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LM4954TL/NOPB Datasheet(PDF) 13 Page - Texas Instruments

Part # LM4954TL/NOPB
Description  LM4954 Boomer™ Audio Power Amplifier Series High Voltage 3 Watt Audio Power Amplifier
PDF  23 Pages
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Manufacturer  TI2 [Texas Instruments]
Direct Link  https://www.ti.com
Logo TI2 - Texas Instruments

LM4954TL/NOPB Datasheet(HTML) 13 Page - Texas Instruments

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LM4954
www.ti.com
SNAS292B – JUNE 2005 – REVISED APRIL 2013
SHUTDOWN FUNCTION
In order to reduce power consumption while not in use, the LM4954 contains a shutdown pin to externally turn off
the amplifier's bias circuitry. This shutdown feature turns the amplifier off when a logic low is placed on the
shutdown pin. By switching the shutdown pin to ground, the LM4954 supply current draw will be minimized in idle
mode. While the device will be disabled with shutdown pin voltages less than 0.4VDC, the idle current may be
greater than the typical value of 0.01µA. (Idle current is measured with the shutdown pin tied to ground). The
LM4954 has an internal 75k
Ω pull-down resistor. If the shutdown pin is left floating the IC will automatically enter
shutdown mode.
PROPER SELECTION OF EXTERNAL COMPONENTS
Proper selection of external components in applications using integrated power amplifiers is critical to optimize
device and system performance. While the LM4954 is tolerant of external component combinations,
consideration to component values must be used to maximize overall system quality.
The LM4954 is unity-gain stable which gives the designer maximum system flexibility. The LM4954 should be
used in low gain configurations to minimize THD+N values, and maximize the signal to noise ratio. Low gain
configurations require large input signals to obtain a given output power. Input signals equal to or greater than 1
Vrms are available from sources such as audio codecs. Please refer to the section, AUDIO POWER AMPLIFIER
DESIGN, for a more complete explanation of proper gain selection.
Besides gain, one of the major considerations is the closed-loop bandwidth of the amplifier. To a large extent, the
bandwidth is dictated by the choice of external components shown in Figure 1. The input coupling capacitor, Ci,
forms a first order high pass filter which limits low frequency response. This value should be chosen based on
needed frequency response for a few distinct reasons.
Selection Of Input Capacitor Size
Large input capacitors are both expensive and space hungry for portable designs. Clearly, a certain sized
capacitor is needed to couple in low frequencies without severe attenuation. But in many cases the speakers
used in portable systems, whether internal or external, have little ability to reproduce signals below 100Hz to
150Hz. Thus, using a large input capacitor may not increase actual system performance.
In addition to system cost and size, click and pop performance is affected by the size of the input coupling
capacitor, Ci. A larger input coupling capacitor requires more charge to reach its quiescent DC voltage (nominally
1/2VDD). This charge comes from the output via the feedback and is apt to create pops upon device enable.
Thus, by minimizing the capacitor size based on necessary low frequency response, turn-on pops can be
minimized.
Besides minimizing the input capacitor size, careful consideration should be paid to the bypass capacitor value.
Choosing CB equal to 2.2µF along with a small value of Ci (in the range of 0.1µF to 0.39µF), should produce a
virtually clickless and popless shutdown function. While the device will function properly, (no oscillations or
motorboating), with CB equal to 0.1µF.
AUDIO POWER AMPLIFIER DESIGN
A designer must first determine the minimum supply rail to obtain the specified output power. By extrapolating
from the Output Power vs Supply Voltage graphs in the Typical Performance Characteristics section, the supply
rail can be easily found.
At this time, the designer must make sure that the power supply choice along with the output impedance does
not violate the conditions explained in the POWER DISSIPATION section.
Once the power dissipation equations have been addressed, the required differential gain can be determined
from Equation 3 and Equation 4.
(3)
AVD = (Rf/Ri) 2
(4)
Copyright © 2005–2013, Texas Instruments Incorporated
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