The LM4940 is a dual audio power amplifier primarily designed for demanding applications in flat panel monitors and
TV’s. It is capable of delivering 6 watts per channel to a 4Ω
load with less than 10% THD+N while operating on a
14.4V
Boomer audio power amplifiers were designed specifically to
provide high quality output power with a minimal amount of
external components. The LM4940 does not require bootstrap capacitors or snubber circuits. Therefore, it is ideally
suited for display applications requiring high power and minimal size.
The LM4940 features a low-power consumption active-low
shutdown mode. Additionally, the LM4940 features an internal thermal shutdown protection mechanism along with short
circuit protection.
The LM4940 contains advanced pop & click circuitry that
eliminates noises which would otherwise occur during
turn-on and turn-off transitions.
The LM4940 is a unity-gain stable and can be configured by
external gain-setting resistors.
power supply.
DC
Typical Application
Key Specifications
j
Quiscent Power Supply Current40mA (max)
j
P
(SE)
OUT
V
= 14.4V, RL=4Ω, 10% THD+N6W (typ)
DD
j
Shutdown current40µA (typ)
Features
n Pop & click circuitry eliminates noise during turn-on and
turn-off transitions
n Low current, active-low shutdown mode
n Low quiescent current
n Stereo 6W output, R
n Short circuit protection
n Unity-gain stable
n External gain configuration capability
L
=4Ω
Applications
n Flat Panel Monitors
n Flat Panel TV’s
n Computer Sound Cards
If Military/Aerospace specified devices are required,
please contact the National Semiconductor Sales Office/
Distributors for availability and specifications.
Supply Voltage (pin 6, referenced
to GND, pins 4 and 5)18.0V
ESD Susceptibility (Note 5)200V
Junction Temperature150˚C
Thermal Resistance
θ
(TS)4˚C/W
JC
θ
(TS) (Note 3)20˚C/W
JA
θ
(TA)4˚C/W
JC
θ
(TA) (Note 3)20˚C/W
JA
Storage Temperature−65˚C to +150˚C
Input Voltage
pins 3 and 7−0.3V to V
DD
+ 0.3V
pins 1, 2, 8, and 9−0.3V to 9.5V
Power Dissipation (Note 3)Internally limited
ESD Susceptibility (Note 4)2000V
Operating Ratings
Temperature Range
T
≤ TA≤ T
MIN
MAX
Supply Voltage10V ≤ V
−40˚C ≤ TA≤ 85˚C
DD
≤ 16V
Electrical Characteristics VDD= 12V (Notes 1, 2)
The following specifications apply for VDD= 12V, AV= 10, RL=4Ω, f = 1kHz unless otherwise specified. Limits apply for TA=
25˚C.
SymbolParameterConditionsLM4940Units
Typical
(Note 6)
I
DD
I
SD
V
SDIH
V
SDIL
Quiescent Power Supply CurrentVIN= 0V, IO= 0A, No Load1640mA (max)
Shutdown CurrentV
SHUTDOWN
= GND (Note 9)40100µA (max)
Shutdown Voltage Input High2.0
Shutdown Voltage Input Low0.4V (max)
Limit
(Notes 7, 8)
V
DD
Single Channel
P
O
Output Power
THD+NTotal Harmomic Distortion + NoiseP
e
OS
X
TALK
Output NoiseA-Weighted Filter, VIN= 0V,
Channel SeparationPO=1W70dB
PSRRPower Supply Rejection RatioV
Note 1: All voltages are measured with respect to the GND pin, unless otherwise specified.
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 andAC 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: The maximum power dissipation must be derated at elevated temperatures and is dictated by T
allowable power dissipation is P
in Figure 1) with V
heatsink surface area.
Note 4: Human body model, 100pF discharged through a 1.5 kΩ resistor.
Note 5: Machine Model, 220pF– 240pF discharged through all pins.
Note 6: Typicals are measured at 25˚C and represent the parametric norm.
Note 7: Limits are guaranteed to National’s AOQL (Average Outgoing Quality Level).
Note 8: Datasheet min/max specification limits are guaranteed by design, test, or statistical analysis.
Note 9: Shutdown current is measured in a normal room environment. The Shutdown pin should be driven as close as possible to GND for minimum shutdown
current.
= 12V, RL=4Ω stereo operation the total power dissipation is 3.65W. θJA= 20˚C/W for both TO263 and TO220 packages mounted to 16in
DD
DMAX
=(T
)/θJAor the given inAbsolute Maximum Ratings, whichever is lower. For the LM4940 typical application (shown
JMAX−TA
THD+N = 1%3.12.8
THD+N = 10%4.2
V
= 14.4V, THD+N = 10%6.0
DD
= 1Wrms, AV= 10, f = 1kHz0.15%
O
Input Referred
= 200mV
RIPPLE
1kHz
p-p,fRIPPLE
=
, θJA, and the ambient temperature, TA. The maximum
External Components Description Refer to (Figure 1.)
ComponentsFunctional Description
This is the inverting input resistance that, along with RF, sets the closed-loop gain. Input
1.R
2.C
3.R
4.C
5.C
BYPASS
6.C
resistance R
IN
=1/(2πRINCIN).
This is the input coupling capacitor. It blocks DC voltage at the amplifier’s inverting input. CINand
IN
IN
create a highpass filter. The filter’s cutoff frequency is fC=1/(2πRINCIN). Refer to the
R
SELECTING EXTERNAL COMPONENTS section for an explanation of determining C
This is the feedback resistance that, along with Ri, sets closed-loop gain.
F
The supply bypass capacitor. Refer to the POWER SUPPLY BYPASSING section for information
S
about properly placing, and selecting the value of, this capacitor.
This capacitor filters the half-supply voltage present on the BYPASS pin. Refer to the Application
section, SELECTING EXTERNAL COMPONENTS, for information about properly placing, and
selecting the value of, this capacitor.
This is the output coupling capacitor. It blocks the nominal VDD/2 voltage present at the output
OUT
and prevents it from reaching the load. C
frequency is f
for an explanation of determining C
and input capacitance CINform a high pass filter. The filter’s cutoff frequency is f
IN
and RLform a high pass filter whose cutoff
OUT
=1/(2πRLC
C
). Refer to the SELECTING EXTERNAL COMPONENTS section
OUT
’s value.
OUT
20075672
’s value.
IN
C
www.national.com4
Typical Performance Characteristics
THD+N vs FrequencyTHD+N vs Frequency
LM4940
VDD= 12V, RL=4Ω, SE operation,
20075699
both channels driven and loaded (average shown),
= 1W, AV=1
P
OUT
THD+N vs FrequencyTHD+N vs Output Power
VDD= 12V, RL=8Ω, SE operation,
200756A1
both channels driven and loaded (average shown),
= 1W, AV=1
P
OUT
THD+N vs Output PowerTHD+N vs Output Power
VDD= 12V, RL=4Ω, SE operation,
200756A0
both channels driven and loaded (average shown),
= 2.5W, AV=1
P
OUT
200756F3
VDD= 14.4V, RL=4Ω, SE operation, AV=1
single channel driven/single channel measured,
= 1kHz
f
IN
VDD= 12V, RL=4Ω, SE operation, AV=1
200756D9
single channel driven/single channel measured,
= 1kHz
f
IN
VDD= 12V, RL=8Ω, SE operation, AV=1
200756E0
single channel driven/single channel measured,
= 1kHz
f
IN
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Typical Performance Characteristics (Continued)
LM4940
THD+N vs Output PowerTHD+N vs Output Power
VDD= 12V, RL=16Ω, SE operation, AV=1
200756E1
single channel driven/single channel measured,
= 1kHz
f
IN
THD+N vs Output PowerTHD+N vs Output Power
VDD= 12V, RL=4Ω, SE operation, AV=10
200756C7
single channel driven/single channel measured,
= 1kHz
f
IN
VDD= 12V, RL=8Ω, SE operation, AV=10
single channel driven/single channel measured,
= 1kHz
f
IN
200756C6
VDD= 12V, RL=16Ω, SE operation, AV=10
single channel driven/single channel measured,
= 1kHz
f
IN
Output Power vs Power Supply VoltageOutput Power vs Power Supply Voltage
RL=4Ω, SE operation,
both channels driven and loaded (average shown),
at (from top to bottom at 12V): THD+N = 10%,
THD+N = 1%
200756E8
RL=8Ω, SE operation, fIN= 1kHz,
both channels driven and loaded (average shown),
at (from top to bottom at 12V): THD+N = 10%,
THD+N = 1%
20075666
200756E9
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Typical Performance Characteristics (Continued)
Output Power vs Power Supply VoltagePower Supply Rejection vs Frequency
LM4940
RL=8Ω, SE operation, fIN= 1kHz,
20075667
both channels driven and loaded (average shown),
at (from top to bottom at 12V): THD+N = 10%,
THD+N = 1%
Power Supply Rejection vs FrequencyTotal Power Dissipation vs Load Dissipation
VDD= 12V, RL=8Ω, SE operation, V
= 10, at (from top to bottom at 60Hz):
A
V
C
BYPASS
= 1µF, C
BYPASS
= 4.7µF, C
RIPPLE
BYPASS
200756D8
= 200mV
= 10µF
Output Power vs Load ResistanceChannel-to-Channel Crosstalk vs Frequency
p-p
VDD= 12V, RL=8Ω, SE operation,
200756B8
V
,
= 200mV
RIPPLE
C
BYPASS
= 1µF, C
VDD= 12V, SE operation, fIN= 1kHz,
at (from top to bottom at 1W):
, at (from top to bottom at 60Hz):
p-p
BYPASS
R
= 4.7µF, C
=4Ω,RL=8Ω
L
BYPASS
20075681
= 10µF,
VDD= 12V, SE operation, fIN= 1kHz,
20075691
both channels driven and loaded,
at (from top to bottom at 15Ω):
THD+N = 10%, THD+N = 1%
VDD= 12V, RL=4Ω,P
= 1W, SE operation,
OUT
at (from top to bottom at 1kHz): V
V
OUTA
measured; V
INA
driven, V
OUTB
20075698
driven,
INB
measured
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Typical Performance Characteristics (Continued)
LM4940
Channel-to-Channel Crosstalk vs FrequencyPower Supply Current vs Power Supply Voltage
200756F0
=50Ω
VDD= 12V, RL=8Ω,P
= 1W, SE operation,
OUT
at (from top to bottom at 1kHz): V
V
OUTA
measured; V
driven, V
INA
OUTB
200756A3
driven,
INB
measured
RL=4Ω, SE operation
= 0V, R
V
IN
SOURCE
Clipping Voltage vs Power Supply VoltageClipping Voltage vs Power Supply Voltage
RL=4Ω, SE operation, fIN= 1kHz
200756F1
both channels driven and loaded,
at (from top to bottom at 13V):
negative signal swing, positive signal swing
Power Dissipation vs Ambient Temperature
VDD= 12V, RL=8Ω (SE), fIN= 1kHz,
(from top to bottom at 120˚C): 16in
heatsink area,
2
copper plane heatsink area
8in
200756E4
2
copper plane
RL=8Ω, SE operation, fIN= 1kHz
200756F2
both channels driven and loaded, at (from top to bottom
amplifiers, the LM4940 is designed to operate over a power supply voltages range of 10V
to 15V. Operating on a 12V power supply, the LM4940 will
deliver 3.1W per channel into 4Ω loads with no more than
1% THD+N.
POWER DISSIPATION
Power dissipation is a major concern when designing a
successful single-ended amplifier. Equation (2) states the
maximum power dissipation point for a single-ended amplifier operating at a given supply voltage and driving a specified output load.
P
DMAX-SE
=(VDD)2/ (2π2RL): Single Ended(1)
The LM4940’s dissipation is twice the value given by Equation (2) when driving two SE loads. For a 12V supply and two
8Ω SE loads, the LM4940’s dissipation is 1.82W.
The maximum power dissipation point (twice the value given
by Equation (2)) must not exceed the power dissipation
given by Equation (4):
’=(T
P
DMAX
The LM4940’s T
LM4940’s θ
is 20˚C/W when the metal tab is soldered to a
JA
= 150˚C. In the TS package, the
JMAX
copper plane of at least 16in
JMAX-TA
2
) / θ
JA
(2)
. This plane can be split be-
tween the top and bottom layers of a two-sided PCB. Con-
20075672
nect the two layers together under the tab with a 5x5 array of
vias. For the TA package, use an external heatsink with a
thermal impedance that is less than 20˚C/W. At any given
ambient temperature T
, use Equation (4) to find the maxi-
A
mum internal power dissipation supported by the IC packaging. Rearranging Equation (4) and substituting P
’ results in Equation (5). This equation gives the maxi-
P
DMAX
DMAX
for
mum ambient temperature that still allows maximum stereo
power dissipation without violating the LM4940’s maximum
junction temperature.
T
A=TJMAX-PDMAX-SEθJA
(3)
For a typical application with a 12V power supply and two 4Ω
SE loads, the maximum ambient temperature that allows
maximum stereo power dissipation without exceeding the
maximum junction temperature is approximately 113˚C for
the TS package.
T
JMAX=PDMAX-SEθJA+TA
(4)
Equation (6) gives the maximum junction temperature
. If the result violates the LM4940’s 150˚C, reduce the
T
JMAX
maximum junction temperature by reducing the power supply voltage or increasing the load resistance. Further allowance should be made for increased ambient temperatures.
The above examples assume that a device is operating
around the maximum power dissipation point. Since internal
power dissipation is a function of output power, higher ambient temperatures are allowed as output power or duty
cycle decreases.
www.national.com9
Application Information (Continued)
If the result of Equation (3) is greater than that of Equation
LM4940
(4), then decrease the supply voltage, increase the load
impedance, or reduce the ambient temperature. Further,
ensure that speakers rated at a nominal 4Ω do not fall below
3Ω. If these measures are insufficient, a heat sink can be
added to reduce θ
additional copper area around the package, with connections to the ground pins, supply pin and amplifier output pins.
Refer to the Typical Performance Characteristics curves
for power dissipation information at lower output power levels.
POWER SUPPLY VOLTAGE LIMITS
Continuous proper operation is ensured by never exceeding
the voltage applied to any pin, with respect to ground, as
listed in the Absolute Maximum Ratings section.
POWER SUPPLY BYPASSING
As with any power amplifier, proper supply bypassing is
critical for low noise performance and high power supply
rejection. Applications that employ a voltage regulator typically use a 10µF in parallel with a 0.1µF filter capacitors to
stabilize the regulator’s output, reduce noise on the supply
line, and improve the supply’s transient response. However,
their presence does not eliminate the need for a local 1.0µF
tantalum bypass capacitance connected between the
LM4940’s supply pins and ground. Do not substitute a ceramic capacitor for the tantalum. Doing so may cause oscillation. Keep the length of leads and traces that connect
capacitors between the LM4940’s power supply pin and
ground as short as possible. Connecting a 10µF capacitor,
C
, between the BYPASS pin and ground improves
BYPASS
the internal bias voltage’s stability and improves the amplifier’s PSRR. The PSRR improvements increase as the bypass pin capacitor value increases. Too large, however,
increases turn-on time and can compromise the amplifier’s
click and pop performance. The selection of bypass capacitor values, especially C
requirements, click and pop performance (as explained in
the section, SELECTING EXTERNAL COMPONENTS),
system cost, and size constraints.
MICRO-POWER SHUTDOWN
The LM4940 features an active-low micro-power shutdown
mode. When active, the LM4940’s micro-power shutdown
feature turns off the amplifier’s bias circuitry, reducing the
supply current. The low 40µA typical shutdown current is
achieved by applying a voltage to the SHUTDOWN pin that
is as near to GND as possible. A voltage that is greater than
GND may increase the shutdown current.
There are a few methods to control the micro-power shutdown. These include using a single-pole, single-throw switch
(SPST), a microprocessor, or a microcontroller. When using
a switch, connect a 100kΩ pull-up resistor between the
SHUTDOWN pin and V
SHUTDOWN pin and GND. Select normal amplifier operation by opening the switch. Closing the switch applies GND
to the SHUTDOWN pin, activating micro-power shutdown.
The switch and resistor guarantee that the SHUTDOWN pin
will not float. This prevents unwanted state changes. In a
system with a microprocessor or a microcontroller, use a
digital output to apply the active-state voltage to the SHUTDOWN pin.
. The heat sink can be created using
JA
, depends on desired PSRR
BYPASS
and the SPST switch between the
DD
SELECTING EXTERNAL COMPONENTS
Input Capacitor Value Selection
Two quantities determine the value of the input coupling
capacitor: the lowest audio frequency that requires amplification and desired output transient suppression.
As shown in Figure 3, the input resistor (R
capacitor (C
) produce a high pass filter cutoff frequency
IN
) and the input
IN
that is found using Equation (7).
= 1/2πRiC
f
c
i
(5)
As an example when using a speaker with a low frequency
limit of 50Hz, C
shown in Figure 3allows the LM4940 to drive high
C
INA
, using Equation (7) is 0.159µF. The 0.39µF
i
efficiency, full range speaker whose response extends below
30Hz.
Output Coupling Capacitor Value Selection
The capacitors C
OUTA
and C
that block the VDD/2 out-
OUTB
put DC bias voltage and couple the output AC signal to the
amplifier loads also determine low frequency response.
These capacitors, combined with their respective loads create a highpass filter cutoff frequency. The frequency is also
given by Equation (6).
Using the same conditions as above, with a 4Ω speaker,
is 820µF (nearest common valve).
C
OUT
Bypass Capacitor Value
Besides minimizing the input capacitor size, careful consideration should be paid to value of C
connected to the BYPASS pin. Since C
BYPASS
BYPASS
, the capacitor
determines
how fast the LM4940 settles to quiescent operation, its value
is critical when minimizing turn-on pops. The slower the
LM4940’s outputs ramp to their quiescent DC voltage (nominally V
/2), the smaller the turn-on pop. Choosing C
DD
BYPASS
equal to 10µF along with a small value of CIN(in the range of
0.1µF to 0.39µF), produces a click-less and pop-less shutdown function. As discussed above, choosing C
no larger
IN
than necessary for the desired bandwidth helps minimize
clicks and pops.
OPTIMIZING CLICK AND POP REDUCTION
PERFORMANCE
The LM4940 contains circuitry that eliminates turn-on and
shutdown transients ("clicks and pops"). For this discussion,
turn-on refers to either applying the power supply voltage or
when the micro-power shutdown mode is deactivated.
As the V
/2 voltage present at the BYPASS pin ramps to its
DD
final value, the LM4940’s internal amplifiers are configured
as unity gain buffers and are disconnected from the AMP
and AMPBpins. An internal current source charges the capacitor connected between the BYPASS pin and GND in a
controlled manner. Ideally, the input and outputs track the
voltage applied to the BYPASS pin. The gain of the internal
amplifiers remains unity until the voltage applied to the BYPASS pin.
The gain of the internal amplifiers remains unity until the
voltage on the bypass pin reaches V
/2. As soon as the
DD
voltage on the bypass pin is stable, the device becomes fully
operational and the amplifier outputs are reconnected to
their respective output pins. Although the BYPASS pin current cannot be modified, changing the size of C
BYPASS
alters
the device’s turn-on time. Here are some typical turn-on
times for various values of C
BYPASS
:
A
www.national.com10
Application Information (Continued)
CB(µF)TON(ms)
1.0120
2.2120
4.7200
10440
In order eliminate "clicks and pops", all capacitors must be
discharged before turn-on. Rapidly switching V
allow the capacitors to fully discharge, which may cause
"clicks and pops".
There is a relationship between the value of C
C
that ensures minimum output transient when power
BYPASS
is applied or the shutdown mode is deactivated. Best performance is achieved by setting the time constant created by
and Ri+Rfto a value less than the turn-on time for a
C
IN
given value of C
as shown in the table above.
BYPASS
AUDIO POWER AMPLIFIER DESIGN
Audio Amplifier Design: Driving 3W into a 4Ω load
The following are the desired operational parameters:
Power Output3W
Load Impedance4Ω
Input Level0.3V
Input Impedance20kΩ
Bandwidth100Hz–20kHz
The design begins by specifying the minimum supply voltage
necessary to obtain the specified output power. One way to
find the minimum supply voltage is to use the Output Power
vs Power Supply Voltage curve in the Typical Performance
Characteristics section. Another way, using Equation (8), is
to calculate the peak output voltage necessary to achieve
the desired output power for a given load impedance. To
account for the amplifier’s dropout voltage, two additional
voltages, based on the Clipping Dropout Voltage vs Power
Supply Voltage in the Typical Performance Characteris-
tics curves, must be added to the result obtained by Equa-
tion (8). The result is Equation (9).
DD
RMS
±
may not
and
IN
RMS
(max)
0.25dB
(8)
Thus, a minimum gain of 11.6 allows the LM4940’s to reach
full output swing and maintain low noise and THD+N performance. For this example, let A
BTL gain is set using the input (RIN
= 12. The amplifier’s overall
V
) and feedback (R)
A
resistors of the first amplifier in the series BTL configuration.
Additionaly,A
and Rf. With the desired input impedance set at 20kΩ,
R
IN
is twice the gain set by the first amplifier’s
V-BTL
the feedback resistor is found using Equation (11).
/ RIN=A
R
f
V
(9)
The value of Rfis 240kΩ. The nominal output power is 3W.
The last step in this design example is setting the amplifier’s
±
-3dB frequency bandwidth. To achieve the desired
0.25dB
pass band magnitude variation limit, the low frequency response must extend to at least one-fifth the lower bandwidth
limit and the high frequency response must extend to at least
five times the upper bandwidth limit. The gain variation for
±
both response limits is 0.17dB, well within the
0.25dB-
desired limit. The results are an
= 100Hz/5=20Hz(10)
f
L
and an
= 20kHzx5=100kHz(11)
f
L
As mentioned in the SELECTING EXTERNAL COMPO-NENTS section, R
INA
and C
, as well as C
INA
OUT
and RL,
create a highpass filter that sets the amplifier’s lower bandpass frequency limit. Find the coupling capacitor’s value
using Equation (14).
=1/ 2πRINf
C
IN
L
(12)
LM4940
(6)
V
DD=VOUTPEAK
+V
ODTOP+VODBOT
(7)
The Output Power vs. Power Supply Voltage graph for an 8Ω
load indicates a minimum supply voltage of 11.8V. The commonly used 12V supply voltage easily meets this. The additional voltage creates the benefit of headroom, allowing the
LM4940 to produce an output power of 3W without clipping
or other audible distortion. The choice of supply voltage must
also not create a situation that violates of maximum power
dissipation as explained above in the Power Dissipation
section. After satisfying the LM4940’s power dissipation requirements, the minimum differential gain needed to achieve
3W dissipation in a 4Ω BTL load is found using Equation
(10).
The result is
1 / (2πx20kΩx20Hz) = 0.398µF = C
IN
and
1 / (2πx4Ωx20Hz) = 1989µF = C
OUT
Use a 0.39µF capacitor for CINand a 2000µF capacitor for
, the closest standard values.
C
OUT
The product of the desired high frequency cutoff (100kHz in
this example) and the differential gain A
upper passband response limit. With A
, determines the
V
= 12 and fH=
V
100kHz, the closed-loop gain bandwidth product (GBWP) is
1.2mHz. This is less than the LM4940’s 3.5MHz GBWP. With
this margin, the amplifier can be used in designs that require
more differential gain while avoiding performance restricting
bandwidth limitations.
www.national.com11
Application Information (Continued)
RECOMMENDED PRINTED CIRCUIT BOARD LAYOUT
LM4940
Figure 5 through Figure 7 show the recommended two-layer
PC board layout that is optimized for the TO263-packaged
LM4940 and associated external components. This circuit
board is designed for use with an external 12V supply and
4Ω(min) speakers.
Demonstration Board Layout
This circuit board is easy to use. Apply 12V and ground to
the board’s V
speaker between the board’s OUT
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:
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.
BANNED SUBSTANCE COMPLIANCE
National Semiconductor certifies that the products and packing materials meet the provisions of the Customer Products
Stewardship Specification (CSP-9-111C2) and the Banned Substances and Materials of Interest Specification
(CSP-9-111S2) and contain no ‘‘Banned Substances’’ as defined in CSP-9-111S2.
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.
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.
LM4940 6W Stereo Audio Power Amplifier
National Semiconductor
Americas Customer
Support Center
Email: new.feedback@nsc.com
Tel: 1-800-272-9959
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.
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