10
LT6300
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
RMS
of power on to the 100
telephone line and assuming a 0.5dBm insertion loss in
the transformer. The quiescent current for the LT6300 is
set to 10mA per amplifier.
The power dissipated in the LT6300 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
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:
P
D
= P
QUIESCENT
+ P
Q(UPPER)
+ P
Q(LOWER)
P
D
= (V
+
– V
) • I
Q
+ (V
+
– V
OUTARMS
) •
I
LOAD
+ (V
– V
OUTBRMS
) • I
LOAD
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:
P
DQ
= 24V • 20mA = 480mW
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.
At full power to the line the driver power dissipation is:
P
D(FULL)
= 24V • 8mA + (12V – 2V
RMS
) • 57mA
RMS
+ [|–12V – (–2V
RMS
)|] • 57mA
RMS
P
D(FULL)
= 192mW + 570mW + 570mW = 1.332W
The junction temperature of the driver must be kept less
than the thermal shutdown temperature when processing
a signal. The junction temperature is determined from the
following expression:
T
J
= T
AMBIENT
(°C) + P
D(FULL)
(W) • θ
JA
(°C/W)
θ
JA
is the thermal resistance from the junction of the
LT6300 to the ambient air, which can be minimized by
heat-spreading PCB metal and airflow through the enclo-
sure as required. For the example given, assuming a
maximum ambient temperature of 50°C and keeping the
junction temperature of the LT6300 to 150°C maximum,
the maximum thermal resistance from junction to ambient
required is:
θ
JA MAX
CC
W
CW
()
.
./=
°°
150 50
1 332
75 1
APPLICATIO S I FOR ATIO
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Figure 7. I
Q
vs I
LOAD
I
LOAD
(mA)
240 200 160 –120 80 40 0 40 80 120 160 200 240
TOTAL I
Q
(mA)
10
15
20
6300 F07
5
0
25
11
LT6300
APPLICATIO S I FOR ATIO
WUUU
Heat Sinking Using PCB Metal
Designing a thermal management system is often a trial
and error process as it is never certain how effective it is
until it is manufactured and evaluated. As a general rule,
the more copper area of a PCB used for spreading heat
away from the driver package, the more the operating
junction temperature of the driver will be reduced. The
limit to this approach however is the need for very com-
pact circuit layout to allow more ports to be implemented
on any given size PCB.
To best extract heat from the GN16 package, a generous
area of top layer PCB metal should be connected to the four
corner pins (Pins 1, 8, 9 and 16). These pins are fused to
the leadframe where the LT6300 die is attached. It is
important to note that this heat spreading metal area is
electrically connected to the V
supply voltage.
Fortunately xDSL circuit boards use multiple layers of
metal for interconnection of components. Areas of metal
beneath the LT6300 connected together through several
small 13 mil vias can be effective in conducting heat away
from the driver package. The use of inner layer metal can
free up top and bottom layer PCB area for external compo-
nent placement.
When PCB cards containing multiple ports are inserted
into a rack in an enclosed cabinet, it is often necessary to
provide airflow through the cabinet and over the cards.
This is also very effective in reducing the junction-to-
ambient thermal resistance of each line driver. To a limit,
this thermal resistance can be reduced approximately
5°C/W for every 100lfpm of laminar airflow.
Layout and Passive Components
With a gain bandwidth product of 200MHz the LT6300
requires attention to detail in order to extract maximum
performance. Use a ground plane, short lead lengths and
a combination of RF-quality supply bypass capacitors (i.e.,
0.1µF). As the primary applications have high drive cur-
rent, use low ESR supply bypass capacitors (1µF to 10µF).
The parallel combination of the feedback resistor and gain
setting resistor on the inverting input can combine with
the input capacitance to form a pole that can cause
frequency peaking. In general, use feedback resistors of
1k or less.
Compensation
The LT6300 is stable in a gain 10 or higher for any supply
and resistive load. It is easily compensated for lower gains
with a single resistor or a resistor plus a capacitor.
Figure␣ 8 shows that for inverting gains, a resistor from the
inverting node to AC ground guarantees stability if the
parallel combination of R
C
and R
G
is less than or equal to
R
F
/9. For lowest distortion and DC output offset, a series
capacitor, C
C
, can be used to reduce the noise gain at
lower frequencies. The break frequency produced by R
C
and C
C
should be less than 5MHz to minimize peaking.
Figure 9 shows compensation in the noninverting configu-
ration. The R
C
, C
C
network acts similarly to the inverting
case. The input impedance is not reduced because the
network is bootstrapped. This network can also be placed
between the inverting input and an AC ground.
Figure 8. Compensation for Inverting Gains
R
G
R
C
V
O
V
I
C
C
(OPTIONAL)
+
6300 F08
R
F
=
–R
F
R
G
V
O
V
I
< 5MHz
1
2πR
C
C
C
(R
C
|| R
G
) R
F
/9
R
C
V
O
V
I
C
C
(OPTIONAL)
+
6300 F09
R
F
R
G
= 1 +
R
F
R
G
V
O
V
I
< 5MHz
1
2πR
C
C
C
(R
C
|| R
G
) R
F
/9
Figure 9. Compensation for Noninverting Gains
12
LT6300
APPLICATIO S I FOR ATIO
WUUU
Another compensation scheme for noninverting circuits is
shown in Figure 10. The circuit is unity gain at low fre-
quency and a gain of 1 + R
F
/R
G
at high frequency. The DC
output offset is reduced by a factor of ten. The techniques
of Figures 9 and 10 can be combined as shown in Fig-
ure␣ 11. The gain is unity at low frequencies, 1 + R
F
/R
G
at
mid-band and for stability, a gain of 10 or greater at high
frequencies.
In differential driver applications, as shown on the first
page of this data sheet, it is recommended that the gain
setting resistor be comprised of two equal value resistors
connected to a good AC ground at high frequencies. This
ensures that the feedback factor of each amplifier remains
less than 0.1 at any frequency. The midpoint of the
resistors can be directly connected to ground, with the
resulting DC gain to the V
OS
of the amplifiers, or just
bypassed to ground with a 1000pF or larger capacitor.
Line Driving Back-Termination
The standard method of cable or line back-termination is
shown in Figure 12. The cable/line is terminated in its
characteristic impedance (50, 75, 100, 135, etc.).
A back-termination resistor also equal to the chararacteristic
impedance should be used for maximum pulse fidelity of
outgoing signals, and to terminate the line for incoming
signals in a full-duplex application. There are three main
drawbacks to this approach. First, the power dissipated in
the load and back-termination resistors is equal so half of
the power delivered by the amplifier is wasted in the
termination resistor. Second, the signal is halved so the
gain of the amplifer must be doubled to have the same
overall gain to the load. The increase in gain increases
noise and decreases bandwidth (which can also increase
distortion). Third, the output swing of the amplifier is
doubled which can limit the power it can deliver to the load
for a given power supply voltage.
An alternate method of back-termination is shown in
Figure 13. Positive feedback increases the effective back-
termination resistance so R
BT
can be reduced by a factor
+
6300 F10
R
F
R
G
V
i
V
O
C
C
< 5MHz
1
2πR
G
C
C
R
G
R
F
/9
= 1 (LOW FREQUENCIES)
(HIGH FREQUENCIES)
V
O
V
I
= 1 +
R
F
R
G
Figure 10. Alternate Noninverting Compensation
R
C
V
O
V
I
C
C
+
6300 F11
R
F
R
G
C
BIG
R
F
R
G
= 1 AT LOW FREQUENCIES
= 1 + AT MEDIUM FREQUENCIES
R
F
(R
C
|| R
G
)
= 1 + AT HIGH FREQUENCIES
V
O
V
I
Figure 11. Combination Compensation
+
6300 F12
R
F
R
BT
CABLE OR LINE WITH
CHARACTERISTIC IMPEDANCE R
L
R
G
V
O
V
I
R
L
(1 + R
F
/R
G
)
=
V
O
V
I
1
2
R
BT
= R
L
Figure 12. Standard Cable/Line Back Termination
+
6300 F13
R
F
R
BT
R
P2
R
P1
R
G
V
I
V
A
V
P
V
O
R
L
R
F
R
G
1 +
R
L
n
=
V
O
V
I
= 1 –
1
n
FOR R
BT
=
()
R
F
R
G
1 +
()
R
P1
R
P1
+ R
P2
R
P1
R
P2
+ R
P1
R
P2
/(R
P2
+ R
P1
)
()
1 + 1/n
Figure 13. Back Termination Using Postive Feedback

LT6300IGN#TRPBF

Mfr. #:
Manufacturer:
Analog Devices Inc.
Description:
High Speed Operational Amplifiers Dual 500mA OA / DSL DRIVER
Lifecycle:
New from this manufacturer.
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