
Application Information
EXPOSED-DAP PACKAGE PCB MOUNTING
CONSIDERATIONS
The LM4836’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 traces, ground plane and, finally,
surrounding air. The result is a low voltage audio power
amplifier that produces 2.1W at
≤ 1% THD with a 4 load.
This high power is achieved through careful consideration of
necessary thermal design. Failing to optimize thermal design
may compromise the LM4836’s high power performance and
activate unwanted, though necessary, thermal shutdown
protection.
The MTE and LQ packages must have their DAPs soldered
to a copper pad on the PCB. The DAP’s PCB copper pad is
connected to a large plane of continuous unbroken copper.
This plane forms a thermal mass and heat sink and radiation
area. Place the heat sink area on either outside plane in the
case of a two-sided PCB, or on an inner layer of a board with
more than two layers. Connect the DAP copper pad to the
inner layer or backside copper heat sink area with 32(4x8)
(MTE) or 6(3x2) (LQ) vias. The via diameter should be
0.012in–0.013in with a 1.27mm pitch. Ensure efficient
thermal conductivity by plating-through and solder-filling the
vias.
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 2.5in2 (min) area is
necessary for 5V operation with a 4
load. Heatsink areas
not placed on the same PCB layer as the LM4836 should be
5in
2 (min) for the same supply voltage and load resistance.
The last two area recommendations apply for 25C ambient
temperature. Increase the area to compensate for ambient
temperatures above 25C. In systems using cooling fans, the
LM4836MTE 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 5.0in
2 inner layer copper plane heatsink,
the LM4836MTE can continuously drive a 3
load to full
power. The LM4836LQ achieves the same output power
level without forced air cooling. In all circumstances and
conditions, the junction temperature must be held below
150C to prevent activating the LM4836’s thermal shutdown
protection. The LM4836’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, fabrication,
and mounting an LQ (LLP) package is available in National
Semiconductor’s AN1187.
PCB LAYOUT AND SUPPLY REGULATION
CONSIDERATIONS FOR DRIVING 3
AND 4 LOADS
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 increas-
ingly 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, 0.1
trace resistance
reduces the output power dissipated by a 4
load from 2.1W
to 2.0W. This 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.
Poor power supply regulation adversely affects maximum
output power. A poorly regulated supply’s output voltage
decreases with increasing load current. Reduced supply
voltage causes decreased headroom, output signal clipping,
and reduced output power. Even with tightly regulated
supplies, trace resistance creates the same effects as poor
supply regulation. Therefore, making the power supply
traces as wide as possible helps maintain full output voltage
swing.
BRIDGE CONFIGURATION EXPLANATION
As shown in
Figure 1, the LM4836 consists of two pairs of
operational amplifiers, forming a two-channel (channel A and
channel B) stereo amplifier. (Though the following discusses
channel A, it applies equally to channel B.) External resistors
R
f and Ri set the closed-loop gain of Amp1A, whereas two
internal 20k
resistors set Amp2A’s gain at 1. The LM4836
drives a load, such as a speaker, connected between the two
amplifier outputs, OUTA and +OUTA.
Figure 1 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/R i)
(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.
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/(2
π2R
L)
Single-Ended
(2)
LM4836
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