NSC LM4673

LM4673 Filterless, 2.65W, Mono, Class D Audio Power Amplifier
General Description
Key Specifications
The LM4673 is a single supply, high efficiency, 2.65W, mono,
Class D audio amplifier. A low noise, filterless PWM architecture eliminates the output filter, reducing external component
count, board area consumption, system cost, and simplifying
design.
The LM4673 is designed to meet the demands of mobile
phones and other portable communication devices. Operating on a single 5V supply, it is capable of driving a 4Ω speaker
load at a continuous average output of 2.1W with less than
1% THD+N. Its flexible power supply requirements allow operation from 2.4V to 5.5V.
The LM4673 has high efficiency with speaker loads compared
to a typical Class AB amplifier. With a 3.6V supply driving an
8Ω speaker, the IC's efficiency for a 100mW power level is
80%, reaching 88% at 400mW output power.
The LM4673 features a low-power consumption shutdown
mode. Shutdown may be enabled by driving the Shutdown
pin to a logic low (GND).
The gain of the LM4673 is externally configurable which allows independent gain control from multiple sources by summing the signals. Output short circuit and thermal overload
protection prevent the device from damage during fault conditions.
■ Efficiency at 3.6V, 400mW into 8Ω speaker
88% (typ)
■ Efficiency at 3.6V, 100mW into 8Ω speaker
80% (typ)
■ Efficiency at 5V, 1W into 8Ω speaker
86% (typ)
■ Quiescent current, 3.6V supply
2.1mA (typ)
■ 0.01µA (typ)
Total shutdown power supply current
■ Single supply range
■ PSRR, f = 217Hz
2.4V to 5.5V
78dB
Features
■
■
■
■
■
■
■
■
Mono Class D Operation
No output filter required for inductive loads
Externally configurable gain
Very fast turn on time: 17μs (typ)
Minimum external components
"Click and pop" suppression circuitry
Micro-power shutdown mode
Available in space-saving 0.4mm pitch micro SMD and
LLPTm packages
Applications
■ Mobile phones
■ PDAs
■ Portable electronic devices
Boomer® is a registered trademark of National Semiconductor Corporation.
© 2007 National Semiconductor Corporation
201522
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LM4673 Filterless, 2.65W, Mono, Class D Audio Power Amplifier
November 1, 2007
LM4673
Typical Application
201522j3
FIGURE 1. Typical Audio Amplifier Application Circuit
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LM4673
Connection Diagrams
9 Bump micro SMD Package
micro SMD Marking
20152257
Top View
X — Date Code
T— Die Traceability
G — Boomer Family
G4 — LM4673TM
20152236
Top View
Order Number LM4673TM
See NS Package Number TMD09GGA
Leadless Leadframe Package (LLP)
LLP Marking
20152202
Top View
Z — Plant Code
XY — Date Code
TT — Die Traceability
L4673 — LM4673SD
20152201
Top View
Order Number LM4673SD
See NS Package Number SDA08A
Contact NSC Sales Office for Availability
3
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LM4673
Thermal Resistance
Absolute Maximum Ratings (Notes 1, 2)
θJA (micro SMD)
If Military/Aerospace specified devices are required,
please contact the National Semiconductor Sales Office/
Distributors for availability and specifications.
Supply Voltage (Note 1)
Storage Temperature
Voltage at Any Input Pin
99.1°C/W
73°C/W
θJA (LLP)
Soldering Information
See AN-1112 "microSMD Wafers Level Chip Scale
Package."
6.0V
−65°C to +150°C
VDD + 0.3V ≥ V ≥ GND - 0.3V
Power Dissipation (Note 3)
Internally Limited
ESD Susceptibility, all other pins (Note 4)
2.0kV
ESD Susceptibility (Note 5)
200V
Junction Temperature (TJMAX)
150°C
Operating Ratings
(Notes 1, 2)
Temperature Range
TMIN ≤ TA ≤ TMAX
Supply Voltage
−40°C ≤ TA ≤ 85°C
2.4V ≤ VDD ≤ 5.5V
Electrical Characteristics
(Notes 1, 2)
The following specifications apply for AV = 2V/V (RI = 150kΩ), RL = 15µH + 8Ω + 15µH unless otherwise specified. Limits apply for
TA = 25°C.
LM4673
Symbol
Parameter
Conditions
Typical
Limit
(Note 6)
(Notes 7, 8)
Units
(Limits)
|VOS|
Differential Output Offset Voltage
VI = 0V, AV = 2V/V,
VDD = 2.4V to 5.0V
|IIH|
Logic High Input Current
VDD = 5.0V, VI = 5.5V
17
100
|IIL|
Logic Low Input Current
VDD = 5.0V, VI = –0.3V
0.9
5
μA (max)
VIN = 0V, No Load, VDD = 5.0V
2.6
3.75
mA (max)
VIN = 0V, No Load, VDD = 3.6V
2.1
2.9
mA
VIN = 0V, No Load, VDD = 2.4V
1.7
2.3
mA (max)
VIN = 0V, RL = 8Ω, VDD = 5.0V
2.6
VIN = 0V, RL = 8Ω, VDD = 3.6V
2.1
VIN = 0V, RL = 8Ω, VDD = 2.4V
1.7
VSHUTDOWN = 0V
VDD = 2.4V to 5.0V
0.01
1
μA (max)
1.4
V (min)
0.4
V (max)
IDD
Quiescent Power Supply Current
ISD
Shutdown Current
VSDIH
Shutdown voltage input high
VSDIL
Shutdown voltage input low
ROSD
Output Impedance
AV
Gain
RSD
Resistance from Shutdown Pin to
GND
PO
Output Power
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VSHUTDOWN = 0.4V
5
mV (max)
100
300kΩ/RI
μA (max)
kΩ
270kΩ/RI
330kΩ/RI
V/V (min)
V/V (max)
300
kΩ
RL = 15μH + 4Ω + 15μH
THD = 10% (max)
f = 1kHz, 22kHz BW
VDD = 5V
VDD = 3.6V
VDD = 2.5V
2.65
1.3
550
W
W
mW
RL = 15μH + 4Ω + 15μH
THD = 1% (max)
f = 1kHz, 22kHz BW
VDD = 5V
VDD = 3.6V
VDD = 2.5V
2.15
1.06
450
W
W
mW
4
Symbol
Parameter
Conditions
Typical
Limit
(Note 6)
(Notes 7, 8)
Units
(Limits)
RL = 15μH + 8Ω + 15μH
THD = 10% (max)
f = 1kHz, 22kHz BW
PO
THD+N
Output Power
Total Harmonic Distortion + Noise
VDD = 5V
1.7
W
VDD = 3.6V
870
mW
VDD = 2.5V
350
mW
RL = 15μH + 8Ω + 15μH
THD = 1% (max)
f = 1kHz, 22kHz BW
VDD = 5V
1.24
VDD = 3.6V
650
PSRR
mW
VDD = 2.5V
300
mW
VDD = 5V, PO = 0.1W, f = 1kHz
0.03
%
VDD = 3.6V, PO = 0.1W, f = 1kHz
0.02
%
VDD = 2.5V, PO = 0.1W, f = 1kHz
0.02
%
78
dB
72
dB
97
dB
30
μVRMS
23
μVRMS
70
dB
VRipple = 200mVPP Sine,
fRipple = 217Hz, VDD = 3.6, 5V
Power Supply Rejection Ratio
(Input Referred)
W
600
Inputs to AC GND, CI = 2μF
VRipple = 200mVPP Sine,
fRipple = 1kHz, VDD = 3.6, 5V
Inputs to AC GND, CI = 2μF
SNR
Signal to Noise Ratio
εOUT
Output Noise
(Input Referred)
VDD = 5V, PO = 1WRMS
VDD = 3.6V, f = 20Hz – 20kHz
Inputs to AC GND, CI = 2μF
No Weighting
VDD = 3.6V, Inputs to AC GND
CI = 2μF, A Weighted
CMRR
Common Mode Rejection Ratio
(Input Referred)
VDD = 3.6V, VRipple = 1VPP Sine
fRipple = 217Hz
TWU
Wake-up Time
VDD = 3.6V
TSD
Shutdown Time
VDD = 3.6V, POUT = 400mW
η
Efficiency
RL = 8Ω
VDD = 5V, POUT = 1W
RL = 8Ω
5
17
μs
140
μs
88
%
86
%
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LM4673
LM4673
LM4673
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 LM4673, TJMAX = 150°C.
The typical θJA is 99.1°C/W for the micro SMD package.
Note 4: Human body model, 100pF discharged through a 1.5kΩ resistor.
Note 5: Machine Model, 220pF – 240pF discharged through all pins.
Note 6: Typical specifications are specified at 25°C and represent the parametric norm.
Note 7: Tested 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. Exposure to direct sunlight will increase ISD by a maximum of 2µA. The Shutdown pin
should be driven as close as possible to GND for minimal shutdown current and to VDD for the best THD performance in PLAY mode. See the Application
Information section under SHUTDOWN FUNCTION for more information.
Note 10: The performance graphs were taken using the Audio Precision AUX-0025 Switching Amplifier measurement Filter in series with the LC filter on the
demo board.
External Components Description
(Figure 1)
Components
Functional Description
1.
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.
2.
CI
Input AC coupling capacitor which blocks the DC voltage at the amplifier's input terminals.
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LM4673
Typical Performance Characteristics
THD + N vs Output Power
f = 1kHz, RL = 8Ω
THD + N vs Output Power
f = 1kHz, RL = 4Ω
20152240
20152241
THD + N vs Frequency
VDD = 2.5V, POUT = 100mW, RL = 8Ω
THD + N vs Frequency
VDD = 3.6V, POUT = 150mW, RL = 8Ω
20152242
20152243
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LM4673
THD + N vs Frequency
VDD = 5V, POUT = 200mW, RL = 8Ω
THD + N vs Frequency
VDD = 2.5V, POUT = 100mW, RL = 4Ω
20152244
20152245
THD + N vs Frequency
VDD = 3.6V, POUT = 100mW, RL = 4Ω
THD + N vs Frequency
VDD = 5V, POUT = 150mW, RL = 4Ω
20152246
20152247
Efficiency vs. Output Power
RL = 4Ω, f = 1kHz
Efficiency vs. Output Power
RL = 8Ω, f = 1kHz
20152249
20152248
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LM4673
Power Dissipation vs. Output Power
RL = 4Ω, f = 1kHz
Power Dissipation vs. Output Power
RL = 8Ω, f = 1kHz
20152250
20152251
Output Power vs. Supply Voltage
RL = 4Ω, f = 1kHz
Output Power vs. Supply Voltage
RL = 8Ω, f = 1kHz
20152252
20152253
PSRR vs. Frequency
VDD = 3.6V ,VRIPPLE = 200mVP-P, RL = 8Ω
CMRR vs. Frequency
VDD = 3.6V, VCM = 1VP-P, RL = 8Ω
20152254
20152255
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LM4673
Supply Current vs. Supply Voltage
No Load
20152256
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10
ply create a voltage drop. The voltage loss on the traces
between the LM4673 and the load results is lower output
power and decreased efficiency. Higher trace resistance between the supply and the LM4673 has the same effect as a
poorly regulated supply, increased ripple on the supply line
also reducing the peak output power. The effects of residual
trace resistance increases as output current increases due to
higher output power, decreased load impedance or both. To
maintain the highest output voltage swing and corresponding
peak output power, the PCB traces that connect the output
pins to the load and the supply pins to the power supply
should be as wide as possible to minimize trace resistance.
The use of power and ground planes will give the best THD
+N performance. While reducing trace resistance, the use of
power planes also creates parasite capacitors that help to filter the power supply line.
The inductive nature of the transducer load can also result in
overshoot on one or both edges, clamped by the parasitic
diodes to GND and VDD in each case. From an EMI standpoint, this is an aggressive waveform that can radiate or
conduct to other components in the system and cause interference. It is essential to keep the power and output traces
short and well shielded if possible. Use of ground planes,
beads, and micro-strip layout techniques are all useful in preventing unwanted interference.
As the distance from the LM4673 and the speaker increase,
the amount of EMI radiation will increase since the output
wires or traces acting as antenna become more efficient with
length. What is acceptable EMI is highly application specific.
Ferrite chip inductors placed close to the LM4673 may be
needed to reduce EMI radiation. The value of the ferrite chip
is very application specific.
GENERAL AMPLIFIER FUNCTION
The LM4673 features a filterless modulation scheme. The
differential outputs of the device switch at 300kHz from VDD
to GND. When there is no input signal applied, the two outputs
(VO1 and VO2) switch with a 50% duty cycle, with both outputs
in phase. Because the outputs of the LM4673 are differential,
the two signals cancel each other. This results in no net voltage across the speaker, thus there is no load current during
an idle state, conserving power.
With an input signal applied, the duty cycle (pulse width) of
the LM4673 outputs changes. For increasing output voltages,
the duty cycle of VO1 increases, while the duty cycle of VO2
decreases. For decreasing output voltages, the converse occurs, the duty cycle of VO2 increases while the duty cycle of
VO1 decreases. The difference between the two pulse widths
yields the differential output voltage.
POWER DISSIPATION AND EFFICIENCY
In general terms, efficiency is considered to be the ratio of
useful work output divided by the total energy required to produce it with the difference being the power dissipated, typically, in the IC. The key here is “useful” work. For audio
systems, the energy delivered in the audible bands is considered useful including the distortion products of the input
signal. Sub-sonic (DC) and super-sonic components
(>22kHz) are not useful. The difference between the power
flowing from the power supply and the audio band power being transduced is dissipated in the LM4673 and in the transducer load. The amount of power dissipation in the LM4673
is very low. This is because the ON resistance of the switches
used to form the output waveforms is typically less than
0.25Ω. This leaves only the transducer load as a potential
"sink" for the small excess of input power over audio band
output power. The LM4673 dissipates only a fraction of the
excess power requiring no additional PCB area or copper
plane to act as a heat sink.
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 (CS) location should be as
close as possible to the LM4673. Typical applications employ
a voltage regulator with a 10µF and a 0.1µF bypass capacitors
that increase supply stability. These capacitors do not eliminate the need for bypassing on the supply pin of the LM4673.
A 4.7µF tantalum capacitor is recommended.
DIFFERENTIAL AMPLIFIER EXPLANATION
As logic supply voltages continue to shrink, designers are increasingly turning to differential analog signal handling to
preserve signal to noise ratios with restricted voltage swing.
The LM4673 is a fully differential amplifier that features differential input and output stages. A differential amplifier amplifies the difference between the two input signals. Traditional audio power amplifiers have typically offered only singleended inputs resulting in a 6dB reduction in signal to noise
ratio relative to differential inputs. The LM4673 also offers the
possibility of DC input coupling which eliminates the two external AC coupling, DC blocking capacitors. The LM4673 can
be used, however, as a single ended input amplifier while still
retaining it's fully differential benefits. In fact, completely unrelated signals may be placed on the input pins. The LM4673
simply amplifies the difference between the signals. A major
benefit of a differential amplifier is the improved common
mode rejection ratio (CMRR) over single input amplifiers. The
common-mode rejection characteristic of the differential amplifier reduces sensitivity to ground offset related noise injection, especially important in high noise applications.
SHUTDOWN FUNCTION
In order to reduce power consumption while not in use, the
LM4673 contains shutdown circuitry that reduces current
draw to less than 0.01µA. The trigger point for shutdown is
shown as a typical value in the Electrical Characteristics Tables and in the Shutdown Hysteresis Voltage graphs found in
the Typical Performance Characteristics section. It is best
to switch between ground and supply for minimum current
usage while in the shutdown state. While the LM4673 may be
disabled with shutdown voltages in between ground and supply, the idle current will be greater than the typical 0.01µA
value.
The LM4673 has an internal resistor connected between
GND and Shutdown pins. The purpose of this resistor is to
eliminate any unwanted state changes when the Shutdown
pin is floating. The LM4673 will enter the shutdown state when
the Shutdown pin is left floating or if not floating, when the
shutdown voltage has crossed the threshold. To minimize the
supply current while in the shutdown state, the Shutdown pin
should be driven to GND or left floating. If the Shutdown pin
is not driven to GND, the amount of additional resistor current
PCB LAYOUT CONSIDERATIONS
As output power increases, interconnect resistance (PCB
traces and wires) between the amplifier, load and power sup11
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LM4673
Application Information
LM4673
differential input configuration shown in Figure 2. Equation (2)
above is used to determine the value of the Ri resistors for a
desired gain.
Input capacitors can be used in a differential configuration as
shown in Figure 3. Equation (3) above is used to determine
the value of the Ci capacitors for a desired frequency response due to the high-pass filter created by Ci and Ri.
Equation (2) above is used to determine the value of the Ri
resistors for a desired gain.
The LM4673 can be used to amplify more than one audio
source. Figure 4 shows a dual differential input configuration.
The gain for each input can be independently set for maximum design flexibility using the Ri resistors for each input and
Equation (2). Input capacitors can be used with one or more
sources as well to have different frequency responses depending on the source or if a DC voltage needs to be blocked
from a source.
due to the internal shutdown resistor can be found by Equation (1) below.
(VSD - GND) / 300kΩ
(1)
With only a 0.5V difference, an additional 1.7µA of current will
be drawn while in the shutdown state.
PROPER SELECTION OF EXTERNAL COMPONENTS
The gain of the LM4673 is set by the external resistors, Ri in
Figure 1, The Gain is given by Equation (2) below. Best THD
+N performance is achieved with a gain of 2V/V (6dB).
AV = 2 * 150 kΩ / Ri (V/V)
(2)
It is recommended that resistors with 1% tolerance or better
be used to set the gain of the LM4673. The Ri resistors should
be placed close to the input pins of the LM4673. Keeping the
input traces close to each other and of the same length in a
high noise environment will aid in noise rejection due to the
good CMRR of the LM4673. Noise coupled onto input traces
which are physically close to each other will be common mode
and easily rejected by the LM4673.
Input capacitors may be needed for some applications or
when the source is single-ended (see Figures 3, 5). Input capacitors are needed to block any DC voltage at the source so
that the DC voltage seen between the input terminals of the
LM4673 is 0V. Input capacitors create a high-pass filter with
the input resistors, Ri. The –3dB point of the high-pass filter
is found using Equation (3) below.
fC = 1 / (2πRi Ci ) (Hz)
SINGLE-ENDED CIRCUIT CONFIGURATIONS
The LM4673 can also be used with single-ended sources but
input capacitors will be needed to block any DC at the input
terminals. Figure 5 shows the typical single-ended application
configuration. The equations for Gain, Equation (2), and frequency response, Equation (3), hold for the single-ended
configuration as shown in Figure 5.
When using more than one single-ended source as shown in
Figure 6, the impedance seen from each input terminal should
be equal. To find the correct values for Ci3 and Ri3 connected
to the +IN input pin the equivalent impedance of all the singleended sources are calculated. The single-ended sources are
in parallel to each other. The equivalent capacitor and resistor, Ci3 and Ri3, are found by calculating the parallel combination of all Civalues and then all Ri values. Equations (4) and
(5) below are for any number of single-ended sources.
(3)
The input capacitors may also be used to remove low audio
frequencies. Small speakers cannot reproduce low bass frequencies so filtering may be desired . When the LM4673 is
using a single-ended source, power supply noise on the
ground is seen as an input signal by the +IN input pin that is
capacitor coupled to ground (See Figures 5 – 7). Setting the
high-pass filter point above the power supply noise frequencies, 217Hz in a GSM phone, for example, will filter out this
noise so it is not amplified and heard on the output. Capacitors
with a tolerance of 10% or better are recommended for
impedance matching.
(4)
Ri3 = 1 / (1/Ri1 + 1/Ri2 + 1/Rin ...) (Ω)
(5)
The LM4673 may also use a combination of single-ended and
differential sources. A typical application with one single-ended source and one differential source is shown in Figure 7.
Using the principle of superposition, the external component
values can be determined with the above equations corresponding to the configuration.
DIFFERENTIAL CIRCUIT CONFIGURATIONS
The LM4673 can be used in many different circuit configurations. The simplest and best performing is the DC coupled,
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Ci3 = Ci1 + Ci2 + Cin ... (F)
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LM4673
20152222
FIGURE 2. Differential Input Configuration
20152223
FIGURE 3. Differential Input Configuration with Input Capacitors
13
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LM4673
20152224
FIGURE 4. Dual Differential Input Configuration
20152225
FIGURE 5. Single-Ended Input Configuration
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LM4673
20152226
FIGURE 6. Dual Single-Ended Input Configuration
20152227
FIGURE 7. Dual Input with a Single-Ended Input and a Differential Input
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LM4673
REFERENCE DESIGN BOARD SCHEMATIC
20152228
FIGURE 8.
The commonly used Audio Precision analyzer is differential,
but its ability to accurately reject high frequency signals is
questionable necessitating the on board measurement filter.
When in doubt or when the signal needs to be single-ended,
use an audio signal transformer to convert the differential output to a single ended output. Depending on the audio
transformer's characteristics, there may be some attenuation
of the audio signal which needs to be taken into account for
correct measurement of performance.
In addition to the minimal parts required for the application
circuit, a measurement filter is provided on the evaluation circuit board so that conventional audio measurements can be
conveniently made without additional equipment. This is a
balanced input, grounded differential output low pass filter
with a 3dB frequency of approximately 35kHz and an on board
termination resistor of 300Ω (see schematic). Note that the
capacitive load elements are returned to ground. This is not
optimal for common mode rejection purposes, but due to the
independent pulse format at each output there is a significant
amount of high frequency common mode component on the
outputs. The grounded capacitive filter elements attenuate
this component at the board to reduce the high frequency
CMRR requirement placed on the analysis instruments.
Measurements made at the output of the measurement filter
suffer attenuation relative to the primary, unfiltered outputs
even at audio frequencies. This is due to the resistance of the
inductors interacting with the termination resistor (300Ω) and
is typically about -0.25dB (3%). In other words, the voltage
levels (and corresponding power levels) indicated through the
measurement filter are slightly lower than those that actually
occur at the load placed on the unfiltered outputs. This small
loss in the filter for measurement gives a lower output power
reading than what is really occurring on the unfiltered outputs
and its load.
Even with the grounded filter the audio signal is still differential, necessitating a differential input on any analysis instrument connected to it. Most lab instruments that feature BNC
connectors on their inputs are NOT differential responding
because the ring of the BNC is usually grounded.
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LM4673
LM4673SD Demo Board Artwork
Top Silkscreen
Top Layer
20152234
20152235
Composite View
Internal Layer 1
20152232
20152231
Internal Layer 2
Bottom Silkscreen
20152233
20152230
17
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LM4673
Bottom Layer
20152229
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LM4673
LM4673TM Demo Board Artwork
Top Silkscreen
Top Layer
20152263
20152264
Composite View
Internal Layer 1
20152261
20152260
Internal Layer 2
Bottom Silkscreen
20152259
20152262
19
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LM4673
Bottom Layer
20152258
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LM4673
Revision History
Rev
Date
Description
1.0
12/16/05
Initial WEB released.
1.1
02/28/06
Taken out “Future Product”, then re-WEBd
the datasheet.
1.2
04/06/06
Added the TM and SD demo boards, then
released to the WEB (per Royce).
1.3
11/01/07
Deleted a sentence under the SHUTDOWN
FUNCTION section.
21
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LM4673
Physical Dimensions inches (millimeters) unless otherwise noted
9 Bump micro SMD
Order Number LM4673TM
NS Package Number TMD09GGA
X1 = 1.405 X2 = 1.405 X3 = 0.600
LLP
Order Number LM4673SD
NS Package Number SDA08A
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LM4673
Notes
23
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LM4673 Filterless, 2.65W, Mono, Class D Audio Power Amplifier
Notes
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