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LT1353CS 数据表(PDF) 10 Page - Linear Technology

部件名 LT1353CS
功能描述  Dual and Quad 250uA, 3MHz, 200V/us Operational Amplifiers
PDF  12 Pages
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制造商  LINER [Linear Technology]
网页  http://www.linear.com
标志 LINER - Linear Technology

LT1353CS 数据表(HTML) 10 Page - Linear Technology

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LT1352/LT1353
APPLICATIONS INFORMATION
mended for applications where DC accuracy must be
maximized. The inputs can withstand differential input
voltages of up to 10V without damage and need no
clamping or source resistance for protection. Differential
inputs generate large supply currents (up to 40mA) as
required for high slew rates. Typically power dissipation
does not significantly increase because of the low duty
cycle of the transient inputs. If the device is used as a
comparator with sustained differential inputs, excessive
power dissipation may result.
Circuit Operation
The LT1352/LT1353 circuit topology is a true voltage
feedback amplifier that has the slewing behavior of a
current feedback amplifier. The operation of the circuit can
be understood by referring to the Simplified Schematic.
The inputs are buffered by complementary NPN and PNP
emitter followers which drive R1, a 1k resistor. The input
voltage appears across the resistor generating currents
which are mirrored into the high impedance node and
compensation capacitor CT. Complementary followers
form an output stage which buffers the gain node from the
load. The output devices Q19 and Q22 are connected to
form a composite PNP and a composite NPN.
The bandwidth is set by the input resistor and the capaci-
tance on the high impedance node. The slew rate is
determined by the current available to charge the high
impedance node capacitance. This current is the differen-
tial input voltage divided by R1, so the slew rate is
proportional to the input. Highest slew rates are therefore
seen in the lowest gain configurations. For example, a 10V
output step in a gain of 10 has only a 1V input step whereas
the same output step in unity gain has a 10 times greater
input step. The graph Slew Rate vs Input Level illustrates
this relationship. In higher gain configurations the large-
signal performance and the small-signal performance
both look like a single pole response.
Capacitive load compensation is provided by the RC, CC
network which is bootstrapped across the output stage.
When the amplifier is driving a light load the network has
no effect. When driving a capacitive load (or a low value
resistive load) the network is incompletely bootstrapped
and adds to the compensation at the high impedance
node. The added capacitance slows down the amplifier
and a zero is created by the RC combination, both of which
improve the phase margin. The design ensures that even
for very large load capacitances, the total phase lag can
never exceed 180 degrees (zero phase margin) and the
amplifier remains stable.
Power Dissipation
The LT1352/LT1353 combine high speed and large output
drive in small packages. Because of the wide supply
voltage range, it is possible to exceed the maximum
junction temperature of 150
°C under certain conditions.
Maximum junction temperature TJ is calculated from the
ambient temperature TA and power dissipation PD as
follows:
LT1352CN8: TJ = TA + (PD)(130°C/W)
LT1352CS8: TJ = TA + (PD)(190°C/W)
LT1353CS:
TJ = TA + (PD)(150°C/W)
Worst-case power dissipation occurs at the maximum
supply current and when the output voltage is at 1/2 of
either supply voltage (or the maximum swing if less than
1/2 supply voltage). For each amplifier PD(MAX) is:
PD(MAX) =(V
+ – V)(IS(MAX)) + (V+/2)2/RL or
(V+ – V )(IS(MAX)) + (V+ – VMAX)(IMAX)
Example: LT1353 in S14 at 85
°C, VS = ±15V, RL = 500Ω,
VOUT = ±5V (±10mA)
PD(MAX) = (30V)(380µA) + (15V – 5V)(10mA) = 111mW
TJ = 85°C + (4)(111mW)(150°C/W) = 152°C



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