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LM4913MM Datasheet(PDF) 9 Page - National Semiconductor (TI)

[Old version datasheet] Texas Instruments acquired National semiconductor.
Part # LM4913MM
Description  2W Monaural, 90mW Stereo Headphone Audio Amplifier
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Manufacturer  NSC [National Semiconductor (TI)]
Direct Link  http://www.national.com
Logo NSC - National Semiconductor (TI)

LM4913MM Datasheet(HTML) 9 Page - National Semiconductor (TI)

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Application Information
BRIDGE (BTL) OR SINGLE-ENDED (SE)
CONFIGURATION EXPLANATION
As shown in Figure 2, the LM4913 consists of two input
multiplexers (MUX) and two power amplifiers designed to
drive loads that have a minimum impedance of 4 ohms. In
mono BTL mode, AMP1 and AMP2 drive a speaker con-
nected between their outputs. In stereo SE mode, AMP1 and
AMP2 each drive a SE load such as stereo headphones.
In mono BTL mode, R1 works with one of AMP1’s internal
62.5kW feedback resistors to set this amplifier’s gain. AMP2
operates unity gain, set by two internal 20kW resistors. In
stereo SE modes, R2 and R3 work with AMP1’s and AMP2’s
internal 62.5kW feedback resistors to set each amplifier’s
gain. The LM4913 drives a BTL load, such as a speaker,
connected between AMP1’s and AMP2’s outputs. Two SE
loads can also be connected to the LM4913’s outputs, one
driven by AMP1 and the other driven by AMP2.
When the LM4913 operates in BTL mode, AMP1’s output
serves as AMP2’s input through AMP2’s input MUX. This
results in AMP1 and AMP2 producing signals identical in
magnitude, but 180˚ out of phase. Taking advantage of this
phase difference, a load placed between ROUT/M+ and
LOUT/M- is driven differentially (commonly referred to as
"bridge mode"). This results in a differential, or BTL, gain of
A
V (BTL) = -2(AV(SE))
A
V (SE) = -2(62.5k
Ω)/R
i
A
V (BTL) = -125k
Ω /R
i
(1)
Bridge mode amplifiers are different from single-ended am-
plifiers that drive loads connected between a single amplifi-
er’s output and ground. At any given supply voltage, bridge
mode has a distinct advantage over the single-ended con-
figuration: its differential output doubles the voltage swing
across the load. Theoretically, this produces four times the
output power when compared to a single-ended, capacitively
coupled amplifier under the same conditions. This increase
in attainable output power assumes that an amplifier is not
current limited and 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 Ampli-
fier Design section.
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-SE =VDD
2 /2
π2R
L:
Single-Ended
(2)
However, a direct consequence of the increased power de-
livered to the load by a bridge amplifier is higher internal
20061799
FIGURE 2. Typical Audio Amplifier Application Circuit
www.national.com
9


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