. Limits apply for TA =
25˚C. (Continued)
LM4991
Symbol
PSRR
Parameter
Power Supply Rejection
Ratio
Conditions
VRIPPLE = 200mV sine p-p,
Input terminated with 10Ω,
f = 1kHz
Typical
(Note 7)
Limit
(Note 8)
Units
(Limits)
68
dB
Electrical Characteristics VDD = 2.6V (Notes 2, 3)
The following specifications apply for VDD = 2.6V and RL = 8Ω unless otherwise specified. Limits apply for TA = 25˚C.
LM4991
Symbol
Parameter
Conditions
Typical
(Note 7)
Limit
(Note 8)
Units
(Limits)
IDD
Quiescent Power Supply
Current
VIN = 0V, no Load
2
VIN = 0V, RL = 8Ω
3
ISD
Shutdown Current
VSHUTDOWN = VDD
0.1
µA(max)
VSDIH
Shutdown Voltage Input High
1
V
VSDIL
Shutdown Voltage Input Low
0.9
VOS
Output Offset Voltage
5
mA (max)
V
35
mV (max)
THD = 1% (max), f = 1kHz
Po
Output Power
THD+N
Total Harmonic
Distortion+Noise
PSRR
Power Supply Rejection
Ratio
400
300
RL = 4Ω
RL = 8Ω
PO = 0.15W, f = 1kHz
VRIPPLE = 200mV sine p-p,
Input terminated with 10Ω,
f = 1kHz
0.1
51
mW
%
dB
Note 2: 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 3: All voltages are measured with respect to the ground pin, unless otherwise specified.
Note 4: The maximum power dissipation must be derated at elevated temperatures and is dictated by TJMAX, θJA, and the ambient temperature TA. The maximum
allowable power dissipation is PDMAX = (TJMAX–TA)/θJA or the number given in Absolute Maximum Ratings, whichever is lower. For the LM4991, TJMAX = 150˚C.
For the θJA’s for different packages, please see the Application Information section or the Absolute Maximum Ratings section.
Note 5: Human body model, 100pF discharged through a 1.5kΩ resistor.
Note 6: Machine Model, 220pF–240pF discharged through all pins.
Note 7: Typicals are specified at 25˚C and represent the parametric norm.
Note 8: Limits are guaranteed to National’s AOQL (Average Outgoing Quality Level).
Note 9: The given θJA is for an LM4991 packaged in an LDC08A with the Exposed–DAP soldered to an exposed 1in2 area of 1oz printed circuit board copper.
Note 10: When driving 3Ω or 4Ω loads from a 5V supply, the LM4991LD must be mounted to a circuit board.
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LM4991
External Components Description
(Figure 1)
Components
Functional Description
1.
Ri
Inverting input resistance that sets the closed-loop gain in conjunction with Rf. This resistor also forms a high
pass filter with Ci at fC= 1/(2π RiCi).
2.
Ci
Input coupling capacitor that blocks the DC voltage at the amplifiers input terminals. Also creates a highpass
filter with Ri at fc = 1/(2π RiCi). Refer to the section, Proper Selection of External Components, for an
explanation of how to determine the value of Ci.
3.
Rf
Feedback resistance that sets the closed-loop gain in conjunction with Ri.
4.
CS
Supply bypass capacitor that provides power supply filtering. Refer to the Power Supply Bypassing section
for information concerning proper placement and selection of the supply bypass capacitor.
5.
CB
Bypass pin capacitor that provides half-supply filtering. Refer to the section, Proper Selection of External
Components, for information concerning proper placement and selection of CB.
Typical Performance Characteristics
LD and MH Specific Characteristics
THD+N vs Output Power
VDD = 5V, RL = 4Ω, and f = 1 kHz
THD+N vs Frequency
VDD = 5V, RL = 4Ω, and PO = 1W
20074041
20074042
Typical Performance Characteristics
THD+N vs Frequency
VDD = 3V, RL = 4Ω, and PO = 500mW
THD+N vs Frequency
VDD = 5V, RL = 8Ω, and PO = 500mW
20074043
20074044
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LM4991
Typical Performance Characteristics
(Continued)
THD+N vs Frequency
VDD = 3V, RL = 8Ω, and PO = 250mW
THD+N vs Frequency
VDD = 2.6V, RL = 4Ω, and PO = 150mW
20074045
20074046
THD+N vs Output Power
VDD = 5V, RL = 8Ω, and f = 1kHz
THD+N vs Frequency
VDD = 2.6V, RL = 8Ω, and PO = 150mW
20074047
20074048
THD+N vs Output Power
VDD = 3V, RL = 8Ω, and f = 1kHz
THD+N vs Output Power
VDD = 3V, RL = 4Ω, and f = 1kHz
20074049
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20074050
6
LM4991
Typical Performance Characteristics
(Continued)
THD+N vs Output Power
VDD = 2.6V, RL = 4Ω, and f = 1kHz
THD+N vs Output Power
VDD = 2.6V, RL = 8Ω, and f = 1kHz
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20074052
Power Supply Rejection Ratio (PSRR) vs Frequency
VDD = 5V, RL = 8Ω, input floating
Power Supply Rejection Ratio (PSRR) vs Frequency
VDD = 5V, RL = 8Ω, input 10Ω terminated
20074053
20074054
Power Supply Rejection Ratio (PSRR) vs Frequency
VDD = 3V, RL = 8Ω, input floating
Power Supply Rejection Ratio (PSRR) vs Frequency
VDD = 3V, RL = 8Ω, input 10Ω terminated
20074055
20074056
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LM4991
Typical Performance Characteristics
(Continued)
Power Supply Rejection Ratio (PSRR) vs Frequency
VDD = 2.6V, RL = 8Ω, input 10Ω terminated
Power Supply Rejection Ratio (PSRR) vs Frequency
VDD = 2.6V, RL = 8Ω, Input Floating
20074057
20074058
Noise Floor, 5V, 8Ω
80kHz Bandwidth, Input to GND
Open Loop Frequency Response, 5V
20074059
20074060
Power Dissipation vs
Output Power, VDD = 3V
Power Dissipation vs
Output Power, VDD = 5V
20074061
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20074062
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LM4991
Typical Performance Characteristics
(Continued)
Power Dissipation vs
Output Power, VDD = 2.6V
Shutdown Hysteresis Voltage
VDD = 5V, SD Mode = VDD
20074072
20074063
Shutdown Hysteresis Voltage
VDD = 3V, SD Mode = VDD
Shutdown Hysteresis Voltage
VDD = 2.6V, SD Mode = VDD
20074073
20074074
Output Power vs
Supply Voltage, RL = 8Ω
Output Power vs
Supply Voltage, RL = 4Ω
20074067
20074068
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LM4991
Typical Performance Characteristics
(Continued)
Output Power vs
Supply Voltage, RL = 16Ω
Output Power vs
Supply Voltage, RL = 32Ω
20074069
20074070
Frequency Response vs
Input Capacitor Size
20074071
two-sided PCB, or on an inner layer of a board with more
than two layers. Connect the DAP copper pad to the inner
layer or backside copper heat sink area with 4(2x2) vias. The
via diameter should be 0.012in-0.013in with a 1.27mm pitch.
Ensure efficient thermal conductivity by plating through the
vias.
Best thermal performance is achieved with the largest practical heat sink area. If the heatsink and amplifier share the
same PCB layer, a nominal 2.5in2 area is necessary for 5V
operation with a 4Ω load. Heatsink areas not placed on the
same PCB layer as the LM4991 should be 5in2 (min) for the
same supply voltage and load resistance. The last two area
recommendations apply for 25˚C ambient temperature. Increase the area to compensate for ambient temperatures
above 25˚C. The LM4991’s power de-rating curve in the
Typical Performance Characteristics shows the maximum
power dissipation versus temperature. An example PCB layout for the LD package is shown in the Demonstration
Board Layout section. Further detailed and specific information concerning PCB layout, fabrication, and mounting an
Application Information
EXPOSED-DAP PACKAGE PCB MOUNTING
CONSIDERATION
The LM4991’s exposed-DAP (die attach paddle) package
(LD) provides a low thermal resistance between the die and
the PCB to which the part is mounted and soldered. This
allows rapid heat transfer from the die to the surrounding
PCB copper traces, ground plane, and surrounding air. The
result is a low voltage audio power amplifier that produces
2W at ≤ 1% THD with a 4Ω load. This high power is achieved
through careful consideration of necessary thermal design.
Failing to optimize thermal design may compromise the
LM4991’s high power performance and activate unwanted,
though necessary, thermal shutdown protection.
The LD package must have its DAP soldered to a copper
pad on the PCB. The DAP’s PCB copper pad is connected to
a large plane of continuous unbroken copper. This plane
forms a thermal mass, heat sink, and radiation area. Place
the heat sink area on either outside plane in the case of a
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amplifier’s half-supply bias voltage across the load. The
current flow created by the half-supply bias voltage increases internal IC power dissipation and my permanently
damage loads such as speakers.
(Continued)
LD (LLP) package is available from National Semiconductor’s Package Engineering Group under application note
AN1187.
POWER DISSIPATION
Power dissipation is a major concern when designing a
successful amplifier, whether the amplifier is bridged or
single-ended. A direct consequence of the increased power
delivered to the load by a bridge amplifier is an increase in
internal power dissipation. Equation 1 states the maximum
power dissipation point for a bridge amplifier operating at a
given supply voltage and driving a specified output load.
PCB LAYOUT AND SUPPLY REGULATION
CONSIDERATIONS FOR DRIVING 3Ω AND 4Ω LOADS
Power dissipated by a load is a function of the voltage swing
across the load and the load’s impedance. As load impedance decreases, load dissipation becomes increasingly dependant on the interconnect (PCB trace and wire) resistance
between the amplifier output pins and the load’s connections. Residual trace resistance causes a voltage drop,
which results in power dissipated in the trace and not in the
load as desired. For example, 0.1Ω trace resistance reduces
the output power dissipated by a 4Ω load from 2.0W to
1.95W. This problem of decreased load dissipation is exacerbated as load impedance decreases. Therefore, to maintain the highest load dissipation and widest output voltage
swing, PCB traces that connect the output pins to a load
must be as wide as possible.
Poor power supply regulation adversely affects maximum
output power. A poorly regulated supply’s output voltage
decreases with increasing load current. Reduced supply
voltage causes decreased headroom, output signal clipping,
and reduced output power. Even with tightly regulated supplies, trace resistance creates the same effects as poor
supply regulation. Therefore, making the power supply
traces as wide as possible helps maintain full output voltage
swing.
PDMAX = 4*(VDD)2/(2π2RL)
(1)
Since the LM4991 has two operational amplifiers in one
package, the maximum internal power dissipation is 4 times
that of a single-ended ampifier. Even with this substantial
increase in power dissipation, the LM4991 does not require
heatsinking under most operating conditions and output
loading. From Equation 1, assuming a 5V power supply and
an 8Ω load, the maximum power dissipation point is
625 mW. The maximum power dissipation point obtained
from Equation 1 must not be greater than the power dissipation that results from Equation 2:
(2)
PDMAX = (TJMAX–TA)/θJA
For the SO package, θJA = 140˚C/W. For the LD package
soldered to a DAP pad that expands to a copper area of
1.0in2 on a PCB, the LM4991’s θJA is 56˚C/W. TJMAX =
150˚C for the LM4991. The θJA can be decreased by using
some form of heat sinking. The resultant θJA will be the
summation of the θJC, θCS, and θSA. θJC is the junction to
case of the package (or to the exposed DAP, as is the case
with the LD package), θCS is the case to heat sink thermal
resistance and θSA is the heat sink to ambient thermal
resistance. By adding additional copper area around the
LM4991, the θJA can be reduced from its free air value for
the SO package. Increasing the copper area around the LD
package from 1.0in2 to 2.0in2 area results in a θJA decrease
to 46˚C/W. Depending on the ambient temperature, TA, and
the θJA, Equation 2 can be used to find the maximum internal
power dissipation supported by the IC packaging. If the
result of Equation 1 is greater than that of Equation 2, then
either the supply voltage must be decreased, the load impedance increased, the θJA decreased, or the ambient temperature reduced. For the typical application of a 5V power
supply, with an 8Ω load, and no additional heatsinking, the
maximum ambient temperature possible without violating the
maximum junction temperature is approximately 61˚C provided that device operation is around the maximum power
dissipation point and assuming surface mount packaging.
For the LD package in a typical application of a 5V power
supply, with a 4Ω load, and 1.0in2 copper area soldered to
the exposed DAP pad, the maximum ambient temperature is
approximately 77˚C providing device operation is around the
maximum power dissipation point. Internal power dissipation
is a function of output power. If typical operation is not
around the maximum power dissipation point, the ambient
temperature can be increased. Refer to the Typical Performance Characteristics curves for power dissipation information for different output powers and output loading.
BRIDGE CONFIGURATION EXPLANATION
As shown in Figure 1, the LM4991 has two operational
amplifiers internally, allowing for a few different amplifier
configurations. The first amplifier’s gain is externally configurable; the second amplifier is internally fixed in a unity-gain,
inverting configuration. The closed-loop gain of the first amplifier is set by selecting the ratio of Rf to Ri while the second
amplifier’s gain is fixed. Figure 1 shows that the output of
amplifier one serves as the input to amplifier two, which
results in both amplifiers producing signals identical in magnitude, but 180˚ out of phase. Consequently, the differential
gain for the IC is
AVD= 2 *(Rf/Ri)
By driving the load differentially through outputs Vo1 and
Vo2, an amplifier configuration commonly referred to as
“bridged mode” is established. Bridged mode operation is
different from the classical single-ended amplifier configuration where one side of its load is connected to ground.
A bridge amplifier design has a few distinct advantages over
the single-ended configuration, as it provides differential
drive to the load, thus doubling output swing for a specified
supply voltage. Four times the output power is possible as
compared to a single-ended amplifier under the same conditions. This increase in attainable output power assumes
that the amplifier is not current limited or clipped. In order to
choose an amplifier’s closed-loop gain without causing excessive clipping, please refer to the Audio Power Amplifier
Design section.
Another advantage of the differential bridge output is no net
DC voltage across load. This results from biasing VO1 and
VO2 at the same DC voltage, in this case VDD/2 . This
eliminates the coupling capacitor that single supply, singleended amplifiers require. Eliminating an output coupling capacitor in a single-ended configuration forces a single supply
POWER SUPPLY BYPASSING
As with any amplifier, proper supply bypassing is critical for
low noise performance and high power supply rejection. The
capacitor location on both the bypass and power supply pins
should be as close to the LM4991 as possible. The capacitor
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LM4991
Application Information
LM4991
Application Information
Selection Of Input Capacitor Size
(Continued)
Large input capacitors are both expensive and space hungry
for portable designs. Clearly, a certain sized capacitor is
needed to couple in low frequencies without severe attenuation. But in many cases the speakers used in portable
systems, whether internal or external, have little ability to
reproduce signals below 100Hz to 150Hz. Thus, using a
large input capacitor may not increase actual system performance.
connected between the bypass pin and ground improves the
internal bias voltage’s stability, producing improved PSRR.
The improvements to PSRR increase as the bypass pin
capacitor increases. Typical applications employ a 5V regulator with 10µF and a 0.1µF bypass capacitors which aid in
supply stability. This does not eliminate the need for bypassing the supply nodes of the LM4991 with a 1µF tantalum
capacitor. The selection of bypass capacitors, especially CB,
is dependent upon PSRR requirements, click and pop performance as explained in the section, Proper Selection of
External Components, system cost, and size constraints.
In addition to system cost and size, click and pop performance is effected by the size of the input coupling capacitor,
Ci. A larger input coupling capacitor requires more charge to
reach its quiescent DC voltage (nominally 1/2 VDD). This
charge comes from the output via the feedback and is apt to
create pops upon device enable. Thus, by minimizing the
capacitor size based on necessary low frequency response,
turn-on pops can be minimized.
Besides minimizing the input capacitor size, careful consideration should be paid to the bypass capacitor value. Bypass
capacitor, CB, is the most critical component to minimize
turn-on pops since it determines how fast the LM4991 turns
on. The slower the LM4991’s outputs ramp to their quiescent
DC voltage (nominally 1/2 VDD), the smaller the turn-on pop.
Choosing CB equal to 1.0µF along with a small value of Ci (in
the range of 0.1µF to 0.39µF), should produce a virtually
clickless and popless shutdown function. While the device
will function properly, (no oscillations or motorboating), with
CB equal to 0.1µF, the device will be much more susceptible
to turn-on clicks and pops. Thus, a value of CB equal to
1.0µF is recommended in all but the most cost sensitive
designs.
SHUTDOWN FUNCTION
In order to reduce power consumption while not in use, the
LM4991 contains a shutdown pin to externally turn off the
amplifier’s bias circuitry. This shutdown feature turns the
amplifier off when a logic high is placed on the shutdown pin.
The trigger point between a logic low and logic high level is
typically half- supply. It is best to switch between ground and
supply to provide maximum device performance. By switching the shutdown pin to VDD, the LM4991 supply current
draw will be minimized in idle mode. While the device will be
disabled with shutdown pin voltages less then VDD, the idle
current may be greater than the typical value of 0.1µA. In
either case, the shutdown pin should be tied to a definite
voltage to avoid unwanted state changes.
In many applications, a microcontroller or microprocessor
output is used to control the shutdown circuitry which provides a quick, smooth transition into shutdown. Another solution is to use a single-pole, single-throw switch in conjunction with an external pull-up resistor. When the switch is
closed, the shutdown pin is connected to ground and enables the amplifier. If the switch is open, then the external
pull-up resistor will disable the LM4991. This scheme guarantees that the shutdown pin will not float thus preventing
unwanted state changes.
AUDIO POWER AMPLIFIER DESIGN
Design a 1W/8Ω Audio Amplifier
Given:
Power Output
Load Impedance
PROPER SELECTION OF EXTERNAL COMPONENTS
Proper selection of external components in applications using integrated power amplifiers is critical to optimize device
and system performance. While the LM4991 is tolerant of
external component combinations, consideration to component values must be used to maximize overall system quality.
The LM4991 is unity-gain stable which gives a designer
maximum system flexibility. The LM4991 should be used in
low gain configurations to minimize THD+N values, and
maximize the signal to noise ratio. Low gain configurations
require large input signals to obtain a given output power.
Input signals equal to or greater than 1 Vrms are available
from sources such as audio codecs. Please refer to the
section, Audio Power Amplifier Design, for a more complete explanation of proper gain selection.
Besides gain, one of the major considerations is the closedloop bandwidth of the amplifier. To a large extent, the bandwidth is dictated by the choice of external components
shown in Figure 1. The input coupling capacitor, Ci, forms a
first order high pass filter which limits low frequency response. This value should be chosen based on needed
frequency response for a few distinct reasons.
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Input Level
Input Impedance
Bandwidth
1 Wrms
8Ω
1 Vrms
20 kΩ
100 Hz–20 kHz ± 0.25 dB
A designer must first determine the minimum supply rail to
obtain the specified output power. By extrapolating from the
Output Power vs Supply Voltage graphs in the Typical Performance Characteristics section, the supply rail can be
easily found. A second way to determine the minimum supply rail is to calculate the required Vopeak using Equation 3
and add the output voltage. Using this method, the minimum
supply voltage would be (Vopeak + (VODTOP + VODBOT)), where
VODBOT and VODTOP are extrapolated from the Dropout Voltage vs Supply Voltage curve in the Typical Performance
Characteristics section.
(3)
Using the Output Power vs Supply Voltage graph for an 8Ω
load, the minimum supply rail is 4.6V. But since 5V is a
standard voltage in most applications, it is chosen for the
supply rail. Extra supply voltage creates headroom that allows the LM4991 to reproduce peaks in excess of 1W without producing audible distortion. At this time, the designer
12
stated as a pair of −3dB frequency points. Five times away
from a −3dB point is 0.17dB down from passband response
which is better than the required ± 0.25dB specified.
(Continued)
must make sure that the power supply choice along with the
output impedance does not violate the conditions explained
in the Power Dissipation section.
Once the power dissipation equations have been addressed,
the required differential gain can be determined from Equation 4.
fL = 100Hz/5 = 20Hz
fH = 20kHz * 5 = 100kHz
As stated in the External Components section, Ri in conjunction with Ci create a highpass filter.
Ci ≥ 1/(2π*20kΩ*20Hz) = 0.397µF; use 0.39µF
The high frequency pole is determined by the product of the
desired frequency pole, fH, and the differential gain, AVD.
With a AVD = 3 and fH = 100kHz, the resulting GBWP =
150kHz which is much smaller than the LM4991 GBWP of
4MHz. This figure displays that if a designer has a need to
design an amplifier with a higher differential gain, the
LM4991 can still be used without running into bandwidth
limitations.
(4)
(5)
Rf/Ri = AVD/2
From Equation 4, the minimum AVD is 2.83; use AVD = 3.
Since the desired input impedance was 20kΩ, and with a
AVD impedance of 2, a ratio of 1.5:1 of Rf to Ri results in an
allocation of Ri = 20kΩ and Rf = 30kΩ. The final design step
is to address the bandwidth requirements which must be
13
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LM4991
Application Information
LM4991
Physical Dimensions
inches (millimeters) unless otherwise noted
Order Number LM4991LD
See NS Package Number LDC08A
Order Number LM4991MA
NS Package Number M08A
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14
LM4991 3W Audio Power Amplifier with Shutdown Mode
Notes
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