LT1739IUE#TR Linear Technology, LT1739IUE#TR Datasheet - Page 9
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LT1739IUE#TR
Manufacturer Part Number
LT1739IUE#TR
Description
IC AMP XDSL LINE DVR DUAL 12-DFN
Manufacturer
Linear Technology
Type
Line Driver, Transmitterr
Datasheet
1.LT1739IUE.pdf
(20 pages)
Specifications of LT1739IUE#TR
Number Of Drivers/receivers
2/0
Voltage - Supply
5 V ~ 12 V
Mounting Type
Surface Mount
Package / Case
12-DFN
Lead Free Status / RoHS Status
Contains lead / RoHS non-compliant
Protocol
-
Other names
LT1739IUETR
Available stocks
Company
Part Number
Manufacturer
Quantity
Price
APPLICATIO S I FOR ATIO
the design of the PCB and card enclosure to take measures
to spread the heat developed in the driver away to the
ambient environment to prevent thermal shutdown (which
occurs when the junction temperature of the LT1739
exceeds 165 C).
Estimating Line Driver Power Dissipation
Figure 6 is a typical ADSL application shown for the
purpose of estimating the power dissipation in the line
driver. Due to the complex nature of the DMT signal,
which looks very much like noise, it is easiest to use the
RMS values of voltages and currents for estimating the
driver power dissipation. The voltage and current levels
shown for this example are for a full-rate ADSL signal
driving 20dBm or 100mW
telephone line and assuming a 0.5dBm insertion loss in
the transformer. The quiescent current for the LT1739 is
set to 10mA per amplifier.
The power dissipated in the LT1739 is a combination of the
quiescent power and the output stage power when driving
a signal. The two amplifiers are configured to place a
differential signal on to the line. The Class AB output stage
in each amplifier will simultaneously dissipate power in
1000pF
U
+IN
–IN
U
RMS
110
110
of power on to the 100
20mA DC
W
Figure 6. Estimating Line Driver Power Dissipation
+
–
–
+
A
B
1k
1k
–12V
12V
I
LOAD
SHDN
SHDNREF
24.9k – SETS I
–2V
U
2V
= 57mA
RMS
RMS
17.4
17.4
RMS
Q
PER AMPLIFIER = 10mA
1:1.7
1739 F06
the upper power transistor of one amplifier, while sourc-
ing current, and the lower power transistor of the other
amplifier, while sinking current. The total device power
dissipation is then:
With no signal being placed on the line and the amplifier
biased for 10mA per amplifier supply current, the quies-
cent driver power dissipation is:
This can be reduced in many applications by operating
with a lower quiescent current value.
When driving a load, a large percentage of the amplifier
quiescent current is diverted to the output stage and
becomes part of the load current. Figure 7 illustrates the
total amount of biasing current flowing between the + and
– power supplies through the amplifiers as a function of
load current. As much as 60% of the quiescent no load
operating current is diverted to the load.
P
P
P
D
D
DQ
= P
= (V
= 24V • 20mA = 480mW
I
LOAD
QUIESCENT
+
– V
+ (V
–
) • I
–
+ P
Q
– V
100
+ (V
Q(UPPER)
OUTBRMS
+
– V
OUTARMS
+ P
) • I
3.16V
Q(LOWER)
LOAD
RMS
) •
LT1739
1739fas, sn1739
9