NSC LM4870

LM4870
1.1W Audio Power Amplifier with Shutdown Mode
General Description
Key Specifications
The LM4870 is a bridge-connected audio power amplifier capable of delivering 1.1W of continuous average power to an
8Ω load with less than 0.5% THD+N over the audio spectrum
from a 5V power supply.
Boomer audio power amplifiers were designed specifically to
provide high quality output power with a minimal number of
external components. Since the LM4870 does not require
output coupling capacitors, bootstrap capacitors or snubber
networks, it is optimally suited for low-power portable systems.
The LM4870 features an externally controlled, low-power
consumption shutdown mode, as well as an internal thermal
shutdown protection mechanism. It also includes two headphone control inputs and a headphone sense output for external monitoring. The LM4870 is unity-gain stable and the
gain is set using external resistors.
Typical Application
n THD+N at 1W into 8Ω
0.5% (max)
n Output power into 8Ω at 1kHz
at 10%THD+N
1.5W (typ)
n Shutdown Current
0.6µA (typ)
Features
n No output coupling capacitors, bootstrap capacitors, or
snubber circuits are necessary
n Small Outline (SOIC) power packaging
n Unity-gain stable
n External gain configuration capability
Applications
n Personal computers
n Desktop computers
n Low voltage audio system
Connection Diagram
Small Outline Package
DS100094-2
Top View
Order Number LM4870M
See NS Package Number M16A
DS100094-1
FIGURE 1. Typical Audio Amplifier Application Circuit
Boomer ® is a registered trademark of National Semiconductor Corporation.
© 1999 National Semiconductor Corporation
DS100094
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LM4870 1.1W Audio Power Amplifier with Shutdown Mode
October 1997
Absolute Maximum Ratings (Note 2)
Infrared (15 sec.)
220˚C
Thermal Resistance
35˚C/W
φJC(typ)
100˚C/W
φJA(typ)
See AN-450 “Surface Mounting and their Effects on Product
Reliability” for other methods of soldering surface mount devices.
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
ESD Susceptibility (Note 4)
ESD Susceptibility (Note 5)
Junction Temperature
Soldering Information
Small Outline Package
Vapor Phase (60 sec.)
6.0V
−65˚C to +150˚C
−0.3V to VDD + 0.3V
Internally limited
3000V
250V
150˚C
Operating Ratings
Temperature Range
TMIN ≤ TA ≤ TMAX
Supply Voltage
−20˚C ≤ TA ≤ +85˚C
2.0V ≤ VDD ≤ 5.5V
215˚C
Electrical Characteristics
(Notes 1, 2) The following specifications apply for VDD = 5V, RL = 8Ω unless otherwise specified. Limits apply for TA = 25˚C.
Symbol
VDD
Parameter
Conditions
LM4870
Typical
Limit
(Note 6)
(Note 7)
Supply Voltage
IDD
Quiescent Power Supply Current
ISD
Shutdown Current
VOS
Output Offset Voltage
PO
Output Power
THD+N
Total Harmonic Distortion + Noise
PSRR
Power Supply Rejection Ratio
Vod
Output Dropout Voltage
VIH
HP-IN High Input Voltage
VIL
HP-IN Low Input Voltage
VOH
VOL
VO = 0V, IO = 0A
Vpin2 = VDD
VIN = 0V
THD+N = 0.5% (max); f = 1 kHz
PO = 1 Wrms; 20 Hz ≤ f ≤ 20 kHz
VDD = 4.9V to 5.1V
Units
(Limits)
2.0
V (min)
5.5
V (max)
15.0
mA (max)
10
50.0
mV (max)
1.1
1.0
W (min)
7.0
0.4
µA
0.25
%
60
dB
HP-SENSE High Output Voltage
VIN = 0V to 5V
HP-SENSE = 0V to 4V
HP-SENSE = 4V to 0V
IO = 500 µA
2.8
2.5
V (min)
HP-SENSE Low Output Voltage
IO = −500 µA
0.2
0.8
V (max)
0.6
1.0
2.5
V (max)
V
2.5
V
Note 1: All voltages are measured with respect to the ground pins, 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 − T A)/θJA or the number given in the Absolute Maximum Ratings, whichever is lower. For the LM4870, TJMAX =
+150˚C, and the typical junction-to-ambient thermal resistance, when board mounted, is 100˚C/W.
Note 4: Human body model, 100 pF discharged through a 1.5 kΩ resistor.
Note 5: Machine Model, 200 pF–240 pF 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).
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External Components Description
(Figure 1)
Components
Functional Description
1.
Ri
Inverting input resistance which sets the closed-loop gain in conjunction with Rf. This resistor also
forms a high pass filter with Ci at fC = 1/(2π Ri Ci).
2.
Ci
Input coupling capacitor which blocks DC voltage at the amplifier’s input terminals. Also creates a
highpass filter with Ri at fC = 1/(2π Ri Ci).
3.
Rf
Feedback resistance which sets closed-loop gain in conjunction with Ri.
4.
CS
Supply bypass capacitor which provides power supply filtering. Refer to the Application Information
section for proper placement and selection of supply bypass capacitor.
5.
CB
Bypass pin capacitor which provides half supply filtering. Refer to Application Information section for
proper placement and selection of bypass capacitor.
Typical Performance Characteristics
THD+N vs Frequency
THD+N vs Frequency
DS100094-9
THD+N vs Output Power
THD+N vs Frequency
DS100094-10
THD+N vs Output Power
DS100094-12
Supply Current vs
Supply Voltage
DS100094-11
THD+N vs Output Power
DS100094-13
DS100094-14
LM4870 Noise Floor
vs Frequency
Power Derating Curve
DS100094-17
DS100094-18
DS100094-16
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Typical Performance Characteristics
Supply Current Distribution
vs Temperature
(Continued)
Power Dissipation
vs Output Power
DS100094-19
Output Power vs
Supply Voltage
Output Power vs
Load Resistance
DS100094-20
Output Power vs
Supply Voltage
DS100094-21
Open Loop
Frequency Response
DS100094-22
DS100094-27
DS100094-23
Power Supply
Rejection Ratio
DS100094-24
Application Information
By driving the load differentially through outputs VO1 and
VO2, an amplifier configuration commonly referred to as
“bridged mode” is established. Bridged mode operation is
different from the classical single-ended amplifier configuration where one side of its load is connected to ground.
A bridge amplifier design has a few distinct advantages over
the single-ended configuration, as it provides differential
drive to the load, thus doubling output swing for a specified
supply voltage. Consequently, four times the output power is
possible as compared to 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 caus-
BRIDGE CONFIGURATION EXPLANATION
As shown in Figure 1, the LM4870 has two operational amplifiers internally, allowing for a few different amplifier configurations. The first amplifier’s gain is externally configurable, while the second amplifier is internally fixed in a
unity-gain, inverting configuration. The closed-loop gain of
the first amplifier is set by selecting the ratio of Rf to R i while
the second amplifier’s gain is fixed by the two internal 40 kΩ
resistors. Figure 1 shows that the output of amplifier one
serves as the input to amplifier two which results in both amplifiers producing signals identical in magnitude, but out of
phase 180˚. Consequently, the differential gain for the IC is:
Avd = 2 * (Rf/Ri)
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Application Information
bypass capacitors, especially CB, is thus dependant upon
desired low frequency THD+N, system cost, and size constraints.
(Continued)
ing excessive clipping which will damage high frequency
transducers used in loudspeaker systems, please refer to
the Audio Power Amplifier Deslgn section.
A bridge configuration, such as the one used in Boomer Audio Power Amplifiers, 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 eliminates the need for an output coupling capacitor which is required in a single supply,
single-ended amplifier configuration. Without a large output
coupling capacitor in a single supply single-ended amplifier,
the half-supply bias across the load would result in both increased internal IC power dissipation.
SHUTDOWN FUNCTION
In order to reduce power consumption while not in use, the
LM4870 contains a shutdown pin to externally turn off the
amplifier’s bias circuitry. The shutdown feature turns the amplifier off when a logic high is placed on the shutdown pin.
Upon going into shutdown, the output is immediately disconnected from the speaker. There is a built-in threshold which
produces a drop in quiescent current to 500 µA typically. For
a 5V power supply, this threshold occurs when 2V–3V is applied to the shutdown pin. A typical quiescent current of
0.6 µA results when the supply voltage is applied to the shutdown pin. In many applications, a microcontroller or microprocessor output is used to control the shutdown circuitry
which provides a quick, smooth transition into shutdown. Another solution is to use a single-pole, single-throw switch that
when closed, is connected to ground and enables the amplifier. If the switch is open, then a soft pull-up resistor of 47 kΩ
will disable the LM4870. There are no soft pull-down resistors inside the LM4870, so a definite shutdown pin voltage
must be applied externally, or the internal logic gate will be
left floating which could disable the amplifier unexpectedly.
POWER DISSIPATION
Power dissipation is a major concern when designing a successful amplifier, whether the amplifier is bridged or
single-ended. A direct consequence of the increased power
delivered to the load by a bridge amplifier is an increase in
internal power dissipation. Equation 1 states the maximum
power dissipation point for a bridge amplifier operating at a
given supply voltage and driving a specified output load.
PDMAX = 4 * (VDD) 2/(2π2RL)
(1)
Since the LM4870 has two operational amplifiers in one
package, the maximum internal power dissipation is 4 times
that of a single-ended amplifier. Even with this substantial increase in power dissipation, the LM4870 does not require
heatsinking. From Equation 1, assuming a 5V power supply
and an 8Ω load, the maximum power dissipation point is 625
mW. The maximum power dissipation point obtained from
Equation 1 must not be greater than the power dissipation
that results from Equation 2:
PDMAX = (TJMAX − T A)/θJA
(2)
For the LM4870 surface mount package, θJA = 100˚C/W and
TJMAX = 150˚C. Depending on the ambient temperature, TA,
of the system surroundings, Equation 2 can be used to find
the maximum internal power dissipation supported by the IC
packaging. If the result of Equation 1 is greater than that of
Equation 2, then either the supply voltage must be decreased or the load impedance increased. 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 88˚C, provided that device operation is around the maximum power
dissipation point. Power dissipation is a function of output
power and thus, if typical operation is not around the maximum power dissipation point, the ambient temperature can
be increased. Refer to the Typical Performance Characteristics curves for power dissipation information for lower output powers.
HEADPHONE CONTROL INPUTS
The LM4870 possesses two headphone control inputs that
disable the amplifier and reduce IDD to less than 1 mA when
either one or both of these inputs have a logic-high voltage
placed on their pins.
Unlike the shutdown function, the headphone control function does not provide the level of current conservation that is
required for battery powered systems. Since the quiescent
current resulting from the headphone control function is
1000 times more than the shutdown function, the residual
currents in the device may create a pop at the output when
coming out of the headphone control mode. The pop effect
may be eliminated by connecting the headphone sensing
output to the shutdown pin input as shown in Figure 2. This
solution will not only eliminate the output pop, but will also
utilize the full current conservation of the shutdown function
by reducing IDD to 0.6 µA. The amplifier will then be fully
shutdown. This configuration also allows the designer to use
the control inputs as either two headphone control pins or a
headphone control pin and a shutdown pin where the lowest
level of current consumption is obtained from either function.
Figure 3 shows the implementation of the LM4870’s headphone control function using a single-supply headphone amplifier. The voltage divider of R1 and R2 sets the voltage at
the HP-IN1 pin to be approximately 50 mV when there are
no headphones plugged into the system. This logic-low voltage at the HP-IN1 pin enables the LM4870 to amplify AC signals. Resistor R3 limits the amount of current flowing out of
the HP-IN1 pin when the voltage at that pin goes below
ground resulting from the music coming from the headphone
amplifier. The output coupling cap protects the headphones
by blocking the amplifier’s half-supply DC voltage. The capacitor also protects the headphone amplifier from the low
voltage set up by resistors R1 and R2 when there aren’t any
headphones plugged into the system. The tricky point to this
setup is that the AC output voltage of the headphone amplifier cannot exceed the 2.0V HP-IN1 voltage threshold when
there aren’t any headphones plugged into the system, assuming that R1 and R2 are 100k and 1k, respectively. The
LM4870 may not be fully shutdown when this level is ex-
POWER SUPPLY BYPASSING
As with any power amplifier, proper supply bypassing is critical for low noise performance and high power supply rejection. The capacitor location on both the bypass and power
supply pins should be as close to the device as possible. As
displayed in the Typical Performance CharacterIstIcs section, the effect of a larger half-supply bypass capacitor is improved low frequency THD+N due to increased half-supply
stability. Typical applications employ a 5V regulator with
a10 µF tantalum and a 0.1 µF film bypass capacitors which
aid in supply stability, but do not eliminate the need for bypassing the supply nodes of the LM4870. The selection of
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Application Information
In addition, the HP-SENSE pin, although it may be connected to the SHUTDOWN pin as shown in Figure 2, may
still be used as a control flag. It is capable of driving the input
to another logic gate or approximately 2 mA without serious
loading.
(Continued)
ceeded momentarily, due to the discharging time constant of
the bias-pin voltage. This time constant is established by the
two 50k resistors (in parallel) with the series bypass capacitor value.
When a set of headphones are plugged into the system, the
contact pin of the headphone jack is disconnected from the
signal pin, interrupting the voltage divider set up by resistors
R1 and R2. Resistor R1 then pulls up the HP-IN1 pin, enabling the headphone function and disabling the LM4870
amplifier. The headphone amplifier then drives the headphones, whose impedance is in parallel with resistor R2.
Since the typical impedance of headphones are 32Ω, resistor R2 has negligible effect on the output drive capability.
Also shown in Figure 3 are the electrical connections for the
headphone jack and plug. A 3-wire plug consists of a Tip,
Ring, and Sleave, where the Tip and Ring are signal carrying
conductors and the Sleave is the common ground return.
One control pin contact for each headphone jack is sufficient
to indicate to control inputs that the user has inserted a plug
into a jack and that another mode of operation is desired.
For a system implementation where the headphone amplifier
is designed using a split supply, the output coupling cap, CC
and resistor R2 of Figure 3, can be eliminated. The functionality described earlier remains the same, however.
DS100094-7
FIGURE 2. HP-SENSE Pin to
SHUTDOWN Pin Connection
DS100094-8
FIGURE 3. Typical Headphone Control Input Circuitry
AUDIO POWER AMPLIFIER DESIGN
Input Impedance:
20 kΩ
Bandwidth: 100 Hz-20 kHz ± 0.25 dB
A designer must first determine the needed supply rail to obtain the specified output power. The Output Power vs Supply
Voltage graphs in the Typical Performance Characteristics section show how much power the LM4870 will output
given different supply voltage. According to the graph, 4.6V
Design a 500 mW/8Ω Audio Amplifier
Given:
Power Output: 1.0Wrms
Load Impedance: 8Ω
Input Level: 1 Vrms(max)
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Application Information
put (Ri) resistor is 1.5:1. If Ri is set to the required input impedance of 20 kΩ, then Rf = 30 kΩ. The final design step is
to address the bandwidth requirements which must be
stated as a pair of −3 dB frequency points. Five times away
from a −3 dB point is 0.17 dB down from passband response
which is better than the required ± 0.25 dB specified.
fL = 100 Hz/5 = 20 Hz
fH = 20 kHz5 = 100 HzAs stated in the External Components section, Ri in conjunction with Ci create a highpass
filter.
Ci ≥ 1/(2π * 20 kΩ * 20 Hz) = 0.397 µF; use 0.39 µF.
(Continued)
are required for 1.0W of output power. Since 5V rails are
common, it is chosen to be the supply voltage. Supply voltage (up to a maximum of 5.5V) above the required 4.6V will
allow the LM4870 to reproduce transient signals at greater
than 1.0W of output power. The extra voltage will also increase the device power dissipation, so the designer must
make sure that the conditions explained in the Power Dissipationsection are not violated.
Once the power dissipation issues have been addressed,
the required differential gain can be determined from Equation 4:
From equation 4, the minimum Avd is A
3.
vd
The high frequency pole is determined by the product of the
desired high frequency pole, fH, and the differential gain, A
vd. With a Avd = 3 and fH = 100 kHz, the resulting GBWP =
150 kHz which is much smaller than the LM4870 GBWP of
4 MHz. This figure displays that if a designer has a need to
design an amplifier with a higher differential gain, the
LM4870 can still be used without running into bandwidth
problems.
= 2.83; use Avd =
Since the amplifier output is bridged, giving a gain of 2, and
the desired system gain is 3, the ratio of feedback (Rf) to in-
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LM4870 1.1W Audio Power Amplifier with Shutdown Mode
Physical Dimensions
inches (millimeters) unless otherwise noted
Small Outline Package (M)
Order Number LM4870M
NS Package Number M16A
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