Datasheet LM4867MTX, LM4867MTEX, LM4867MTE, LM4867MT, LM4867LQX Datasheet (NSC)

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LM4867
Output-Transient-Free Dual 2.1W Audio Amplifier Plus No Coupling Capacitor Stereo Headphone Function
General Description
The LM4867 is a dual bridge-connected audio power ampli­fier which, when connected to a 5V supply, will deliver 2.1W toa4Ωload (Note 1) or 2.4W to a 3load (Note 2) with less than 1.0% THD+N. The LM4867 uses advanced, latest gen­eration circuitry to eliminate all traces of clicks and pops when the supply voltage is first applied. The amplifier has a headphone-amplifier-select input pin. It is used to switch the amplifiers from bridge to single-ended mode for driving headphones. A new circuit topology eliminates headphone output coupling capacitors. A MUX control pin allows selec­tion between the two sets of stereo input signals. The MUX control can also be used to select between two different customer-specified closed-loop responses.
Boomer audio power amplifiers are designed specifically to provide high quality output power from a surface mount package and require few external components. To simplify audio system design, the LM4867 combines dual bridge speaker amplifiers and stereo headphone amplifiers in one package.
The LM4867 features an externally controlled power-saving micropower shutdown mode, a stereo headphone amplifier mode, and thermal shutdown protection.
Note 1: An LM4867LQ or LM4867MTE that has been properly mounted to a circuit board will deliver 2.1W into 4. The Mux control can also be used to select two different closed-loop responses. LM4867MT will deliver 1.1W into 8. See the Application Information sections for further information concern­ing the LM4867LQ and the LM4867MT.
Note 2: An LM4867LQ or LM4867MTE that has been properly mounted to a circuit board and forced-air cooled will deliver 2.4W into 3.
Key Specifications
n POat 1% THD+N n LM4867LQ, 3load 2.4W (typ) n LM4867LQ, 4load 2.1W (typ) n LM4867MTE, 4 1.9W (typ) n LM4867MT, 8 1.1W (typ) n Single-ended mode - THD+N at 75mW into 32 0.5%
(max)
n Shutdown current 0.7µA (typ)
Features
n Advanced “click and pop” suppression circuitry n Eliminates headphone amplifier output coupling
capacitors
n Stereo headphone amplifier mode n Input mux control and two separate inputs per channel n Thermal shutdown protection circuitry n LLP, TSSOP, and exposed-DAP TSSOP packaging
available
Applications
n Multimedia monitors n Portable and desktop computers n Portable audio systems
Typical Application
Boomer®is a registered trademark of National Semiconductor Corporation.
DS200013-31
*
Refer to the Application Information section titled PROPER SELECTION OF EXTERNAL COMPONENTS for details concerning the value of CB.
FIGURE 1. Typical Audio Amplifier Application Circuit
(Pin out shown for the 24-pin Exposed-DAP LLP package. Numbers in ( ) are for the 20-pin MTE and MT
packages.)
February 2001
LM4867 Output-Transient-Free Dual 2.1W Audio Amplifier Plus No Coupling Capacitor Stereo
Headphone Function
© 2001 National Semiconductor Corporation DS200013 www.national.com
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Connection Diagram
Connection Diagram
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Top View
Order Number LM4867MT, LM4867MTE
See NS Package Number MTC20 for TSSOP
See NS Package Number MXA20A for Exposed-DAP TSSOP
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Top View
Order Number LM4867LQ
See NS Package Number LQA24A for Exposed-DAP LLP
LM4867
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Absolute Maximum Ratings (Note 3)
If Military/Aerospace specified devices are required, please contact the National Semiconductor Sales Office/ Distributors for availability and specifications.
Supply Voltage 6.0V Storage Temperature −65˚C to +150˚C Input Voltage −0.3V to V
DD
+0.3V Power Dissipation (Note 4) Internally limited ESD Susceptibility (Note 5)
All pins except Pin 3 (MT, MTE), Pin 2 (LQ) 2000V
Pin 3 (MT, MTE), Pin 2 (LQ) 8000V ESD Susceptibility (Note 6) 200V Junction Temperature 150˚C Solder Information
Small Outline Package
Vapor Phase (60 sec.) 215˚C Infrared (15 sec.) 220˚C
See AN-450 “Surface Mounting and their Effects on Product Reliablilty” for other methods of soldering surface mount devices.
Thermal Resistance
θ
JC
(typ)—MTC20 20˚C/W
θ
JA
(typ)—MTC20 80˚C/W
θ
JC
(typ)—MXA20A 2˚C/W
θ
JA
(typ)—MXA20A 41˚C/W (Note 7)
θ
JA
(typ)—MXA20A 51˚C/W (Note 8)
θ
JA
(typ)—MXA20A 90˚C/W (Note 9)
θ
JC
(typ)—LQA24A 3.0˚C/W
θ
JA
(typ)—LQA24A TBD˚C/W (Note 10)
θ
JA
(typ)—LQA24A TBD˚C/W (Note 11)
θ
JA
(typ)—LQA24A TBD˚C/W (Note 12)
Operating Ratings
Temperature Range
T
MIN
TA≤ T
MAX
−40˚C TA≤ 85˚C
Supply Voltage 2.0V V
DD
5.5V
Electrical Characteristics for Entire IC (Notes 3, 13)
The following specifications apply for VDD= 5V unless otherwise noted. Limits apply for TA= 25˚C.
Symbol Parameter Conditions LM4867 Units
(Limits)
Typical Limit
(Note 14) (Note 15)
V
DD
Supply Voltage 2 V (min)
5.5 V (max)
I
DD
Quiescent Power Supply Current VIN= 0V, IO= 0A (Note 16) , HP-IN = 0V 7.5 15 mA (max)
V
IN
= 0V, IO= 0A (Note 16) , HP-IN = 4V 3.0 6 mA (max)
I
SD
Shutdown Current VDDapplied to the SHUTDOWN pin 0.7 2 µA (max)
Electrical Characteristics for Bridged-Mode Operation (Notes 3, 13)
The following specifications apply for VDD= 5V unless otherwise specified. Limits apply for TA= 25˚C.
Symbol Parameter Conditions LM4867 Units
(Limits)
Typical Limit
(Note 14) (Note 15)
V
OS
Output Offset Voltage VIN= 0V 5 50 mV (max)
P
O
Output Power (Note 17) THD = 1%, f = 1kHz
LM4867MTE, R
L
=3Ω(Note 18) 2.2 W
LM4867LQ, R
L
=3Ω(Note 18) 2.2 W
LM4867MTE, R
L
=4Ω(Note 19) 1.9 W
LM4867LQ, R
L
=4Ω(Note 19) 1.9 W
LM4867, R
L
=8 1.1 1.0 W (min)
THD+N = 10%, f = 1kHz
LM4867MTE, R
L
=3Ω(Note 18) 3.0 W
LM4867LQ, R
L
=3Ω(Note 18) 3.0 W
LM4867MTE, R
L
=4Ω(Note 19) 2.6 W
LM4867LQ, R
L
=4Ω(Note 19) 2.6 W
LM4867, R
L
=8 1.5 W
THD+N = 1%, f = 1 kHz, R
L
=32 0.34 W
LM4867
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Electrical Characteristics for Bridged-Mode Operation (Notes 3, 13) (Continued)
The following specifications apply for VDD= 5V unless otherwise specified. Limits apply for TA= 25˚C.
Symbol Parameter Conditions LM4867 Units
(Limits)
Typical Limit
(Note 14) (Note 15)
THD+N Total Harmonic Distortion+Noise 20Hz f 20kHz, A
VD
=2
LM4867MTE, R
L
=4Ω,PO=2W
LM4867LQ, R
L
=4Ω,PO=2W
LM4867, R
L
=8Ω,PO=1W
0.3
0.3
0.3
% % %
PSRR Power Supply Rejection Ratio V
DD
= 5V, V
RIPPLE
= 200 mV
RMS,RL
=8Ω,
C
B
= 2.2µF
67 dB
X
TALK
Channel Separation f = 1 kHz, CB= 2.2µF 80 dB
SNR Signal To Noise Ratio V
DD
= 5V, PO= 1.1W, RL=8 97 dB
Electrical Characteristics for Single-Ended Operation (Notes 3, 13)
The following specifications apply for VDD= 5V unless otherwise specified. Limits apply for TA= 25˚C.
Symbol Parameter Conditions LM4867 Units
(Limits)
Typical Limit
(Note 14) (Note 15)
V
OS
Output Offset Voltage VIN= 0V 5 50 mV (max)
P
O
Output Power THD = 0.5%, f = 1kHz, RL=32 85 75 mW (min)
THD+N = 1%, f = 1kHz, R
L
=8Ω(Note
20)
180 mW
THD+N = 1%, f = 1kHz, R
L
=16
THD+N = 10%, f = 1kHz, R
L
=32
THD+N = 10%, f = 1kHz, R
L
=16
THD+N = 10%, f = 1kHz, R
L
=32
165
88 208 114
mW mW mW mW
V
OUT
Output Voltage Swing THD = 0.05%, RL=5k 1V
P-P
THD+N Total Harmonic Distortion+Noise AV= −1, PO= 75mW, 20 Hz f 20kHz,
R
L
=32
0.2 %
PSRR Power Supply Rejection Ratio C
B
= 2.2µF, V
RIPPLE
= 200mV
RMS
,
f = 1kHz
52 dB
X
TALK
Channel Separation f = 1kHz, CB= 2.2µF 60 dB
SNR Signal To Noise Ratio V
DD
= 5V, PO= 340mW, RL=8 94 dB
Note 3: Absolute Maximum Ratings indicate limits beyond which damage to the device may occur. Operating Ratings indicate conditions for which the device is functional, but donotguaranteespecific performance limits. Electrical Characteristics state DC and AC electrical specifications under particular test conditions which guarantee specific performance limits. This assumes that the device operates within the Operating Ratings. Specifications are not guaranteed for parameters where no limit is given. The typical value however, is a good indication of device performance.
Note 4: The maximum power dissipation must be derated at elevated temperatures and is dictated by T
JMAX
, θJA, and the ambient temperature TA. The maximum
allowable power dissipation is P
DMAX
=(T
JMAX−TA
)/θJA. For the LM4867, T
JMAX
= 150˚C. For the θJAs for different packages, please see the Application
Information section or the Absolute Maximum Ratings section.
Note 5: Human body model, 100 pF discharged through a 1.5 kresistor. Note 6: Machine model, 220 pF–240 pF discharged through all pins. Note 7: The given θ
JA
is for an LM4867 packaged in an MXA20A with the Exposed-DAP soldered to an exposed 2in2area of 1oz printed circuit board copper.
Note 8: The given θ
JA
is for an LM4867 packaged in an MXA20A with the Exposed-DAP soldered to an exposed 1in2area of 1oz printed circuit board copper.
Note 9: The given θ
JA
is for an LM4867 packaged in an MXA20A with the Exposed-DAP not soldered to printed circuit board copper.
Note 10: The given θ
JA
is for an LM4867 packaged in an LQA24A with the Exposed-DAP soldered to an exposed 2in2area of 1oz printed circuit board copper.
Note 11: The given θ
JA
is for an LM4867 packaged in an LQA24A with the Exposed-DAP soldered to an exposed 1in2area of 1oz printed circuit board copper.
Note 12: The given θ
JA
is for an LM4867 packaged in an LQA24A with the Exposed-DAP not soldered to printed circuit board copper.
Note 13: All voltages are measured with respect to the ground (GND) pins, unless otherwise specified. Note 14: Typicals are measured at 25˚C and represent the parametric norm. Note 15: Limits are guaranteed to National’s AOQL (Average Outgoing Quality Level). Datasheet min/max specification limits are guaranteed by design, test, or
statistical analysis.
Note 16: The quiescent power supply current depends on the offset voltage when a practical load is connected to the amplifier. Note 17: Output power is measured at the device terminals. Note 18: When driving 3loads from a 5V supply,the LM4867LQ, LM4867MTE, or LM4867MTE-1 must be mounted to the circuit board and forced-air cooled (450
linear-feet per minute).
Note 19: When driving 4loads from a 5V supply, the LM4867LQ, LM4867MTE or LM4867MTE-1 must be mounted to the circuit board.
LM4867
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Electrical Characteristics for Single-Ended Operation (Notes 3, 13) (Continued)
Note 20: See Application Information section ’Single-Ended Output Power Performance and Measurement Considerations’ for more information.
Typical Performance Characteristics MTE- and LQ- Specific Characteristics
Note 21: This curve shows the LM4867MTE’s thermal dissipation ability at different ambient temperatures given these conditions:
500LFPM + JEDEC board: The part is soldered to a 1S2P 20-lead exposed-DAP TSSOP test board with 500 linear feet per minute of forced-air flow across
it. Board information - copper dimensions: 74x74mm, copper coverage: 100% (buried layer) and 12% (top/bottom layers), 16 vias under the exposed-DAP.
500LFPM + 2.5in
2
: The part is soldered to a 2.5in2, 1 oz. copper plane with 500 linear feet per minute of forced-air flow across it.
2.5in
2
: The part is soldered to a 2.5in2, 1oz. copper plane.
Not Attached: The part is not soldered down and is not forced-air cooled.
LM4867MTE THD+N vs Output Power
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LM4867MTE THD+N vs Frequency
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LM4867LQ THD+N vs Output Power
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LM4867LQ THD+N vs Frequency
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LM4867MTE THD+N vs Output Power
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LM4867LQ THD+N vs Output Power
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LM4867LQ, LM4867MTE Power Dissipation vs Power Output
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LM4867LQ, LM4867MTE(Note 21) Power Derating Curve
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LM4867
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Typical Performance Characteristics
THD+N vs Frequency
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THD+N vs Frequency
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THD+N vs Frequency
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THD+N vs Output Power
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THD+N vs Output Power
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THD+N vs Output Power
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THD+N vs Output Power
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THD+N vs Frequency
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THD+N vs Output Power
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THD+N vs Frequency
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Output Power vs Load Resistance
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Power Dissipation vs Supply Voltage
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Typical Performance Characteristics (Continued)
Output Power vs Supply Voltage
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Output Power vs Supply Voltage
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Output Power vs Supply Voltage
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Output Power vs Load Resistance
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Output Power vs Load Resistance
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Power Dissipation vs Output Power
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Dropout Voltage vs Supply Voltage
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Power Derating Curve
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Power Dissipation vs Output Power
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LM4867
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Typical Performance Characteristics (Continued)
Noise Floor
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Channel Separation
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Channel Separation
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Power Supply Rejection Ratio
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Open Loop Frequency Response
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Supply Current vs Supply Voltage
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LM4867
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External Components Description
( Refer to Figure 1. )
Components Functional Description
1. R
i
Inverting input resistance which sets the closed-loop gain in conjunction with Rf. This resistor also forms a high pass filter with C
i
at fc= 1/(2πRiCi).
2. C
i
Input coupling capacitor which blocks the DC voltage at the amplifier’s input terminals. Also creates a highpass filter with R
i
at fc= 1/(2πRiCi). Refer to the section, Proper Selection of External Components,
for an explanation of how to determine the value of C
i
.
3. R
f
Feedback resistance which sets the closed-loop gain in conjunction with Ri.
4. C
s
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.
5. C
B
Bypass pin capacitor which provides half-supply filtering. Refer to the section, Proper Selection of External Components, for information concerning proper placement and selection of C
B
.
Application Information
ELIMINATING OUTPUT COUPLING CAPACITORS
Typical single-supply audio amplifiers that can switch be­tween driving bridge-tied-load (BTL) speakers and single-ended (SE) headphones use a coupling capacitor on each SE output. This capacitor blocks the half-supply volt­age to which the output amplifiers are typically biased and couples the audio signal to the headphones. The signal return to circuit ground is through the headphone jack’s sleeve.
The LM4867 eliminates these coupling capacitors. Amp2A is internally configured to apply V
DD
/2 to a stereo headphone jack’s sleeve. This voltage matches the quiescent voltage present on the Amp1A and Amp1B outputs that drive the headphones. The headphones operate in a manner very similar to a bridge-tied-load (BTL). The same DC voltage is applied to both headphone speaker terminals. This results in no net DC current flow through the speaker.AC current flows through a headphone speaker as an audio signal’s output amplitude increases on the speaker’s terminal.
When operating as a headphone amplifier, the headphone jack sleeve is not connected to circuit ground. Using the headphone output jack as a line-level output will place the LM4867’s one-half supply voltage on a plug’s sleeve con­nection. Driving a portable notebook computer or audio-visual display equipment is possible. This presents no difficulty when the external equipment uses capacitively coupled inputs. For the very small minority of equipment that is DC-coupled, the LM4867 monitors the current supplied by the amplifier that drives the headphone jack’s sleeve. If this current exceeds 500mA
PK
, the amplifier is shutdown, pro­tecting the LM4867 and the external equipment. For more information, see the section titled ’Single-Ended Output
Power Performance and Measurement Considerations’.
OUTPUT TRANSIENT (’POPS AND CLICKS’) ELIMINATED
The LM4867 contains advanced circuitry that eliminates out­put transients (’pop and click’). This circuitry prevents all traces of transients when the supply voltage is first applied, when the part resumes operation after shutdown, or when switching between BTL speakers and SE headphones. Two circuits combine to eliminate pop and click. One circuit mutes the output when switching between speaker loads. Another circuit monitors the input signal. It maintains the muted condition until there is sufficient input signal magni­tude to mask any remaining transient that may occur.
Figure 2
shows the LM4867’s lack of transients in the differ­ential signal (Trace B) across a BTL 8load. The LM4867’s active-high SHUTDOWN pin is driven by the logic signal shown in Trace A. Trace C is the VOUT- output signal and trace D is the VOUT+ output signal. The shutdown signal frequency is 1Hz with a 50% duty cycle.
Figure 3
is gener­ated with the same conditions except that the output drives a 32single-ended (SE) load. Again, no trace of output tran­sients is seen.
USING THE LM4867 TO UPGRADE LM4863 AND LM4873 DESIGNS
The LM4867’s noise-free operation plus coupling-capacitorless headphone operation and functional compatibility with the LM4873 and the LM4863 simplifies upgrading systems using these parts. Upgrading older de­signs that use either the LM4863 or the LM4873 is easy. Simply remove and short the coupling capacitors located between the LM4873’s or LM4863’s Amp1A and Amp1B outputs and the headphone connections. Also remove the 1kresistor between each headphone connection and ground. Finally, remove any resistors connected to the HP-IN pin (typically two 100kresistors). Connect the HP-IN pin directly to the headphone jack control pin as shown in
Figure 4
.
DS200013-56
FIGURE 2. Differential output signal (Trace B) is devoid
of transients. The SHUTDOWN pin is driven by a
shutdown signal (Trace A). The inverting output (Trace
C) and the non-inverting output (Trace D) are applied
across an 8BTL load.
LM4867
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Application Information (Continued)
The LM4867’s pin configuration simplifies the process of upgrading systems that use the LM4863. Except for its four MUX function pins, the LM4867’s pin configuration matches the LM4863’s pin configuration. If the LM4867’s MUX func­tionality is not needed when replacing an LM4863, connect the MUX CTRL pin to either V
DD
or ground. To ensure
correct amplifier operation, unused MUX inputs must be tied to GND. As shown in Table1, grounding the MUX CTRL
pin selects stereo input 1 (−IN A1 and −IN B1), whereas applying V
DD
to the MUX CTRL pin selects stereo input 2
(−IN A2 and −IN B2). The LM4867’s unique headphone sense circuit requires a
dual switch headphone jack. Replace the four-terminal head­phone jack used with the LM4863 and LM4873 with the five-terminal headphone jack, such as the Switchcraft 35RAPC4BH3, shown in Figure 4. Connect the +OUT A (Amp2A) pin to the five-terminal headphone jack’s sleeve pin.
DS200013-57
FIGURE 3. Single-ended output signal (Trace B) is
devoid of transients. The SHUTDOWN pin is driven by
a shutdown signal (Trace A). The inverting output
(Trace C) and the V
BYPASS
output (Trace D) are applied
across a 32BTL load.
DS200013-31
FIGURE 4. Typical Audio Amplifier Application Circuit
(Pin out shown for the 24-pin Exposed-DAP LLP package. Numbers in ( ) are for the 20-pin MTE and MT packages.)
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Application Information (Continued)
STEREO-INPUT MULTIPLEXER (STEREO MUX)
The LM4867 has two stereo inputs. The MUX CTRL Pin controls which stereo input is active. As shown in the Truth Tablefor Logic Inputs, applying 0V to the MUX CTRL input activates stereo input 1, whereas applying V
DD
to the MUX
CTRL inputs activates stereo input 2. To ensure correct
amplifier operation, unused MUX inputs must be tied to GND.
TypicalLM4867 applications use the MUX to switch between two stereo input signals. Each stereo channel’s gain can be tailored to produce the required output signal level by choos­ing the appropriate input and feedback resistor ratio.
Another configuration uses the MUX to select two different gains or frequency compensated gains that amplify a single pair of stereo input signals.
Figure 5
shows two different feedback networks, Network 1 and Network 2. Network 1 produces increasing gain as the input signal’s frequency
decreases. This can be used to compensate a small, full-range speaker’s low frequency response roll-off. Network 2 sets the gain for an alternate load such as headphones. The circuit in
Figure 6
uses Network 1 when driving external speakers, switching to Network 2 when headphones are connected. The normally closed control switch in
Figure 6
’s headphone jack connects to the MUX CTRL pin. When headphones are connected, the LM4867’s internal pull-up that applies V
DD
to the HP-IN and the external 100kresis-
tor applies V
DD
to MUX CTRL pin. Simultaneously applying these control voltages automatically selects the amplifier (headphone or bridge) and switches the gain (MUX channel selection).Alternatively,leaving the MUX CTRL pin indepen­dently accessible allows a user to select bass boost as needed. This alternative user-selectable bass-boost scheme requires connecting equal ratio resistor feedback networks to each MUX input channel. The value of the resistor in the RC network is chosen to give a gain that is necessary to achieve the desired bass-boost.
PIN OUT COMPATIBILITY WITH THE LM4863
The LM4867 pin out was designed to simplify replacing the LM4863: except for the four Pins(-INA
2
, MUX CTRL, -IN B2, and NC) that implement the LM4867’s extra functionality,the LM4867MT/MTE and LM4863MT/MTE pin outs match. (Note 22)
Note 22: If the LM4867 replaces an LM4863 and the input MUX circuitry is not being used, the LM4867 MUX CTRL pin must be tied to V
DD
or GND and
the unused MUX inputs must be connected to GND.
EXPOSED-DAP MOUNTING CONSIDERATIONS
The LM4867’s exposed-DAP (die attach paddle) packages (MTE and LQ) provide a low thermal resistance between the die and the PCB to which the part is mounted and soldered. This allows rapid heat transfer from the die to the surround­ing PCB copper area heatsink, copper traces, ground plane, and finally, surrounding air. The result is a low voltage audio
power amplifier that produces 2.4W dissipation in a 4load at 1% THD+N and over 3W in a 3load at 10% THD+N. This high power is achieved through careful consideration of necessary thermal design. Failing to optimize thermal design may compromise the LM4867’s high power performance and activate unwanted, though necessary, thermal shutdown protection.
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FIGURE 5. Input MUX Example
DS200013-39
FIGURE 6. As configured, connecting headphones to this jack automatically selects the stereo headphone amplifier
and, with the additional NC switch, changes MUX channels (Network 2 in Figure 2 )
LM4867
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Application Information (Continued)
The MTE and LQ packages must have their DAPs soldered to a copper pad on the PCB. The DAP’s PCB copper pad is then, ideally, connected to a large plane of continuous un­broken copper. This plane forms a thermal mass, heat sink, and radiation area. Place the heat sink area on either outside plane in the case of a two-sided or multi-layer PCB. (The heat sink area can also be placed on an inner layer of a multi-layer board. The thermal resistance, however, will be higher.) Connect the DAP copper pad to the inner layer or backside copper heat sink area with 32 (4 X 8) (MTE) or 6 (3 X 2) (LQ) vias. The via diameter should be 0.012in - 0.013in with a 1.27mm pitch. Ensure efficient thermal conductivity by plugging and tenting the vias with plating and solder mask, respectively.
Best thermal performance is achieved with the largest prac­tical copper heat sink area. If the heatsink and amplifier share the same PCB layer, a nominal 2.5in
2
(min) area is necessary for 5V operation with a 4load. Heatsink areas not placed on the same PCB layer as the LM4867 should be 5in
2
(min) for the same supply voltage and load resistance. The last two area recommendations apply for 25˚C ambient temperature. Increase the area to compensate for ambient temperatures above 25˚C. In systems using cooling fans, the LM4867MTE can take advantage of forced air cooling. With an air flow rate of 450 linear-feet per minute and a 2.5in
2
exposed copper or 5.0in2inner layer copper plane heatsink, the LM4867MTE can continuously drive a 3load to full power. The LM4867LQ achieves the same output power level without forced-air cooling. In all circumstances and under all conditions, the junction temperature must be held below 150˚C to prevent activating the LM4867’s thermal shutdown protection. The LM4867’s power de-rating curve in the Typical Performance Characteristics shows the maxi­mum power dissipation versus temperature. Example PCB layouts for the exposed-DAP TSSOP and LQ packages are shown in the Demonstration Board Layout section. Further detailed and specific information concerning PCB layout and fabrication and mounting an LQ (LLP) is found in National Semiconductor’s AN1187.
PCB LAYOUT AND SUPPLY REGULATION CONSIDERATIONS FOR DRIVING 3AND 4LOADS
Power dissipated by a load is a function of the voltage swing across the load and the load’s impedance. As load imped­ance decreases, load dissipation becomes increasingly de­pendent on the interconnect (PCB trace and wire) resistance between the amplifier output pins and the load’s connec­tions. Residual trace resistance causes a voltage drop, which results in power dissipated in the trace and not in the load as desired. For example, 0.1trace resistance reduces the output power dissipated by a 4load from 2.1W to 2.0W. The problem of decreased load dissipation is exacerbated as load impedance decreases. Therefore, to maintain the highest load dissipation and widest output voltage swing, PCB traces that connect the output pins to a load must be as wide as possible.
BRIDGE CONFIGURATION EXPLANATION
As shown in
Figure 4
, the LM4867 consists of two pairs of operational amplifiers, forming a two-channel (channel A and channel B) stereo amplifier. (Though the following discusses channelA, it applies equally to channel B.) External resistors R
f
and Riset the closed-loop gain of Amp1A, whereas two internal 20kresistors set Amp2A’s gain at -1. The LM4867 drives a load, such as a speaker,connected between the two amplifier outputs, -OUTA and +OUTA.
Figure 4
shows that Amp1A’s output serves as Amp2A’s input. This results in both amplifiers producing signals iden­tical in magnitude, but 180˚ out of phase. Taking advantage of this phase difference, a load is placed between -OUTA and +OUTA and driven differentially (’commonly referred to as bridge mode’). This results in a differential gain of
A
VD
=2*(Rf/Ri) (1)
Bridge mode amplifiers are different from single-ended am­plifiers that drive loads connected between a single amplifi­er’s output and ground. For a given supply voltage, bridge mode has a distinct advantage over the single-ended con­figuration: its differential output doubles the voltage swing across the load. This produces four times the output power when 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 that the output signal is not clipped. To ensure minimum output sig­nal clipping when choosing an amplifier’s closed-loop gain, refer to the Audio Power Amplifier Design section.
A bridge amplifier design has a few distinct advantages over the single-ended configuration, as it provides differential drive to the load, thus doubling the output swing for a speci­fied supply voltage. 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 caus­ing excessive clipping, please refer to the Audio Power Amplifier Design section.
Another advantage of the differential bridge output is no net DC voltage across the load. This is accomplished by biasing channel A’s and channel B’s outputs at half-supply. This eliminates the coupling capacitor that single supply, single-ended amplifiers require. Eliminating an output cou­pling capacitor in a single-ended configuration forces a single-supply amplifier’s half-supply bias voltage across the load. This increases internal IC power dissipation and may permanently damage loads such as speakers.
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 single-ended amplifier operating at a given supply voltage and driving a specified output load.
P
DMAX
=(VDD)2/(2π2RL): Single-Ended (2)
However, a direct consequence of the increased power de­livered to the load by a bridge amplifier is higher internal power dissipation for the same conditions.
The LM4867 has two operational amplifiers per channel. The maximum internal power dissipation per channel operating in
LM4867
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Page 13
Application Information (Continued)
the bridge mode is four times that of a single-ended ampli­fier. From Equation (3), assuming a 5V power supply and an 4load, the maximum single channel power dissipation is
1.27W or 2.54W for stereo operation.
P
DMAX
=4*(VDD)2/(2π2RL): Bridge Mode (3)
The LM4867’s power dissipation is twice that given by Equa­tion (2) or Equation (3) when operating in the single-ended mode or bridge mode, respectively. Twice the maximum power dissipation point given by Equation (3) must not ex­ceed the power dissipation given by Equation (4):
P
DMAX
’=(T
JMAX−TA
)/θ
JA
(4)
The LM4867’s TJMAX = 150˚C. In the LQ package soldered to a DAP pad that expands to a copper area of 5in
2
on a
PCB, the LM4867’s θ
JA
is 20˚C/W. In the MTE package
soldered to a DAP pad that expands to a copper area of 2in
2
on a PCB, the LM4867’s θJAis 41˚C/W.At any given ambient temperature T
A
, use Equation (4) to find the maximum inter­nal power dissipation supported by the IC packaging. Rear­ranging Equation (4) and substituting P
DMAX
for P
DMAX
’ re­sults in Equation (5). This equation gives the maximum ambient temperature that still allows maximum stereo power dissipation without violating the LM4867’s maximum junction temperature.
T
A=TJMAX
−2XP
DMAXθJA
(5)
For a typical application with a 5V power supply and an 4 load, the maximum ambient temperature that allows maxi­mum stereo power dissipation without exceeding the maxi­mum junction temperature is approximately 99˚C for the LQ package and 45˚C for the MTE package.
T
JMAX=PDMAXθJA+TA
(6)
Equation (6) gives the maximum junction temperature T
JMAX
. If the result violates the LM4867’s 150˚C, reduce the 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 a surface mount part operating around the maximum power dissipation point. Since internal power dissipation is a function of output power, higher ambient temperatures are allowed as output power or duty cycle decreases.
JA
. The heat sink can be created using additional copper area around the package, with connections to the ground pin(s), supply pin and amplifier output pins. External, solder attached SMT heatsinks such as the Thermalloy 7106D can also improve power dissipation. When adding a heat sink, the θ
JA
is the sum of θJC, θCS, and θSA.(θJCis the
junction−to−case thermal impedance, θ
CS
is the
case−to−sink thermal impedance, and θ
SA
is the sink−to−ambient thermal impedance.) Refer to the Typical Performance Characteristics curves for power dissipation information at lower output power levels.
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 5V 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 1.0µF tantalum bypass capacitance connected between the LM4867’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 LM4867’s power supply pin and ground as short as possible. Connecting a 1µF capacitor, C
B
, between the BYPASS 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 and can compromise the amplifier’s click and pop performance. The selection of bypass capacitor values, especially C
B
, depends on desired PSRR requirements, click and pop performance (as explained in the section, Proper Selection of External Components), system cost, and size constraints.
MICRO−POWER SHUTDOWN
The voltage applied to the SHUTDOWN pin controls the LM4867’s shutdown function. Activate micro−power shut­down by applying V
DD
to the SHUTDOWN pin. When active, the LM4867’s micro−power shutdown feature turns off the amplifier’s bias circuitry, reducing the supply current. The logic threshold is typically V
DD
/2. The low 0.7µA typical shutdown current is achieved by applying a voltage that is as near as V
DD
as possible to the SHUTDOWN pin. A voltage
that is less than V
DD
may increase the shutdown current. Table 1 shows the logic signal levels that activate and deac­tivate micro−power shutdown and headphone amplifier op­eration. To ensure that the output signal remains
transient−free, do not cycle the shutdown function faster than 1Hz.
There are a few ways to control the micro−power shutdown. These include using a single−pole, single, throw switch, a microprocessor, or a microcontroller. When using a switch, connect an external 100kpull−up resistor between the SHUTDOWN pin and V
DD
. Connect the switch between the SHUTDOWN pin and ground. Select normal amplifier opera­tion by closing the switch. Opening the switch connects the SHUTDOWN pin to V
DD
through the pull−up resistor, acti­vating micro−power shutdown. The switch and resistor guar­antee that the SHUTDOWN pin will not float. This prevents unwanted state changes. In a system with a microprocessor or a microcontroller, use a digital output to apply the control voltage to the SHUTDOWN pin. Driving the SHUTDOWN pin with active circuitry eliminates the pull up resistor.
LM4867
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Page 14
Application Information (Continued) Truth Table for Logic Inputs
SHUTDOWN
PIN
HP-IN
PIN
MUX CHANNEL
INPUT SELECT
OPERATIONAL MODE (MUX
INPUTCHANNEL #)
Logic Low = −OUTB signal Logic Low Bridged amplifiers (1) Logic Low = −OUTB signal Logic High Bridged amplifiers (2) Logic Low
−OUTB signal Logic Low Single-ended amplifiers (1)
Logic Low
−OUTB signal Logic High Single-ended amplifiers (2)
Logic High X X Micro−power shutdown
HP-IN FUNCTION
An internal pull−up circuit is connected to the HP−IN (pin 20) headphone amplifier control pin. When this pin is left uncon­nected, V
DD
is applied to the HP−IN. This turns off Amp2B and switches Amp2A’s input signal from an audio signal to the V
DD
/2 voltage present on pin 14. The result is muted bridge-connected loads. Quiescent current consumption is reduced when the IC is in this single−ended mode.
Figure 7
shows the implementation of the LM4867’s head­phone control function. An internal comparator with a nomi­nal 400mV offset monitors the signal present at the −OUTB output. It compares this signal against the signal applied to the HP−IN pin. When these signals are equal, as is the case when a BTL is connected to the amplifier, the comparator forces the LM4867 to maintain bridged−amplifier operation. When the HP−IN pin is externally floated, such as when headphones are connected to the jack shown in
Figure 7
,
and internal pull−up forces V
DD
on the internal comparator’s HP−IN inputs. This changes the comparator’s output state and enables the headphone function: it turns off Amp2B, switches Amp2A’s input signal from an audio signal to the V
DD
/2 voltage present on pin 14, and mutes the bridge-connected loads. Amp1A and Amp1B drive the head­phones.
Figure 7
also shows the suggested headphone jack electri­cal connections. The jack is designed to mate with a three−wire plug. The plug’s tip and ring should each carry one of the two stereo output signals, whereas the sleeve provides the return to Amp2A. A headphone jack with one control pin contact is sufficient to drive the HP−IN pin when connecting headphones.
A switch can replace the headphone jack contact pin. When a switch shorts the HP−IN pin to V
DD
, bridge−connected
speakers are muted and Amp1A and Amp2A drive a pair of
headphones. When a switch shorts the HP−IN pin to GND, the LM4867 operates in bridge mode. If headphone drive is not needed, short the HP−IN pin to the −OUTB pin.
Single-Ended Output Power Performance and Measurement Considerations
The LM4867 delivers clean, low distortion SE output power into loads that are greater than 10. As an example, output power for 16and 32loads are shown in the Typical Performance Characteristic curves. For loads less than 10, the LM4876 can typically supply 180mW of low distor­tion power. However, when higher dissipation is desired in loads less than 10, a dramatic increase in THD+N may occur. This is normal operation and does not indicate that proper functionality has ceased. When a jump from moder­ate to excessively high distortion is seen, simply reducing the output voltage swing will restore the clean, low distortion SE operation.
The dramatic jump in distortion for loads less than 10 occurs when current limiting circuitry activates. During SE operation, AMP2A (refer to
Figure 4
) drives the headphone sleeve. An on-board circuit monitors this amplifier’s output current. The sudden increase in THD+N is caused by the current limit circuitry forcing AMP2A into a high−impedance output mode. When this occurs, the output waveform has discontinuities that produce large amounts of distortion. It has been observed that as the output power is steadily increased, the distortion may jump from 5% to greater than 35%. Indeed, 10% THD+N may not actually be achievable.
Using the Single−Ended Output for Line Level Applications
Some samples of the LM4867 may exhibit small amplitude, high frequency oscillation when the SE output is connected to a line-level input. This oscillation can be eliminated by connecting a 5%, 300resistor betweenAmp2A’s output pin and each amplifier, AMP1A and AMP1B, output.
LM4867
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Page 15
Application Information (Continued)
Input Capacitor Value Selection
Amplifying the lowest audio frequencies requires high value input coupling capacitor (C
i
in
Figure 4
).A high value capaci­tor can be expensive and may compromise space efficiency in portable designs. In many cases, however, the speakers used in portable systems, whether internal or external, have little ability to reproduce signals below 150Hz. Applications using speakers with this limited frequency response reap little improvement by using large input capacitor.
Besides effecting system cost and size, C
i
has an affect on the LM4867’s click and pop performance. When the supply voltage is first applied, a transient (pop) is created as the charge on the input capacitor changes from zero to a quies­cent state. The magnitude of the pop is directly proportional to the input capacitor’s size. Higher value capacitors need more time to reach a quiescent DC voltage (usually V
DD
/2) when charged with a fixed current. The amplifier’s output charges the input capacitor through the feedback resistor, R
f
. Thus, pops can be minimized by selecting an input capacitor value that is no higher than necessary to meet the desired −3dB frequency and is between 0.14C
B
and 0.20CB.
A shown in
Figure 4
, the input resistor (RI) and the input
capacitor,C
I
produce a −3dB high pass filter cutoff frequency
that is found using Equation (7).
f
−3dB
= 1/(2πRINCI) (7)
As an example when using a speaker with a low frequency limit of 150Hz, C
i
, using Equation (4) is 0.063µF. The 1.0µF
C
i
shown in
Figure 4
allows the LM4867 to drive high effi­ciency, full range speaker whose response extends below 30Hz.
Bypass Capacitor Value Selection
Besides minimizing the input capacitor size, careful consid­eration should be paid to value of C
B
, the capacitor con-
nected to the BYPASS pin. Since C
B
determines how fast the LM4867 settles to quiescent operation, its value is critical when minimizing turn-on pops. The slower the LM4867’s outputs ramp to their quiescent DC voltage (nominally 1/2 V
DD
), the smaller the turn-on pop. Choosing CBequal to
1.0µF along with a small value of C
i
(in the range of 0.1µF to
0.39µF), produces a click-less and pop-less shutdown func­tion. As discussed above, choosing C
i
no larger than neces-
sary for the desired bandwidth helps minimize clicks and pops. C
B
’s value should be in the range of 5 times to 7 times
the value of C
i
. This ensures that output transients are eliminated when power is first applied or the LM4867 re­sumes operation after shutdown.
OPTIMIZING CLICK AND POP REDUCTION PERFORMANCE
The LM4867 contains circuitry that eliminates turn-on and shutdown transients (“clicks and pops“) and transients that could occur when switching between BTL speakers and single-ended headphones. For this discussion, turn-on re­fers to either applying the power supply voltage or when the shutdown mode is deactivated. While the power supply is ramping to its final value, the LM4867’s internal amplifiers are configured as unity gain buffers and are disconnected from the -OUT and +OUT pins. An internal current source changes the voltage of the BYPASS pin in a controlled, linear manner.Ideally, the input and outputs track the voltage applied to the BYPASS pin. The gain of the internal amplifi­ers remains unity until the voltage on the bypass pin reaches 1/2 V
DD
. As soon as the voltage on the bypass pin is stable, the device becomes fully operational and the amplifier out­puts are reconnected to the -OUT and +OUT pins. Although the BYPASS pin current cannot be modified, changing the size of C
B
alters the device’s turn-on time. There is a linear
relationship between the size of C
B
and the turn-on time.
Here are some typical turn-on times for various values of C
B
:
C
B
T
ON
0.01µF 3ms
0.1µF 30ms
0.22µF 63ms
0.47µF 134ms
1.0µF 300ms
2.2µF 630ms
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“.
DS200013-24
FIGURE 7. Headphone Circuit
(Pin numbers in ( ) are for the 20-pin MTE and MT packages.)
LM4867
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Application Information (Continued)
NO LOAD STABILITY
AUDIO POWER AMPLIFIER DESIGN Audio Amplifier Design: Driving 1W into an 8Load
The following are the desired operational parameters:
Power Output: 1 W
RMS
Load Impedance: 8 Input Level: 1 V
RMS
Input Impedance: 20 k
Bandwidth: 100 Hz−20 kHz
±
0.25 dB
The design begins by specifying the minimum supply voltage necessary to obtain the specified output power. One way to find the minimum supply voltage is to use the Output Power vs Supply Voltage curve in the Typical Performance Char- acteristics section. Another way, using Equation (8), is to calculate the peak output voltage necessary to achieve the desired output power for a given load impedance. To ac­count for the amplifier’s dropout voltage, two additional volt­ages, based on the Dropout Voltage vs Supply Voltagein the Typical Performance Characteristics curves, must be added to the result obtained by Equation (8). The result is Equation (9).
(8)
V
DD
(V
OUTPEAK
+(V
OD
TOP
+V
OD
BOT
)) (9)
The Output Power vs Supply Voltage graph for an 8load indicates a minimum supply voltage of 4.6V. This is easily met by the commonly used 5V supply voltage. The additional voltage creates the benefit of headroom, allowing the LM4867 to produce peak output power in excess of 1W without clipping or other audible distortion. The choice of supply voltage must also not create a situation that violates of maximum power dissipation as explained above in the Power Dissipation section.
After satisfying the LM4867’s power dissipation require­ments, the minimum differential gain needed to achieve 1W dissipation in an 8load is found using Equation (10).
(10)
Thus, a minimum gain of 2.83 allows the LM4867’s to reach full output swing and maintain low noise and THD+N perfor­mance. For this example, let A
VD
=3.
The amplifier’s overall gain is set using the input (R
i
) and
feedback (R
i
) resistors. With the desired input impedance set at 20k, the feedback resistor is found using Equation (11).
R
f/Ri=AVD
/2 (11)
The value of R
f
is 30k.
The last step in this design example is setting the amplifier’s
−3dB frequency bandwidth. To achieve the desired
±
0.25dB pass band magnitude variation limit, the low frequency re­sponse must extend to at least one-fifth the lower bandwidth limit and the high frequency response must extend to at least five times the upper bandwidth limit. The gain variation for both response limits is 0.17dB, well within the
±
0.25dB desired limit. The results are an
f
L
= 100Hz/5 = 20Hz (12)
and an
f
H
= 20kHz x 5 = 100kHz (13)
As mentioned in the Selecting Proper External Compo- nents section, R
i
and Cicreate a highpass filter that sets the amplifier’s lower bandpass frequency limit. Find the coupling capacitor’s value using Equation (12).
C
i
1/(2πRifL) (14)
The result is
1/(2π
*
20k*20Hz) = 0.397µF (15)
Use a 0.39µF capacitor, the closest standard value.
The product of the desired high frequency cutoff (100kHz in this example) and the differential gain A
VD
, determines the
upper passband response limit. With A
VD
= 3 and fH= 100kHz, the closed-loop gain bandwidth product (GBWP) is 300kHz. This is less than the LM4867’s 3.5MHz GBWP.With this margin, the amplifier can be used in designs that require more differential gain while avoiding performance,restricting bandwidth limitations.
RECOMMENDED PRINTED CIRCUIT BOARD LAYOUT
These circuit boards are easy to use.Apply 5V and ground to the board’s V
DD
and GND pads, respectively. Connect 4 speakers between the board’s −OUTA and +OUTA and OUTB and +OUTB pads.
LM4867
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Page 17
Application Information (Continued)
DS200013-40
Figure 8. Recommended LQ PC Board Layout:
Component-Side Silkscreen
DS200013-41
Figure 9. Recommended LQ PC Board Layout:
Component-Side Layout
LM4867
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Page 18
Application Information (Continued)
DS200013-42
Figure 10. Recommended LQ PC Board Layout:
Upper Inner-Layer Layout
DS200013-43
Figure 11. Recommended LQ PC Board Layout:
Lower Inner-Layer Layout
LM4867
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Page 19
Application Information (Continued)
DS200013-44
Figure 12. Recommended LQ PC Board Layout:
Bottom-Side Layout
DS200013-45
Figure 13. Recommended MTE PC Board Layout:
Component-Side Silkscreen
LM4867
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Page 20
Application Information (Continued)
DS200013-46
Figure 14. Recommended MTE PC Board Layout:
Component-Side Layout
DS200013-47
Figure 15. Recommended MTE PC Board Layout:
Upper Inner-Layer Layout
LM4867
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Application Information (Continued)
DS200013-48
Figure 16. Recommended MTE PC Board Layout:
Lower Inner-Layer Layout
DS200013-49
Figure 17. Recommended MTE PC Board Layout:
Bottom-Side Layout
LM4867
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Page 22
Application Information (Continued)
DS200013-50
Figure 18. Recommended MT PC Board Layout:
Component-Side Silkscreen
DS200013-51
Figure 19. Recommended MT PC Board Layout:
Component-Side Layout
LM4867
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Page 23
Application Information (Continued)
DS200013-52
Figure 20. Recommended MT PC Board Layout:
Bottom-Side Layout
LM4867
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Page 24
Physical Dimensions inches (millimeters) unless otherwise noted
24-Lead MOLDED PKG, Leadless Leadframe Package LLP
Order Number LM4867LQ
NS Package Number LQA24A
20-Lead MOLDED PKG, TSSOP, JEDEC, 4.4mm BODY WIDTH
Order Number LM4867MT
NS Package Number MTC20
LM4867
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Page 25
Physical Dimensions inches (millimeters) unless otherwise noted (Continued)
20-Lead MOLDED TSSOP, EXPOSED PAD, 6.5x4.4x0.9mm
Order Number LM4867MTE
NS Package Number MXA20A
LM4867
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Page 26
Notes
LIFE SUPPORT POLICY
NATIONAL’S PRODUCTS ARE NOT AUTHORIZED FOR USE AS CRITICAL COMPONENTS IN LIFE SUPPORT DEVICES OR SYSTEMS WITHOUT THE EXPRESS WRITTEN APPROVAL OF THE PRESIDENT AND GENERAL COUNSEL OF NATIONAL SEMICONDUCTOR CORPORATION. As used herein:
1. Life support devices or systems are devices or systems which, (a) are intended for surgical implant into the body, or (b) support or sustain life, and whose failure 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.
2. A critical component is any component of a life support device or system whose failure to perform can be reasonably expected to cause the failure of the life support device or system, or to affect its safety or effectiveness.
National Semiconductor Corporation
Americas Tel: 1-800-272-9959 Fax: 1-800-737-7018 Email: support@nsc.com
National Semiconductor Europe
Fax: +49 (0) 180-530 85 86
Email: europe.support@nsc.com Deutsch Tel: +49 (0) 69 9508 6208 English Tel: +44 (0) 870 24 0 2171 Français Tel: +33 (0) 1 41 91 8790
National Semiconductor Asia Pacific Customer Response Group
Tel: 65-2544466 Fax: 65-2504466 Email: ap.support@nsc.com
National Semiconductor Japan Ltd.
Tel: 81-3-5639-7560 Fax: 81-3-5639-7507
www.national.com
LM4867 Output-Transient-Free Dual 2.1W Audio Amplifier Plus No Coupling Capacitor Stereo
Headphone Function
National does not assume any responsibility for use of any circuitry described, no circuit patent licenses are implied and National reserves the right at any time without notice to change said circuitry and specifications.
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