NSC LM4923_07

LM4923 1.1 Watt Fully Differential Audio Power Amplifier With
Shutdown Select
General Description
Key Specifications
The LM4923 is a fully differential audio power amplifier primarily designed for demanding applications in mobile phones
and other portable communication device applications. It is
capable of delivering 1.1 watt of continuous average power to
an 8Ω BTL load with less than 1% distortion (THD+N) from a
5VDC power supply.
Boomer audio power amplifiers were designed specifically to
provide high quality output power with a minimal amount of
external components. The LM4923 does not require output
coupling capacitors or bootstrap capacitors, and therefore is
ideally suited for mobile phone and other low voltage applications where minimal power consumption is a primary requirement.
The LM4923 features a low-power consumption shutdown
mode. To facilitate this, Shutdown may be enabled by logic
low. Additionally, the LM4923 features an internal thermal
shutdown protection mechanism.
The LM4923 contains advanced pop & click circuitry which
eliminates noises which would otherwise occur during turn-on
and turn-off transitions.
■ Improved PSRR at 217Hz
85dB(typ)
■ Power Output at 5.0V
@ 1% THD+N
1.1W(typ)
■ Power Output at 3.3V
@ 1% THD+N
400mW(typ)
■ Shutdown Current
0.1µA(typ)
Features
■
■
■
■
■
Fully differential amplification
Available in space-saving LLP package
Ultra low current shutdown mode
Can drive capacitive loads up to 100pF
Improved pop & click circuitry eliminates noises during
turn-on and turn-off transitions
■ 2.4 - 5.5V operation
■ No output coupling capacitors, snubber networks or
bootstrap capacitors required
Applications
■ Mobile phones
■ PDAs
■ Portable electronic devices
Connection Diagrams
LQ Package
8 Pin LQ Marking
20071302
X − Date Code
TT − Die Traceability
G − Boomer
B2 − LM4923LQ
20071330
Top View
Order Number LM4923LQ
See NS Package Number LQB08A
8 Pin MSOP Package
200713a1
Top View
See Order Number LM4923MM
See NS Package Number MUA08A
Boomer® is a registered trademark of National Semiconductor Corporation.
© 2007 National Semiconductor Corporation
200713
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LM4923 1.1 Watt Fully Differential Audio Power Amplifier With Shutdown Select
December 17, 2007
LM4923
Typical Application
20071313
FIGURE 1. Typical Audio Amplifier Application Circuit
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2
If Military/Aerospace specified devices are required,
please contact the National Semiconductor Sales Office/
Distributors for availability and specifications.
Supply Voltage
Storage Temperature
Input Voltage
Power Dissipation (Note 3)
ESD Susceptibility (Note 4)
ESD Susceptibility (Note 5)
Junction Temperature
Thermal Resistance
θJA (LLP)
140°C/W
θJA (MM)
210°C/W
θJC (MM)
Soldering Information
See AN-1187
6.0V
−65°C to +150°C
−0.3V to VDD +0.3V
Internally Limited
2000V
200V
150°C
56°C/W
Operating Ratings
Temperature Range
TMIN ≤ TA ≤ TMAX
Supply Voltage
−40°C ≤ TA ≤ 85°C
2.4V ≤ VDD ≤ 5.5V
Electrical Characteristics VDD = 5V
(Notes 1, 2)
The following specifications apply for VDD = 5V, AV = 1, and 8Ω load unless otherwise specified. Limits apply for TA = 25°C.
LM4923
Symbol
IDD
Quiescent Power Supply Current
Units
(Limits)
Typical
Limit
(Note 6)
(Note 7)
VIN = 0V, RL = 8Ω
4
4
9
9
mA (max)
0.1
1
µA (max)
1
Parameter
Conditions
VIN = 0V, no load
ISD
Shutdown Current
VSHUTDOWN = GND
Po
Output Power
THD = 1% (max); f = 1 kHz
LM4923, RL = 8Ω
1.1
THD+N
Total Harmonic Distortion+Noise
Po = 0.4 Wrms; f = 1kHz
0.02
PSRR
Power Supply Rejection Ratio
Vripple = 200mV sine p-p
%
f = 217Hz (Note 8)
85
73
f = 1kHz (Note 8)
85
73
50
dB
CMRR
Common_Mode Rejection Ratio
f = 217Hz,
VCM = 200mVpp
VOS
Output Offset
VIN = 0V
4
mV
VSDIH
Shutdown Voltage Input High
0.9
V
VSDIL
Shutdown Voltage Input Low
0.7
V
Electrical Characteristics VDD = 3V
(Notes 1, 2)
The following specifications apply for VDD = 3V, AV = 1, and 8Ω load unless otherwise specified. Limits apply for TA = 25°C.
LM4923
Symbol
IDD
Quiescent Power Supply Current
Units
(Limits)
Typical
Limit
(Note 6)
(Note 7)
VIN = 0V, RL = 8Ω
3
3
5.5
5.5
mA (max)
0.1
1
µA (max)
Parameter
Conditions
VIN = 0V, no load
ISD
Shutdown Current
VSHUTDOWN = GND
Po
Output Power
THD = 1% (max); f = 1kHz
LM4923, RL = 8Ω
0.375
W
THD+N
Total Harmonic Distortion+Noise
Po = 0.25Wrms; f = 1kHz
0.02
%
PSRR
Power Supply Rejection Ratio
Vripple = 200mV sine p-p
f = 217Hz (Note 8)
85
f = 1kHz (Note 8)
85
73
CMRR
Common-Mode Rejection Ratio
f = 217Hz
VCM = 200mVpp
50
dB
VOS
Output Offset
VIN = 0V
4
mV
3
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LM4923
Absolute Maximum Ratings (Note 2)
LM4923
LM4923
Symbol
Parameter
Conditions
Typical
Limit
(Note 6)
(Note 7)
Units
(Limits)
VSDIH
Shutdown Voltage Input High
0.8
V
VSDIL
Shutdown Voltage Input Low
0.6
V
Note 1: All voltages are measured with respect to the ground 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 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: 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 LM4923, see power
derating curve for additional information.
Note 4: Human body model, 100pF discharged through a 1.5kΩ 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: Datasheet min/max specification limits are guaranteed by design, test, or statistical analysis.
Note 8: 10Ω terminated input.
External Components Description
(Figure 1)
Components
Functional Description
1.
Ri
Inverting input resistance which sets the closed-loop gain in conjunction with Rf.
2.
Rf
Feedback resistance which sets the closed-loop gain in conjunction with Ri.
3.
CS
Supply bypass capacitor which provides power supply filtering. Refer to the Power Supply Bypassing section for
information concerning proper placement and selection of the supply bypass capacitor.
4.
CB
Bypass pin capacitor which provides half-supply filtering. Refer to the section, Proper Selection of External
Components, for information concerning proper placement and selection of CB.
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LM4923
Typical Performance Characteristics
THD+N vs Frequency
VDD = 2.6V, RL = 8Ω, PO = 150mW
THD+N vs Frequency
VDD = 2.6V, RL = 4Ω, PO = 150mW
20071306
20071305
THD+N vs Frequency
VDD = 5V, RL = 8Ω, PO = 400mW
THD+N vs Frequency
VDD = 3V, RL = 8Ω, PO = 275mW
20071309
20071308
THD+N vs Frequency
VDD = 3V, RL = 4Ω, PO = 225mW
THD+N vs Output Power
VDD = 2.6V, RL = 8Ω
20071307
20071311
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LM4923
THD+N vs Output Power
VDD = 2.6V, RL = 4Ω
THD+N vs Output Power
VDD = 5V, RL = 8Ω
20071310
20071315
THD+N vs Output Power
VDD = 3V, RL = 8Ω
THD+N vs Output Power
VDD = 3V, RL = 4Ω
20071314
20071312
PSRR vs Frequency
VDD = 5V, RL = 8Ω, Input terminated
PSRR vs Frequency
VDD = 3V, RL = 8Ω, Input terminated
20071304
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20071303
6
LM4923
Output Power vs Supply Voltage
RL = 8Ω
CMRR vs Frequency
VDD = 5V, RL = 8Ω
20071301
20071317
CMRR vs Frequency
VDD = 3V, RL = 8Ω
PSRR vs Common Mode Voltage
VDD = 3V, RL = 8Ω, f = 217Hz
20071326
20071322
PSRR vs Common Mode Voltage
VDD = 5V, RL = 8Ω, f = 217Hz
Power Dissipation vs Output Power
VDD = 2.6V, RL = 8Ω and 4Ω
20071316
20071321
7
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LM4923
Power Dissipation vs Output Power
VDD = 5V, RL = 8Ω
Power Dissipation vs Output Power
VDD = 3V, RL = 8Ω
20071319
20071325
Power Derating Curve
Noise Floor
VDD = 5V
20071318
20071324
Noise Floor
VDD = 3V
Clipping Voltage vs Supply Voltage
20071323
20071320
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Supply Current Shutdown Voltage
20071328
20071327
Application Information
A bridged configuration, such as the one used in the LM4923,
also creates a second advantage over single-ended amplifiers. Since the differential outputs, Vo1 and Vo2, are biased at
half-supply, no net DC voltage exists across the load. This
assumes that the input resistor pair and the feedback resistor
pair are properly matched (see Proper Selection of External
Components). BTL configuration eliminates the output coupling capacitor required in single-supply, single-ended amplifier configurations. If an output coupling capacitor is not used
in a single-ended output configuration, the half-supply bias
across the load would result in both increased internal IC
power dissipation as well as permanent loudspeaker damage. Further advantages of bridged mode operation specific
to fully differential amplifiers like the LM4923 include increased power supply rejection ratio, common-mode noise
reduction, and click and pop reduction.
DIFFERENTIAL AMPLIFIER EXPLANATION
The LM4923 is a fully differential audio amplifier that features
differential input and output stages. Internally this is accomplished by two circuits: a differential amplifier and a common
mode feedback amplifier that adjusts the output voltages so
that the average value remains VDD / 2. When setting the differential gain, the amplifier can be considered to have
"halves". Each half uses an input and feedback resistor (Ri1
and RF1) to set its respective closed-loop gain (see Figure 1).
With Ri1 = Ri2 and RF1 = RF2, the gain is set at -RF / Ri for each
half. This results in a differential gain of
AVD = -RF/Ri
LM4923
Output Power vs Load Resistance
(1)
It is extremely important to match the input resistors to each
other, as well as the feedback resistors to each other for best
amplifier performance. See the Proper Selection of External Components section for more information. A differential
amplifier works in a manner where the difference between the
two input signals is amplified. In most applications, this would
require input signals that are 180° out of phase with each other. The LM4923 can be used, however, as a single ended
input amplifier while still retaining its fully differential benefits.
In fact, completely unrelated signals may be placed on the
input pins. The LM4923 simply amplifies the difference between them.
EXPOSED-DAP PACKAGE PCB MOUNTING
CONSIDERATIONS
The LM4923's exposed-DAP (die attach paddle) package
(LLP) provide 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, finally, surrounding air. Failing to optimize thermal design may compromise the LM4923's
high power performance and activate unwanted, though necessary, thermal shutdown protection. The LLP 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 and heat
sink and radiation area. Place the heat sink area on either
outside plane in the case of a 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 a thermal via. The via diameter should be 0.012in 0.013in. Ensure efficient thermal conductivity by platingthrough and solder-filling the vias.
All of these applications provide what is known as a "bridged
mode" output (bridge-tied-load, BTL). This results in output
signals at Vo1 and Vo2 that are 180° out of phase with respect
to each other. Bridged mode operation is different from the
single-ended amplifier configuration that connects the load
between the amplifier output and ground. A bridged amplifier
design has distinct advantages over the single-ended configuration: it provides differential drive to the load, thus doubling
maximum possible output swing for a specific supply voltage.
Four times the output power is possible compared with 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 excess clipping, please refer to the Audio Power Amplifier Design section.
Best thermal performance is achieved with the largest practical copper heat sink area. In all circumstances and conditions, the junction temperature must be held below 150°C to
prevent activating the LM4923's thermal shutdown protection.
The LM4923's power de-rating curve in the Typical Performance Characteristics shows the maximum power dissipation versus temperature. Example PCB layouts are shown in
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LM4923
either the supply voltage must be decreased, the load
impedance increased, the ambient temperature reduced, or
the θJA reduced with heatsinking. In many cases, larger traces
near the output, VDD, and GND pins can be used to lower the
θJA. The larger areas of copper provide a form of heatsinking
allowing higher power dissipation. For the typical application
of a 5V power supply, with an 8Ω load, the maximum ambient
temperature possible without violating the maximum junction
temperature is approximately 62°C provided that device operation is around the maximum power dissipation point. Recall that internal power dissipation is a function of output
power. If typical operation is not around the maximum power
dissipation point, the LM4923 can operate at higher ambient
temperatures. Refer to the Typical Performance Characteristics curves for power dissipation information.
the Demonstration Board Layout section. Further detailed
and specific information concerning PCB layout, fabrication,
and mounting an LLP package is available from National
Semiconductor's package Engineering Group under application note AN1187.
PCB LAYOUT AND SUPPLY REGULATION
CONSIDERATIONS FOR DRIVING 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 dependent
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. 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.
POWER SUPPLY BYPASSING
As with any power amplifier, proper supply bypassing is critical for low noise performance and high power supply rejection ratio (PSRR). The capacitor location on both the bypass
and power supply pins should be as close to the device as
possible. A larger half-supply bypass capacitor improves
PSRR because it increases half-supply stability. Typical applications employ a 5V regulator with 10µF and 0.1µF bypass
capacitors that increase supply stability. This, however, does
not eliminate the need for bypassing the supply nodes of the
LM4923. The LM4923 will operate without the bypass capacitor CB, although the PSRR may decrease. A 1µF capacitor is
recommended for CB. This value maximizes PSRR performance. Lesser values may be used, but PSRR decreases at
frequencies below 1kHz. The issue of CB selection is thus
dependant upon desired PSRR and click and pop performance as explained in the section Proper Selection of External Components.
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.
POWER DISSIPATION
Power dissipation is a major concern when designing a successful amplifer, whether the amplifier is bridged or singleended. 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.
PDMAX = (VDD)2 / (2π2RL) Single-Ended
SHUTDOWN FUNCTION
In order to reduce power consumption while not in use, the
LM4923 contains shutdown circuitry that is used to turn off the
amplifier's bias circuitry. The device may then be placed into
shutdown mode by toggling the Shutdown Select pin to logic
low. The trigger point for shutdown is shown as a typical value
in the Supply Current vs Shutdown Voltage graphs in the
Typical Performance Characteristics section. It is best to
switch between ground and supply for maximum performance. While the device may be disabled with shutdown
voltages in between ground and supply, 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.
(2)
However, a direct consequence of the increased power delivered to the load by a bridge amplifier is an increase in
internal power dissipation versus a single-ended amplifier operating at the same conditions.
PDMAX = 4 * (VDD)2 / (2π2RL) Bridge Mode
(3)
Since the LM4923 has bridged outputs, the maximum internal
power dissipation is 4 times that of a single-ended amplifier.
Even with this substantial increase in power dissipation, the
LM4923 does not require additional heatsinking under most
operating conditions and output loading. From Equation 3,
assuming a 5V power supply and an 8Ω load, the maximum
power dissipation point is 625mW. The maximum power dissipation point obtained from Equation 3 must not be greater
than the power dissipation results from Equation 4:
PDMAX = (TJMAX - TA) / θJA
In many applications, a microcontroller or microprocessor
output is used to control the shutdown circuitry, which provides a quick, smooth transition to shutdown. Another solution
is to use a single-throw switch in conjunction with an external
pull-up resistor. This scheme guarantees that the shutdown
pin will not float, thus preventing unwanted state changes.
PROPER SELECTION OF EXTERNAL COMPONENTS
Proper selection of external components in applications using
integrated power amplifiers is critical when optimizing device
and system performance. Although the LM4923 is tolerant to
a variety of external component combinations, consideration
of component values must be made when maximizing overall
system quality.
The LM4923 is unity-gain stable, giving the designer maximum system flexibility. The LM4923 should be used in low
closed-loop gain configurations to minimize THD+N values
(4)
The LM4923's θJA in an LQB08A package is 140°C/W. Depending on the ambient temperature, TA, of the system surroundings, Equation 4 can be used to find the maximum
internal power dissipation supported by the IC packaging. If
the result of Equation 3 is greater than that of Equation 4, then
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VCMi < (VDD-1.2)*((Rf+(Ri)/(Rf)-VDD*(Ri / 2Rf)
(5)
-RF / RI = AVD
(6)
A designer must first determine the minimum supply rail to
obtain the specified output power. The supply rail can easily
be found by extrapolating from the Output Power vs Supply
Voltage graphs in the Typical Performance Characteristics section. A second way to determine the minimum supply
rail is to calculate the required VOPEAK using Equation 7 and
add the dropout voltages. Using this method, the minimum
supply voltage is (Vopeak + (VDO TOP + (VDO BOT )), where
VDO BOT and VDO TOP are extrapolated from the Dropout Voltage vs Supply Voltage curve in the Typical Performance
Characteristics section.
(7)
Using the Output Power vs Supply Voltage graph for an 8Ω
load, the minimum supply rail just about 5V. Extra supply voltage creates headroom that allows the LM4923 to reproduce
peaks in excess of 1W without producing audible distortion.
At this time, the designer 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 8.
Special care must be taken to match the values of the feedback resistors (RF1 and RF2) to each other as well as matching
the input resistors (Ri1 and Ri2) to each other (see Figure 1)
more in front. Because of the balanced nature of differential
amplifiers, resistor matching differences can result in net DC
currents across the load. This DC current can increase power
consumption, internal IC power dissipation, reduce PSRR,
and possibly damaging the loudspeaker. The chart below
demonstrates this problem by showing the effects of differing
values between the feedback resistors while assuming that
the input resistors are perfectly matched. The results below
apply to the application circuit shown in Figure 1, and assumes that VDD = 5V, RL = 8Ω, and the system has DC
coupled inputs tied to ground.
Tolerance RF1
RF2
V02 - V01
ILOAD
20%
0.8R
1.2R
-0.500V
62.5mA
10%
0.9R
1.1R
-0.250V
31.25mA
5%
0.95R 1.05R -0.125V
15.63mA
1%
0.99R 1.01R -0.025V
3.125mA
0%
R
0
R
0
(8)
Rf / Ri = AVD
From Equation 7, the minimum AVD is 2.83. Since the desired
input impedance was 20kΩ, a ratio of 2.83:1 of Rf to Ri results
in an allocation of Ri = 20kΩ for both input resistors and Rf =
60kΩ for both feedback resistors. The final design step is to
address the bandwidth requirement which must be stated as
a single -3dB frequency point. Five times away from a -3dB
point is 0.17dB down from passband response which is better
than the required ±0.25dB specified.
fH = 20kHz * 5 = 100kHz
The high frequency pole is determined by the product of the
desired frequency pole, fH , and the differential gain, AVD .
With a AVD = 2.83 and fH = 100kHz, the resulting GBWP =
150kHz which is much smaller than the LM4923 GBWP of
10MHz. This figure displays that if a designer has a need to
design an amplifier with a higher differential gain, the LM4923
can still be used without running into bandwidth limitations.
Similar results would occur if the input resistors were not
carefully matched. Adding input coupling capacitors in between the signal source and the input resistors will eliminate
this problem, however, to achieve best performance with minimum component count it is highly recommended that both
the feedback and input resistors matched to 1% tolerance or
better.
AUDIO POWER AMPLIFIER DESIGN
Design a 1W/8Ω Audio Amplifier
Given:
Power Output
Load Impedance
Input Level
Input Impedance
Bandwidth
1Wrms
8Ω
1Vrms
20kΩ
100Hz–20kHz ± 0.25dB
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LM4923
and maximize signal to noise ratio. Low gain configurations
require large input signals to obtain a given output power. Input signals equal to or greater than 1Vrms are available from
sources such as audio codecs. Please refer to the Audio
Power Amplifier Design section for a more complete explanation of proper gain selection. When used in its typical
application as a fully differential power amplifier the LM4923
does not require input coupling capacitors for input sources
with DC common-mode voltages of less than VDD. Exact allowable input common-mode voltage levels are actually a
function of VDD, Ri, and Rf and may be determined by Equation 5:
LM4923
Revision History
Rev
Date
1.0
09/28/07
Added the MSOP package, then released.
1.01
12/17/07
Updated the mktg outline LQB08A into the rev B.
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Description
12
LM4923
Physical Dimensions inches (millimeters) unless otherwise noted
LQ Package
Order Number LM4923LQ
NS Package Number LQB08A
MSOP Package
Order Number LM4923MM
NS Package Number MUA08A
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LM4923 1.1 Watt Fully Differential Audio Power Amplifier With Shutdown Select
Notes
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