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LM7372IMAX/NOPB Datasheet(PDF) 15 Page - Texas Instruments

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Part # LM7372IMAX/NOPB
Description  LM7372 High Speed, High Output Current, Dual Operational Amplifier
PDF  28 Pages
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Manufacturer  TI1 [Texas Instruments]
Direct Link  http://www.ti.com
Logo TI1 - Texas Instruments

LM7372IMAX/NOPB Datasheet(HTML) 15 Page - Texas Instruments

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LM7372
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SNOS926F – MAY 1999 – REVISED SEPTEMBER 2014
Application Details (continued)
For a Class B output stage, one transistor of the output pair will conduct the load current as the output voltage
swings positive, with the other transistor drawing no current, and hence dissipating no power. During the other
half of the signal swing, this situation is reversed, with the lower transistor sinking the load current and the upper
transistor cut off. The current in each transistor will be a half wave rectified version of the total load current.
Ideally neither transistor will dissipate power when there is no signal swing, but will dissipate increasing power as
the output current increases. However, as the signal voltage across the load increases with load current, the
voltage across the output transistor (which is the difference voltage between the supply voltage and the
instantaneous voltage across the load) will decrease and a point will be reached where the dissipation in the
transistor will begin to decrease again. If the signal is driven into a square wave, ideally the transistor dissipation
will fall to zero.
Therefore, for each amplifier, with an effective load each of RL and a sine wave source, integration over the half
cycle with a supply voltage VS and a load voltage VL yields the average power dissipation of:
PD = VSVL/πRL - VL
2/2R
L
where
•
VS is the supply voltage
•
VL is the peak signal swing across the load RL
(2)
For the package, the power dissipation will be doubled since there are two amplifiers in the package, each
contributing half the swing across the load.
The circuit in Single Supply Application, Figure 24, is using the LM7372 as the upstream driver in an ADSL
application with Discrete MultiTone modulation. With DMT the upstream signal is spread into 32 adjacent
channels each 4 kHz wide. For transmission over POTS, the regular telephone service, this upstream signal from
the CPE (Customer Premise Equipment) occupies a frequency band from around 20 kHz up to a maximum
frequency of 135 kHz. At first sight, these relatively low transmission frequencies certainly do not seem to require
the use of very high speed amplifiers with GBW products in the range of hundreds of megahertz. However, the
close spacing of multiple channels places stringent requirements on the linearity of the amplifier, since non-
linearities in the presence of multiple tones will cause harmonic products to be generated that can easily interfere
with the higher frequency down stream signals also present on the line. The need to deliver 3rd Harmonic
distortion terms lower than
−75 dBc is the reason for the LM7372 quiescent current levels. Each amplifier is
running over 3mA in the output stage alone in order to minimize crossover distortion. The xDSL signal levels are
adjusted to provide a given power level on the line, and in the case of ADSL, this is an average power of 13
dBm. For a line with a characteristic impedance of 100
Ω this is only 20 mW (= 1 mW x 10(13/10)). Because the
transformer shown in Figure 24 is part of a transceiver circuit, two back-termination resistors are connected in
series with each amplifier output. Therefore the equivalent RL for each amplifier is also 100 Ω, and each amplifier
is required to deliver 20 mW to this load.
Since VL
2/2RL = 20mW then V
L = 2V(peak).
(3)
Using Equation 2 with this value for signal swing and a 24V supply, the internal power dissipation per amplifier is
132.8mW. Adding the quiescent power dissipation to the amplifier dissipation gives the total package internal
power dissipation as
PD(TOTAL) = 312mW + (2 x 132.8mW) = 578mW
(4)
This result is actually quite pessimistic because it assumes that the dissipation as a result of load current is
simply added to the dissipation as a result of quiescent current. This is not correct, since the AB bias current in
the output stage is diverted to load current as the signal swing amplitude increases from zero. In fact with load
currents in excess of 3.3 mA, all the bias current is flowing in the load, consequently reducing the quiescent
component of power dissipation. Also, it assumes a sine wave signal waveform when the actual waveform is
composed of many tones of different phases and amplitudes which may demonstrate lower average power
dissipation levels.
Copyright © 1999–2014, Texas Instruments Incorporated
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