Datasheet LM4952 Datasheet (National Semiconductor)

LM4952
3.1W Stereo-SE Audio Power Amplifier with DC Volume Control
August 2004
LM4952 3.1W Stereo-SE Stereo Audio Power Amplifier
with DC Volume Control

General Description

The LM4952 is a dual audio power amplifier primarily de­signed for demanding applications in flat panel monitors and TV’s. It is capable of delivering 3.1 watts per channel to a 4 single-ended load with less than 1% THD+N when powered by a 12V
Eliminating external feedback resistors, an internal, DC­controlled, volume control allows easy and variable gain adjustment.
Boomer audio power amplifiers were designed specifically to provide high quality output power with a minimal amount of external components. The LM4952 does not require boot­strap capacitors or snubber circuits. Therefore, it is ideally suited for display applications requiring high power and mini­mal size.
The LM4952 features a low-power consumption active-low shutdown mode. Additionally, the LM4952 features an inter­nal thermal shutdown protection mechanism along with short circuit protection.
The LM4952 contains advanced pop & click circuitry that eliminates noises which would otherwise occur during turn-on and turn-off transitions.
power supply.
DC

Connection Diagram

Key Specifications

j
Quiscent Power Supply Current 18mA (typ)
j
P
OUT
VDD= 12V, RL=4Ω, 10% THD+N 3.8W (typ)
j
Shutdown current 55µA (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 3.8W output, R n DC-controlled volume control n Short circuit protection
L
=4

Applications

n Flat Panel Monitors n Flat panel TV’s n Computer Sound Cards
Top View
Order Number LM4952TS
See NS Package Number TS9A
U = Wafer Fab Code
Z = Assembly Plant Code
XY = Date Coce
TT = Die Traceability
L4952TS = LM4952TS
Boomer®is a registered trademark of National Semiconductor Corporation.
© 2004 National Semiconductor Corporation DS200809 www.national.com
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Typical Application

LM4952

FIGURE 1. Typical LM4952 SE Audio Amplifier Application Circuit

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LM4952

Absolute Maximum Ratings (Notes 1, 2)

If Military/Aerospace specified devices are required, please contact the National Semiconductor Sales Office/ Distributors for availability and specifications.
Supply Voltage (pin 6, referenced to GND, pins 4 and 5) 18.0V
Storage Temperature −65˚C to +150˚C
Input Voltage
pins 4, 6, and 7 −0.3V to V
pins 1, 2, 3, 8, and 9 −0.3V to 9.5V
Power Dissipation (Note 3) Internally limited
DD
+ 0.3V
ESD Susceptibility (Note 5) 200V
Junction Temperature 150˚C
Thermal Resistance
θ
(TS) 4˚C/W
JC
θ
(TS) (Note 3) 20˚C/W
JA

Operating Ratings

Temperature Range
T
TA≤ T
MIN
MAX
Supply Voltage 9.6V V
−40˚C TA≤ 85˚C
16V
DD
ESD Susceptibility (Note 4) 2000V
Electrical Characteristics VDD= 12V (Notes 1, 2)
The following specifications apply for VDD= 12V, AV= 20dB (nominal), RL=4Ω, and TA= 25˚C unless otherwise noted.
Symbol Parameter Conditions LM4952 Units
Typical
(Note 6)
I
DD
I
SD
R
IN
V
IN
V
SDIH
V
SDIL
T
WU
Quiescent Power Supply Current VIN= 0V, IO= 0A, No Load 18 35 mA (max)
Shutdown Current V
Amplifier Input Resistance V
SHUTDOWN
DC VOL=VDD
V
DC VOL
= GND (Note 9) 55 85 µA (max)
/2 44 k
= GND 200 k
Amplifier Input Signal VDD/2 V
Shutdown Voltage Input High 2.0
Shutdown Voltage Input Low 0.4 V (max)
Wake-up Time CB= 4.7µF 440 ms
Limit
(Notes 7, 8)
V
DD
TSD Thermal Shutdown Temperature 170 ˚C
P
O
THD+N Total Harmomic Distortion + Noise P
e
OS
X
TALK
Output Power f = 1kHz,
THD+N = 1% THD+N = 10%
= 2.0Wrms, f = 1kHz 0.08 %
O
Output Noise A-Weighted Filter, VIN= 0V,
Input Referred
Channel Separation fIN= 1kHz, PO= 1W,
3.1
2.8 W (min)
3.8
V
Input Referred
78 72 dB
89 80 dB (min)
PSRR Power Supply Rejection Ratio V
I
OL
Output Current Limit VIN= 0V, RL= 500m 5A
=8
R
L
=4
R
L
= 200mV
RIPPLE
Input Referred
, f = 1kHz,
p-p
(Limits)
p-p
V (min)
/2
V (max)
(max)
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Electrical Characteristics for Volume Control (Notes 1, 2)
The following specifications apply for VDD= 12V, AV= 20dB (nominal), and TA= 25˚C unless otherwise noted.
LM4952
LM4952
Symbol Parameter Conditions
VOL
VOL
A
M
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 area.
Note 4: Human body model, 100pF discharged through a 1.5kresistor.
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.
Gain V
max
Gain V
min
Mute Attenuation V
=(T
DMAX
= 12V, RL=4Ω stereo operation the total power dissipation is 3.65W. θJA= 20˚C/W for the TO263 package mounted to 16in2heatsink surface
DD
JMAX−TA
= Full scale, No Load 20 dB
DC-VOL
= +1LSB, No Load -46 dB
DC-VOL
= 0V, No Load 75 63 dB (min)
DC-VOL
, θJA, and the ambient temperature, TA. The maximum
)/θJAor the given in Absolute Maximum Ratings, whichever is lower. For the LM4952 typical application (shown
JMAX
Typical
(Note 6)
Limit
(Note 7)

External Components Description Refer to Figure 1

Units
(Limits)
Components Functional Description
This is the input coupling capacitor. It blocks DC voltage at the amplifier’s inverting input. CINand R
1. C
IN
create a highpass filter. The filter’s cutoff frequency is fC=1/(2πRINCIN). Refer to the SELECTING EXTERNAL COMPONENTS, for an explanation of determining C
2. C
S
The supply bypass capacitor. Refer to the POWER SUPPLY BYPASSING section for information 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,
3. C
BYPASS
SELECTING EXTERNAL COMPONENTS, for information about properly placing, and selecting the value of, this capacitor.
’s value.
IN
IN
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LM4952

Typical Performance Characteristics A

THD+N vs Frequency THD+N vs Frequency
VDD= 12V, RL=4Ω,
= 2W, CIN= 1.0µF
P
OUT
THD+N vs Output Power THD+N vs Output Power
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= 20dB and TA= 25˚C, unless otherwise noted.
V
VDD= 12V, RL=8Ω,
= 1W, CIN= 1.0µF
P
OUT
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VDD= 12V, RL=4Ω,
= 1kHz
f
IN
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VDD= 12V, RL=8Ω,
= 1kHz
f
IN
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Typical Performance Characteristics A
(Continued)
LM4952
Output Power vs Power Supply Voltage Output Power vs Power Supply Voltage
= 20dB and TA= 25˚C, unless otherwise noted.
V
RL=4Ω,fIN= 1kHz
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both channels driven and loaded (average shown),
at (from top to bottom at 12V):
both channels driven and loaded (average shown),
RL=8Ω,fIN= 1kHz
at (from top to bottom at 12V):
THD+N = 10%, THD+N = 1%
THD+N = 10%, THD+N = 1%
Power Supply Rejection vs Frequency Total Power Dissipation vs Load Dissipation
VDD= 12V, fIN= 1kHz,
at (from top to bottom at 1W):
=4Ω,RL=8
R
L
VDD= 12V, RL=4Ω,
RIPPLE
= 200mV
p-p
V
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Output Power vs Load Resistance Channel-to-Channel Crosstalk vs Frequency
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VDD= 12V, fIN= 1kHz,
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at (from top to bottom at 15):
THD+N = 10%, THD+N = 1%
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VDD= 12V, RL=4Ω,P
= 1W, Input Referred
OUT
at (from top to bottom at 1kHz): V
V
OUTA
measured, V
driven, V
INA
OUTB
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driven,
INB
measured
LM4952
Typical Performance Characteristics A
= 20dB and TA= 25˚C, unless otherwise noted.
V
(Continued)
Channel-to-Channel Crosstalk vs Frequency Amplifier Gain vs DC Volume Voltage
VDD= 12V, RL=8Ω,P
= 1W, Input Referred
OUT
at (from top to bottom at 1kHz): V
V
OUTA
measured, V
INA
driven, V
OUTB
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driven,
INB
measured
VDD= 12V, RL=8Ω, at (from top to bottom at 1.5V):
Decreasing DC Volume Voltage, Increasing DC Volume
Voltage
Amplifier Gain vs Part-to-Part DC Volume Voltage
Variation (Five parts) THD+N vs Frequency
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VDD= 12V, RL=8Ω,
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VDD= 9.6V, RL=4Ω,
= 1.1W, CIN= 1.0µF
P
OUT
THD+N vs Frequency THD+N vs Output Power
VDD= 9.6V, RL=8Ω,
= 850mW, CIN= 1.0µF
P
OUT
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VDD= 9.6V, RL=4Ω,
= 1kHz
f
IN
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Typical Performance Characteristics A
(Continued)
LM4952
THD+N vs Output Power Total Power Dissipation vs Load Dissipation
= 20dB and TA= 25˚C, unless otherwise noted.
V
VDD= 9.6V, fIN= 1kHz
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at (from top to bottom at 1W):
=4Ω,RL=8
R
L
VDD= 9.6V, RL=8Ω,
= 1kHz
f
IN
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Output Power vs Load Resistance Power Supply Rejection vs Frequency
VDD= 9.6V, fIN= 1kHz,
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at (from top to bottom at 15):
THD+N = 10%, THD+N = 1%
VDD= 9.6V, RL=4Ω,
RIPPLE
= 200mV
P-P
V
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Channel-to Channel Crosstalk vs Frequency Channel-to Channel Crosstalk vs Frequency
VDD= 9.6V, RL=4Ω,P
= 1W, Input Referred
OUT
at (from top to bottom at 1kHz): V
measured; V
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INA
driven, V
OUTB
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driven, V
INB
measured
OUTA
VDD= 9.6V, RL=8Ω,P
= 1W, Input Referred
OUT
at (from top to bottom at 1kHz): V
measured; V
INA
driven, V
OUTB
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driven, V
INB
measured
OUTA
LM4952
Typical Performance Characteristics A
(Continued)
THD+N vs Frequency THD+N vs Frequency
VDD= 14V, RL=4Ω,
= 2W, CIN= 1.0µF
P
OUT
THD+N vs Output Power THD+N vs Output Power
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= 20dB and TA= 25˚C, unless otherwise noted.
V
VDD= 14V, RL=8Ω,
= 1W, CIN= 1.0µF
P
OUT
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VDD= 14V, RL=4Ω,
= 1kHz
f
IN
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VDD= 14V, RL=8
= 1kHz
f
IN
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Power Supply Rejection vs Frequency Output Power vs Load Resistance
VDD= 15V, fIN= 1kHz,
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at (from top to bottom at 2W):
=4Ω,RL=8
R
L
VDD= 14V, RL=4
RIPPLE
= 200mV
P-P
V
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Typical Performance Characteristics A
(Continued)
LM4952
THD+N vs Output Power THD+N vs Output Power
= 20dB and TA= 25˚C, unless otherwise noted.
V
VDD= 15V, at (from top to bottom at 15):
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THD+N = 10%, THD+N = 1%, f
= 1kHz
IN
VDD= 16V, RL=4Ω,
= 1kHz
f
IN
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Channel-to-Channel Crosstalk vs Frequency Channel-to-Channel Crosstalk vs Frequency
VDD= 16V, RL=4Ω,P
= 1W, Input Referred
OUT
at (from top to bottom at 1kHz): V
measured; V
INA
driven, V
OUTB
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driven, V
INB
measured
OUTA
VDD= 16V, RL=8Ω,P
= 1W, Input Referred
OUT
at (from top to bottom at 1kHz): V
measured; V
INA
driven, V
OUTB
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driven, V
INB
measured
Power Supply Current vs Power Supply Voltage Clipping Voltage vs Power Supply Voltage
OUTA
RL=4Ω,
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= 0V, R
V
IN
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SOURCE
=50
RL=4Ω,fIN= 1kHz
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at (from top to bottom at 12.5V):
positive signal swing, negative signal swing
LM4952
Typical Performance Characteristics A
= 20dB and TA= 25˚C, unless otherwise noted.
V
(Continued)
Clipping Voltage vs Power Supply Voltage Power Dissipation vs Ambient Temperature
RL=8Ω,fIN= 1kHz
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VDD= 12V, RL=4Ω (SE), fIN= 1kHz,
(from to bottom at 80˚C): 16in
area, 8in
2
copper plane heatsink area
2
copper plane heatsink
at (from to bottom at 12.5V):
positive signal swing, negative signal swing
Power Dissipation vs Ambient Temperature
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VDD= 12V, RL=8Ω,fIN= 1kHz,
(from to bottom at 120˚C): 16in
area, 8in
2
copper plane heatsink area
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2
copper plane heatsink
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Application Information

LM4952

HIGH VOLTAGE BOOMER WITH INCREASED OUTPUT POWER

FIGURE 2. Typical LM4952 SE Application Circuit

®
Unlike previous 5V Boomer
amplifiers, the LM4952 is de-
signed to operate over a power supply voltages range of
9.6V to 16V. Operating on a 12V power supply, the LM4952 will deliver 3.8W into a 4SE load with no more than 10% THD+N.

POWER DISSIPATION

Power dissipation is a major concern when designing a successful single-ended or bridged amplifier. Equation (2) states the maximum power dissipation point for a single­ended amplifier operating at a given supply voltage and driving a specified output load.
P
DMAX-SE
=(VDD)2/ (2π2RL): Single Ended (1)
The LM4952’s dissipation is twice the value given by Equa­tion (2) when driving two SE loads. For a 12V supply and two 4SE loads, the LM4952’s dissipation is 1.82W.
The maximum power dissipation point given by Equation (1) must not exceed the power dissipation given by Equation (2):
’=(T
P
DMAX
The LM4952’s T LM4952’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
) / θ
JA
2
. This plane can be split be-
(2)
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tween the top and bottom layers of a two-sided PCB. Con­nect the two layers together under the tab with a 5x5 array of vias. At any given ambient temperature T
, use Equation (2)
A
to find the maximum internal power dissipation supported by the IC packaging. Rearranging Equation (2) and substituting P
DMAX
for P
’ results in Equation (3). This equation gives
DMAX
the maximum ambient temperature that still allows maximum stereo power dissipation without violating the LM4952’s maximum junction temperature.
T
A=TJMAX-PDMAX-SEθJA
(3)
For a typical application with a 12V power supply and an SE 4load, the maximum ambient temperature that allows maximum stereo power dissipation without exceeding the maximum junction temperature is approximately 77˚C for the TS package.
T
JMAX=PDMAX-MONOBTLθJA+TA
(4)
Equation (4) gives the maximum junction temperature
. If the result violates the LM4952’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
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Application Information (Continued)
power dissipation is a function of output power, higher am­bient temperatures are allowed as output power or duty cycle decreases.
If the result of Equation (1) is greater than that of Equation (2), then decrease the supply voltage, increase the load impedance, or reduce the ambient temperature. Further, ensure that speakers rated at a nominal 4do not fall below 3. 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 10µF tantalum bypass capacitance connected between the LM4952’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 LM4952’s power supply pin and ground as short as possible.
. The heat sink can be created using
JA
LM4952
changes. In a system with a microprocessor or a microcon­troller, use a digital output to apply the active-state voltage to the SHUTDOWN pin.
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FIGURE 3. Simple switch and voltage divider
generates shutdown control signal

DC VOLUME CONTROL

The LM4952 has an internal stereo volume control whose setting is a function of the DC voltage applied to the DC VOL input pin.
The LM4952 volume control consists of 31 steps that are individually selected by a variable DC voltage level on the volume control pin. As shown in Figure 4, the range of the steps, controlled by the DC voltage, is 20dB to -46dB.
The gain levels are 1dB/step from 20dB to 14dB, 2dB/step from 14dB to -16dB, 3dB/step from -16dB to -27dB, 4dB/step from -27db to -31dB, 5dB/step from -31dB to -46dB.

BYPASS PIN BYPASSING

Connecting a 4.7µF capacitor, C
, between the BY-
BYPASS
PASS pin and ground improves 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. The selection of bypass capacitor values, especially C
BYPASS
depends on desired PSRR requirements, click and pop per­formance (as explained in the section, SELECTING EXTER-
NAL COMPONENTS), system cost, and size constraints.

MICRO-POWER SHUTDOWN

The LM4952 features an active-low micro-power shutdown mode. When active, the LM4952’s micro-power shutdown feature turns off the amplifier’s bias circuitry, reducing the supply current. The low 55µA 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. Figure 3 shows a simple switch-based circuit that can be used to control the LM4952’s shutdown fucntion. Select normal am­plifier operation by closing the switch. Opening 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
,
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FIGURE 4. Volume control response

Like all volume controls, the LM4952’s internal volume con­trol is set while listening to an amplified signal that is applied to an external speaker. The actual voltage applied to the DC VOL input pin is a result of the volume a listener desires. As such, the volume control is designed for use in a feedback system that includes human ears and preferences. This feedback system operates quite well without the need for accurate gain. The user simply sets the volume to the de­sired level as determined by their ear, without regard to the actual DC voltage that produces the volume. Therefore, the accuracy of the volume control is not critical, as long as volume changes monotonically and step size is small enough to reach a desired volume that is not too loud or too
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Application Information (Continued)
soft. Since the gain is not critical, there may be a volume
LM4952
variation from part-to-part even with the same applied DC volume control voltage. The gain of a given LM4952 can be set with fixed external voltage, but another LM4952 may require a different control voltage to achieve the same gain. Figure 5 is a curve showing the volume variation of five typical LM4952s as the voltage applied to the DC VOL input pin is varied. For gains between –20dB and +16dB, the typical part-to-part variation is typically control voltage.
FIGURE 5. Typical part-to-part gain variation as a
function of DC Vol control voltage

VOLUME CONTROL VOLTAGE GENERATION

Figure 6 shows a simple circuit that can be used to create an adjustable DC control voltage that is applied to the DC Vol input. The 91kseries resistor and the 50kpotentiometer create a voltage divider between the supply voltage, V and GND. The series resistor’s value assumes a 12V power supply voltage. The voltage present at the node between the series resistor and the top of the potentiometer need only be a nominal value of 3.5V and must not exceed 9.5V, as stated in the LM4952’s Absolute Maximum Ratings.
±
1dB for a given
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20080966
FIGURE 6. Typical circuit used for DC voltage volume
control. Capacitor connected to DC VOL pin minimizes
voltage fluctuation when using unregulated supplies
that could cause changes in perceived volume setting

UNREGULATED POWER SUPPLIES AND THE DC VOL CONTROL

As an amplifier’s output power increases, the current that flows from the power supply also increases. If an unregu­lated power supply is used, its output voltage can decrease (“droop” or “sag”) as this current increases. It is not uncom­mon for an unloaded unregulated 15V power supply con­nected to the LM4952 to sag by as much as 2V when the amplifier is drawing 1A to 2A while driving 4stereo loads to full power dissipation. Figure 7 is an oscilloscope photo showing an unregulated power supply’s voltage sag while powering an LM4952 that is driving 4stereo loads. The amplifier’s input is a typical music signal supplied by a CD player. As shown, the sag can be quite significant.
,
DD
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20080968
FIGURE 7. LM4952 operating on an unregulated 12V
(nominal) power supply. Wave forms shown include
(Trace A), V
V
DD
OUT A
(Trace B), V
(Trace C), and
OUT B
the DC voltage applied to the DC VOL pin (Trace D)
This sagging supply voltage presents a potential problem when the voltage that drives the DC Vol pin is derived from the voltage supplied by an unregulated power supply. This is the case for the typical volume control circuit (a 50kpoten­tiometer in series with a 91kresistor) shown in Figure 6. The potentiometer’s wiper is connected to the DC Vol pin. With this circuit, power supply voltage fluctuations will be
Application Information (Continued)
seen by the DC Vol input. Though attenuated by the voltage divider action of the potentiometer and the series resistor, these fluctuations may cause perturbations in the perceived volume. An easy and simple solution that suppresses these perturbations is a 10µF capacitor connected between the DC Vol pin and ground. See the result of this capacitor in Figure
8. This capacitance can also be supplemented with bulk capacitance in the range of 1000µF to 10,000µF connected to the unregulated power supply’s output. Figure 10 shows
20080969
.
DD
how this bulk capacitance minimizes fluctuations on V
FIGURE 8. Same conditions and waveforms as shown
in Figure 7, except that a 10µF capacitor has been
connected between the DC VOL pin and GND (Trace D)
If space constraints preclude the use of a 10µF capacitor connected to the DC Vol pin or large amounts of bulk supply capacitance, or if more resistance to the fluctuations is de­sired, using an LM4040-4.1 voltage reference shown in Fig­ure 9 is recommended. The value of the 91kresistor, already present in the typical volume applications circuit, should be changed to 62k. This sets the LM4040-4.1’s bias current at 125µA when using a nominal 12V supply, well within the range of current needed by this reference.
20080970
FIGURE 10. Same conditions and waveforms as shown
in Figure 8, except that a 4700µF capacitor has been
connected between the V
pin and GND (Trace A)
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.
The amplifier’s input resistance and the input capacitor (C
IN
produce a high pass filter cutoff frequency that is found using Equation (5).
= 1/(2πRINCIN) (5)
F
CIN
As an example when using a speaker with a low frequency limit of 50Hz and based on the LM4952’s 44knominal minimum input resistance, C
0.072µF. The 0.39µF C
INA
, using Equation (5) is
IN
shown in Figure 2 allows the LM4952 to drive high efficiency, full range speaker whose response extends below 30Hz.
Similarly, the output coupling capacitor and the load imped­ance also form a high pass filter. The cutoff frequency formed by these two components is found using Equation (6)
f
COUT
= 1/(2πR
LOADCOUT
) (6)
Expanding on the example above and assuming a nominal speaker impedance of 4, response below 30Hz is assured if the output coupling capacitors have a value, using Equa­tion (6), greater than 1330µF.
LM4952
)
20080967
FIGURE 9. Using an LM4040–4.1 to set the maximum DC volume control voltage and attenuate power supply variations when using unregulated supplies that would
otherwise perturb the volume setting.

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 LM4952 settles to quiescent operation, its value is critical when minimizing turn-on pops. The slower the LM4952’s outputs ramp to their quiescent DC voltage (nomi­nally V
/2), the smaller the turn-on pop. Choosing C
DD
BYPASS
equal to 4.7µF 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.

Routing Input and BYPASS Capacitor Grounds

Optimizing the LM4952’s low distortion performance is easily accomplished by connecting the input signal’s ground refer­ence directly to the TO263’s grounded tab connection. In like
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Application Information (Continued)
manner, the ground lead of the capacitor connected between
LM4952
the BYPASS pin and GND should also be connected to the package’s grounded tab.

OPTIMIZING CLICK AND POP REDUCTION PERFORMANCE

The LM4952 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 final value, the LM4952’s internal amplifiers are muted. Once the voltage at the BYPASS pin reaches V are unmuted.
The gain of the internal amplifiers remains unity until the voltage on the bypass pin reaches V voltage on the bypass pin is stable, the device becomes fully operational and the amplifier outputs are reconnected to their respective output pins.
/4 voltage present at the BYPASS pin ramps to its
DD
/4, the amplifiers
DD
/4. As soon as the
DD
In order eliminate "clicks and pops", all capacitors must be discharged before turn-on. Rapidly switching V
DD
may not 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
and
IN
is applied or the shutdown mode is deactivated. Best perfor­mance is achieved by selecting a C greater than twelve times C
’s value.
IN
BYPASS
value that is

RECOMMENDED PRINTED CIRCUIT BOARD LAYOUT

Figure 9 through Figure 11 show the recommended two­layer PC board layout that is optimized for the TO263­packaged, SE-configured LM4952 and associated external components. These circuits are designed for use with an external 12V supply and 4(min)(SE) speakers.
These circuit boards are easy to use. Apply 12V and ground to the board’s V speaker between the board’s OUT
and GND pads, respectively. Connect a
DD
and OUTBoutputs and
A
respective GND pins.
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Demonstration Board Layout

LM4952
200809F2
FIGURE 11. Recommended TS SE PCB Layout:
Top Silkscreen
200809F4
FIGURE 12. Recommended TS SE PCB Layout:
Top Layer
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Demonstration Board Layout (Continued)
LM4952
FIGURE 13. Recommended TS SE PCB Layout:
200809F3
Bottom Layer
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Physical Dimensions inches (millimeters)

unless otherwise noted
LM4952
Order Number LM4952TS
NS Package Number TS9A
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with DC Volume Control
Notes
LM4952 3.1W Stereo-SE Stereo Audio Power Amplifier
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