Application Information (Continued)
livered to the load. For example, with a 4Ω load and 0.1Ω of
trace resistance in each output, output power at the load
drops from 2.1W to 2.0W
Output power is also dependent on supply regulation. To
keep the supply voltage from sagging under full output
power conditions, the supply traces should be as wide as
practical.
BRIDGE CONFIGURATION EXPLANATION
As shown in
Figure 1
, the LM4873 has two pairs of 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 R
f
to Riwhile
the second amplifier’s gain is fixed by the two internal 20 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 each
channel of the IC is
A
VD
=2*(Rf/Ri)
By driving the load differentially through outputs +OutA and
−OutA or +OutB and −OutB, 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 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 Am-
plifier Design section.
A bridge configuration, such as the one used in LM4873,
also creates a second advantage over single-ended amplifiers. Since the differential outputs, +OutA, −OutA, +OutB,
and −OutB, 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. If an output coupling
capacitor is not used in a single-ended configuration, the
half-supply bias across the load would result in both increased internal IC power dissipation as well as permanent
loudspeaker damage.
POWER DISSIPATION
Whether the power amplifier is bridged or single-ended,
power dissipation is a major concern when designing the
amplifier. Equation 1 states the maximum power dissipation
point for a single-ended amplifier operating at a given supply
voltage and driving a specified load.
P
DMAX
=(VDD)2/(2π2RL): Single-Ended (1)
However, a direct consequence of the increased power delivered to the load by a bridge amplifier is an increase in internal power dissipation. Equation 2 states the maximum
power dissipation point for a bridge amplifier operating at the
same given conditions.
P
DMAX
=4*(VDD)2/(2π2RL): Bridge Mode (2)
Since the LM4873 is a dual channel power amplifier, the
maximum internal power dissipation is 2 times that of Equation 1 or Equation 2 depending on the mode of operation.
Even with this substantial increase in power dissipation, the
LM4873 does not require heatsinking. The power dissipation
from Equation 2, assuming a 5V power supply and an 8Ω
load, must not be greater than the power dissipation that results from Equation 3:
P
DMAX
=(T
JMAX−TA
)/θ
JA
(3)
For packages M16A and MTC20, θ
JA
= 80˚C/W, and for
package N16A, θ
JA
= 63˚C/W. T
JMAX
= 150˚C for the
LM4873. Depending on the ambient temperature, T
A
,ofthe
system surroundings, Equation 3 can be used to find the
maximum internal power dissipation supported by the IC
packaging. If the result of Equation 2 is greater than that of
Equation 3, then either the supply voltage must be decreased, the load impedance increased, or the ambient temperature reduced. For the typical application of a 5V power
supply,with an 8Ω bridged load, the maximum ambient temperature possible without violating the maximum junction
temperature is approximately 48˚C provided that device operation is around the maximum power dissipation point and
assuming surface mount packaging. Internal power dissipation is a function of output power. If typical operation is not
around the maximum power dissipation point, the ambient
temperature can be increased. Refer to the Typical Perfor-
mance Characteristics curves for power dissipation information for different output powers.
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. The
effect of a larger half supply bypass capacitor is improved
PSRR due to increased half-supply stability. Typical applications employ a 5V regulator with 10 µF and a 0.1 µF bypass
capacitors which aid in supply filtering. This does not eliminate the need for bypassing the supply nodes of the
LM4873. The selection of bypass capacitors, especially C
B
,
is thus dependent upon desired PSRR requirements, click
and pop performance as explained in the section, Proper
Selection of External Components, system cost, and size
constraints.
SHUTDOWN FUNCTION
In order to reduce power consumption while not in use, the
LM4873 contains a shutdown pin to externally turn off the
amplifier’s bias circuitry.This shutdown feature turns the amplifier off when a logic high is placed on the shutdown pin.
The trigger point between a logic low and logic high level is
typically half supply. It is best to switch between ground and
the supply V
DD
to provide maximum device performance. By
switching the shutdown pin to V
DD
, the LM4873 supply current draw will be minimized in idle mode. While the device
will be disabled with shutdown pin voltages less than V
DD
,
the idle current may be greater than the typical value of
0.7 µA. In either case, the shutdown pin should be tied to a
definite voltage to avoid unwanted state changes.
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 in conjunction
with an external pull-up resistor. When the switch is closed,
the shutdown pin is connected to ground and enables the
amplifier. If the switch is open, then the external pull-up re-
LM4873
www.national.com11