NSC LM4752T

LM4752
Stereo 11W Audio Power Amplifier
General Description
The LM4752 is a stereo audio amplifier capable of delivering
11W per channel of continuous average output power to a
4Ω load, or 7W per channel into 8Ω using a single 24V supply at 10% THD+N.
The LM4752 is specifically designed for single supply operation and a low external component count. The gain and bias
resistors are integrated on chip, resulting in a 11W stereo
amplifier in a compact 7 pin TO220 package. High output
power levels at both 20V and 24V supplies and low external
component count offer high value for compact stereo and TV
applications. A simple mute function can be implemented
with the addition of a few external components.
n PO at 10% THD @ 1 kHz into 8Ω bridged TO-263 pkg.
at VCC = 12V 5W (typ)
Features
n
n
n
n
n
n
n
n
Drives 4Ω and 8Ω loads
Internal gain resistors (AV = 34 dB)
Minimum external component requirement
Single supply operation
Internal current limiting
Internal thermal protection
Compact 7 lead TO-220 package
Low cost-per-watt
Applications
Key Specifications
n Output power at 10% THD+N with 1 kHz into 4Ω at V CC
= 24V 11W (typ)
n Output power at 10% THD+N with 1 kHz into 8Ω at V CC
= 24V 7W (typ)
n Closed loop gain 34 dB (typ)
n PO at 10% THD @ 1 kHz into 4Ω Single-ended TO-263
pkg. at VCC = 12V 2.5W (typ)
Typical Application
n
n
n
n
Compact stereos
Stereo TVs
Mini component stereos
Multimedia speakers
Connection Diagram
Plastic Package
DS100039-2
Package Description
Top View
Order Number LM4752T
Package Number TA07B
DS100039-50
DS100039-1
FIGURE 1. Typical Audio Amplifier Application Circuit
© 1999 National Semiconductor Corporation
DS100039
Package Description
Top View
Order Number LM4752TS
Package Number TS07B
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LM4752 Stereo 11W Audio Power Amplifier
February 1999
Absolute Maximum Ratings (Note 2)
Storage Temperature
If Military/Aerospace specified devices are required,
please contact the National Semiconductor Sales Office/
Distributors for availability and specifications.
Supply Voltage
Operating Ratings
Temperature Range
TMIN ≤ TA ≤ TMAX
40V
± 0.7V
Input Voltage
Output Current
−40˚C to 150˚C
−40˚C ≤ TA ≤ +85˚C
Supply Voltage
9V to 32V
Internally Limited
θJC
2˚C/W
62.5W
θJA
79˚C/W
Power Dissipation (Note 3)
ESD Susceptability (Note 4)
2 kV
Junction Temperature
150˚C
Soldering Information
T Package (10 sec)
250˚C
Electrical Characteristics
The following specifications apply to each channel with VCC = 24V, TA = 25˚C unless otherwise specified.
LM4752
Symbol
Itotal
Po
Parameter
Conditions
Total Quiescent Power Supply
Current
VINAC = 0V, Vo = 0V, RL = ∞
Output Power (Continuous
f = 1 kHz, THD+N = 10%, RL = 8Ω
Average per Channel)
f = 1 kHz, THD+N = 10%, RL = 4Ω
THD+N
Total Harmonic Distortion plus
Noise
VOSW
Output Swing
Units
(Limits)
Typical
(Note 5)
Limit
(Note 6)
10.5
20
mA(max)
7
mA(min)
10
W(min)
7
W
VCC = 20V, RL = 8Ω
4
W
VCC = 20V, R
7
W
f = 1 kHz, THD+N = 10%, RL = 4Ω
VS = 12V, TO-263 Pkg.
2.5
W
f = 1 kHz, Po = 1 W/ch, RL = 8Ω
0.08
%
V
L
= 4Ω
RL = 8Ω, V
CC
= 20V
15
RL = 4Ω, V
CC
= 20V
14
V
55
dB
50
dB
Xtalk
Channel Separation
See Figure 1
PSRR
Power Supply Rejection Ratio
See Figure 1
f = 1 kHz, Vo = 4 Vrms, RL = 8Ω
VCC = 22V to 26V, R
L
= 8Ω
VODV
Differential DC Output Offset
Voltage
SR
Slew Rate
2
RIN
Input Impedance
83
kΩ
PBW
Power Bandwidth
3 dB BW at Po = 2.5W, RL = 8Ω
65
kHz
A VCL
Closed Loop Gain (Internally Set)
RL = 8Ω
34
ein
Noise
VINAC = 0V
0.09
IHF-A Weighting Filter, RL = 8Ω
0.4
V(max)
V/µs
33
dB(min)
35
dB(max)
0.2
mVrms
Output Referred
Io
Output Short Circuit Current Limit
VIN = 0.5V, R
L
= 2Ω
2
A(min)
Note 1: All voltages are measured with respect to the GND pin (4), 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: For operating at case temperatures above 25˚C, the device must be derated based on a 150˚C maximum junction temperature and a thermal resistance of
θJC = 2˚C/W (junction to case). Refer to the section Determining the Maximum Power Dissipation in the Application Information section for more information.
Note 4: Human body model, 100 pF discharged through a 1.5 kΩ resistor.
Note 5: Typicals are measured at 25˚C and represent the parametric norm.
Note 6: Limits are guarantees that all parts are tested in production to meet the stated values.
Note 7: The TO-263 Package is not recommended for VS > 16V due to impractical heatsinking limitations.
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Test Circuit
DS100039-36
FIGURE 2. Test Circuit
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Typical Application with Mute
DS100039-3
FIGURE 3. Application with Mute Function
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4
DS100039-4
Equivalent Schematic Diagram
5
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System Application Circuit
DS100039-5
FIGURE 4. Circuit for External Components Description
External Components Description
Components
Function Description
1, 2
Cs
Provides power supply filtering and bypassing.
3, 4
Rsn
Works with Csn to stabilize the output stage from high frequency oscillations.
5, 6
Csn
Works with Rsn to stabilize the output stage from high frequency oscillations.
7
Cb
Provides filtering for the internally generated half-supply bias generator.
8, 9
Ci
Input AC coupling capacitor which blocks DC voltage at the amplifier’s input terminals.
Also creates a high pass filter with fc=1/(2 • π • Rin • Cin).
10, 11
Co
Output AC coupling capacitor which blocks DC voltage at the amplifier’s output terminal.
Creates a high pass filter with fc=1/(2 • π • Rout • Cout).
12, 13
Ri
Voltage control - limits the voltage level to the amplifier’s input terminals.
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Typical Performance Characteristics
THD+N vs Output Power
THD+N vs Output Power
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THD+N vs Output Power
THD+N vs Output Power
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THD+N vs Output Power
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THD+N vs Output Power
THD+N vs Output Power
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THD+N vs Output Power
DS100039-15
THD+N vs Output Power
DS100039-14
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THD+N vs Output Power
DS100039-16
THD+N vs Output Power
DS100039-9
THD+N vs Output Power
DS100039-10
7
DS100039-17
DS100039-11
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Typical Performance Characteristics
(Continued)
THD+N vs Output Power
THD+N vs Output Power
DS100039-38
THD+N vs Output Power
DS100039-39
THD+N vs Output Power
DS100039-41
THD+N vs Output Power
THD+N vs Output Power
THD+N vs Output Power
THD+N vs Output Power
DS100039-40
DS100039-42
DS100039-44
DS100039-43
THD+N vs Output Power
DS100039-45
THD+N vs Output Power
DS100039-47
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THD+N vs Output Power
THD+N vs Output Power
DS100039-48
8
DS100039-46
DS100039-49
Typical Performance Characteristics
Output Power vs Supply Voltage
(Continued)
Output Power vs Supply Voltage
DS100039-18
THD+N vs Frequency
DS100039-19
THD+N vs Frequency
DS100039-21
Channel Separation
Frequency Response
DS100039-20
Frequency Response
DS100039-23
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PSRR vs Frequency
DS100039-24
Supply Current vs
Supply Voltage
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Power Derating Curve
Power Dissipation vs Output Power
DS100039-28
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Power Dissipation vs Output Power
DS100039-29
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Typical Performance Characteristics
Power Dissipation vs Output Power
(Continued)
Power Dissipation vs Output Power
DS100039-51
DS100039-52
differential pair, resulting in an output DC shift towards
V SUPPLY. An R-C timing circuit should be used to limit the
pull-down time such that output “pops” and signal
feedthroughs will be minimized. The pull-down timing is a
function of a number of factors, including the external mute
circuitry, the voltage used to activate the mute, the bias capacitor, the half-supply voltage, and internal resistances
used in the half-supply generator. Table 1 shows a list of recommended values for the external mute circuitry.
Application Information
CAPACITOR SELECTION AND FREQUENCY
RESPONSE
With the LM4752, as in all single supply amplifiers, AC coupling capacitors are used to isolate the DC voltage present at
the inputs (pins 2,6) and outputs (pins 1,7). As mentioned
earlier in the External Components section these capacitors create high-pass filters with their corresponding input/
output impedances. The Typical Application Circuit shown
in Figure 1 shows input and output capacitors of 0.1 µF and
1,000 µF respectively. At the input, with an 83 kΩ typical input resistance, the result is a high pass 3 dB point occurring
at 19 Hz. There is another high pass filter at 39.8 Hz created
with the output load resistance of 4Ω. Careful selection of
these components is necessary to ensure that the desired
frequency response is obtained. The Frequency Response
curves in the Typical Performance Characteristics section
show how different output coupling capacitors affect the low
frequency rolloff.
TABLE 1. Values for Mute Circuit
VMUTE
R2
C1
R3
CB
VCC
5V
10 kΩ 10 kΩ 4.7 µF 360Ω 100 µF 21V–32V
VS
20 kΩ 1.2 kΩ 4.7 µF 180Ω 100 µF 15V–32V
VS
20 kΩ
910Ω
4.7 µF 180Ω
47 µF
22V–32V
OPERATING IN BRIDGE-MODE
Though designed for use as a single-ended amplifier, the
LM4752 can be used to drive a load differentially (bridgemode). Due to the low pin count of the package, only the
non-inverting inputs are available. An inverted signal must
be provided to one of the inputs. This can easily be done with
the use of an inexpensive op-amp configured as a standard
inverting amplifier. An LF353 is a good low-cost choice. Care
must be taken, however, for a bridge-mode amplifier must
theoretically dissipate four times the power of a single-ended
type. The load seen by each amplifier is effectively half that
of the actual load being used, thus an amplifier designed to
drive a 4Ω load in single-ended mode should drive an 8Ω
load when operating in bridge-mode.
APPLICATION CIRCUIT WITH MUTE
With the addition of a few external components, a simple
mute circuit can be implemented, such as the one shown in
Figure 3. This circuit works by externally pulling down the
half supply bias line (pin 5), effectively shutting down the input stage.
When using an external circuit to pull down the bias, care
must be taken to ensure that this line is not pulled down too
quickly, or output “pops” or signal feedthrough may result. If
the bias line is pulled down too quickly, currents induced in
the internal bias resistors will cause a momentary DC voltage to appear across the inputs of each amplifier’s internal
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R1
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Application Information
(Continued)
DS100039-30
FIGURE 5. Bridge-Mode Application
DS100039-31
DS100039-37
FIGURE 6. THD+N vs. POUT for Bridge-Mode Application
UNDERVOLTAGE SHUTDOWN
PREVENTING OSCILLATIONS
With the integration of the feedback and bias resistors onchip, the LM4752 fits into a very compact package. However,
due to the close proximity of the non-inverting input pins to
the corresponding output pins, the inputs should be AC terminated at all times. If the inputs are left floating, the amplifier will have a positive feedback path through high impedance coupling, resulting in a high frequency oscillation. In
most applications, this termination is typically provided by
the previous stage’s source impedance. If the application will
require an external signal, the inputs should be terminated to
ground with a resistance of 50 kΩ or less on the AC side of
the input coupling capacitors.
If the power supply voltage drops below the minimum operating supply voltage, the internal under-voltage detection circuitry pulls down the half-supply bias line, shutting down the
preamp section of the LM4752. Due to the wide operating
supply range of the LM4752, the threshold is set to just under 9V. There may be certain applications where a higher
threshold voltage is desired. One example is a design requiring a high operating supply voltage, with large supply and
bias capacitors, and there is little or no other circuitry connected to the main power supply rail. In this circuit, when the
power is disconnected, the supply and bias capacitors will
discharge at a slower rate, possibly resulting in audible output distortion as the decaying voltage begins to clip the out11
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Application Information
When determining the proper heatsink, the above equation
should be re-written as:
(Continued)
put signal. An external circuit may be used to sense for the
desired threshold, and pull the bias line (pin5) to ground to
disable the input preamp. Figure 7 shows an example of
such a circuit. When the voltage across the zener diode
drops below its threshold, current flow into the base of Q1 is
interrupted. Q2 then turns on, discharging the bias capacitor.
This discharge rate is governed by several factors, including
the bias capacitor value, the bias voltage, and the resistor at
the emitter of Q2. An equation for approximating the value of
the emitter discharge resistor, R, is given below:
θSA ≤ [ (TJ − TA) / PDMAX] − θ
JC
− θCS
TO-263 HEATSINKING
Surface mount applications will be limited by the thermal dissipation properties of printed circuit board area. The TO-263
package is not recommended for surface mount applications
with VS > 16V due to limited printed circuit board area.
There are TO-263 package enhancements, such as clip-on
heatsinks and heatsinks with adhesives, that can be used to
improve performance.
Standard FR-4 single-sided copper clad will have an approximate Thermal resistance (θSA) ranging from:
R = (0.7V) / (CB • (V S / 2) / 0.1s)
Note that this is only a linearized approximation based on a
discharge time of 0.1s. The circuit should be evaluated and
adjusted for each application.
As mentioned earlier in the Application Circuit with Mute
section, when using an external circuit to pull down the bias
line, the rate of discharge will have an effect on the turn-off
induced distortions. Please refer to the Application Circuit
with Mute section for more information.
1.5 x 1.5 in. sq.
20–27˚C/W (TA=28˚C, Sine wave
2 x 2 in. sq.
16–23˚C/W testing, 1 oz. Copper)
The above values for θSA vary widely due to dimensional
proportions (i.e. variations in width and length will vary θSA).
For audio applications, where peak power levels are short in
duration, this part will perform satisfactory with less
heatsinking/copper clad area. As with any high power design
proper bench testing should be undertaken to assure the design can dissipate the required power. Proper bench testing
requires attention to worst case ambient temperature and air
flow. At high power dissipation levels the part will show a tendency to increase saturation voltages, thus limiting the undistorted power levels.
Determining Maximum Power Dissipation
For a single-ended class AB power amplifier, the theoretical
maximum power dissipation point is a function of the supply
voltage, V S, and the load resistance, RL and is given by the
following equation:
(single channel)
PDMAX (W) = [VS 2 / (2 • π2 • RL) ]
The above equation is for a single channel class-AB power
amplifier. For dual amplifiers such as the LM4752, the equation for calculating the total maximum power dissipated is:
(dual channel)
PDMAX (W) = 2 • [V S2 / (2 • π2 • RL) ]
DS100039-32
FIGURE 7. External Undervoltage Pull-Down
THERMAL CONSIDERATIONS
Heat Sinking
Proper heatsinking is necessary to ensure that the amplifier
will function correctly under all operating conditions. A heatsink that is too small will cause the die to heat excessively
and will result in a degraded output signal as the internal
thermal protection circuitry begins to operate.
The choice of a heatsink for a given application is dictated by
several factors: the maximum power the IC needs to dissipate, the worst-case ambient temperature of the circuit, the
junction-to-case thermal resistance, and the maximum junction temperature of the IC. The heat flow approximation
equation used in determining the correct heatsink maximum
thermal resistance is given below:
TJ–TA = P
DMAX
• (θJC + θCS + θ
or
VS2 / (π 2 • RL)
(Bridged Outputs)
PDMAX (W) = 4[VS2 / (2π2 • RL)]
Heatsink Design Example:
Determine the system parameters:
V
= 24V
Operating Supply Voltage
Minimum load impedance
TA = 55˚C
Worst case ambient temperature
Device parameters from the datasheet:
SA)
T
where:
J
= 150˚C
Maximum junction temperature
θJC = 2˚C/W
Junction-to-case thermal resistance
Calculations:
2 • PDMAX = 2 • [V S2 / (2 • π2 • RL) ] = (24V)2 / (2 • π2 •
4Ω) = 14.6W
θSA ≤ [ (TJ − TA) / PDMAX] − θ JC − θCS = [ (150˚C − 55˚C)
/ 14.6W ] − 2˚C/W − 0.2˚C/W = 4.3˚C/W
Conclusion: Choose a heatsink with θSA ≤ 4.3˚C/W.
PDMAX = maximum power dissipation of the IC
TJ(˚C) = junction temperature of the IC
TA(˚C) = ambient temperature
θJC(˚C/W) = junction-to-case thermal resistance of the IC
θCS(˚C/W) = case-to-heatsink thermal resistance (typically
0.2 to 0.5 ˚C/W)
θSA(˚C/W) = thermal resistance of heatsink
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S
RL = 4Ω
12
Application Information
Layout and Ground Returns
Proper PC board layout is essential for good circuit performance. When laying out a PC board for an audio power amplifer, particular attention must be paid to the routing of the
output signal ground returns relative to the input signal and
bias capacitor grounds. To prevent any ground loops, the
ground returns for the output signals should be routed separately and brought together at the supply ground. The input
signal grounds and the bias capacitor ground line should
also be routed separately. The 0.1 µF high frequency supply
bypass capacitor should be placed as close as possible to
the IC.
(Continued)
TO-263 HEATSINK DESIGN EXAMPLES:
Example 1: (Stereo Single-Ended Output)
Given:
TA = 30˚C
TJ = 150˚C
RL = 4Ω
VS = 12V
θJC = 2˚C/W
PDMAX from PD vs PO Graph:
PDMAX ≈ 3.7W
Calculating PDMAX:
PDMAX = VCC2 / (π2RL) = (12V)2 / π2(4Ω)) = 3.65W
Calculating Heatsink Thermal Resistance:
θSA < [(T J − TA) / PDMAX] − θJC − θCS
θSA < 120˚C / 3.7W − 2.0˚C/W − 0.2˚C/W = 30.2˚C/W
Therefore the recommendation is to use 1.5 x 1.5 square
inch of single-sided copper clad.
Example 2: (Stereo Single-Ended Output)
Given:
TA = 50˚C
TJ = 150˚C
RL = 4Ω
VS = 12V
θJC = 2˚C/W
PDMAX from PD vs PO Graph:
PDMAX ≈ 3.7W
Calculating PDMAX:
PDMAX = VCC2 / (π2RL) = (12V)2 / (π2(4Ω)) = 3.65W
Calculating Heatsink Thermal Resistance:
θSA < [(TJ − TA) / PDMAX] − θJC − θCS
θSA < 100˚C / 3.7W − 2.0˚C/W − 0.2˚C/W = 24.8˚C/W
Therefore the recommendation is to use 2.0 x 2.0 square
inch of single-sided copper clad.
Example 3: (Bridged Output)
Given:
TA = 50˚C
TJ = 150˚C
RL = 8Ω
VS = 12V
θJC = 2˚C/W
Calculating PDMAX:
PDMAX = 4[VCC2 / (2π2RL)] = 4(12V)2 / (2π2(8Ω)) = 3.65W
Calculating Heatsink Thermal Resistance:
θSA < [(TJ − TA) / PDMAX] − θJC − θCS
θSA < 100˚C / 3.7W − 2.0˚C/W − 0.2˚C/W = 24.8˚C/W
Therefore the recommendation is to use 2.0 x 2.0 square
inch of single-sided copper clad.
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Application Information
(Continued)
PC BOARD LAYOUT — COMPOSITE
DS100039-33
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Application Information
(Continued)
PC BOARD LAYOUT — SILK SCREEN
DS100039-34
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Application Information
(Continued)
PC BOARD LAYOUT — SOLDER SIDE
DS100039-35
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Physical Dimensions
inches (millimeters) unless otherwise noted
Order Number LM4752T
NS Package Number TA07B
Order Number LM4752TS
NS Package Number TS7B
17
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LM4752 Stereo 11W Audio Power Amplifier
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2. A critical component is any component of a life support
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sonably expected to cause the failure of the life support
the body, or (b) support or sustain life, and whose faildevice or system, or to affect its safety or effectiveness.
ure 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.
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