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| 型号： | LT1359IS14#TRPBF |
| 厂商： | Linear Technology |
| 文件页数： | 3/16页 |
| 文件大小： | 0K |
| 描述： | IC OP-AMP HISPD 25MHZ QD 14SOIC |
| 标准包装： | 2,500 |
| 系列： | C-Load™ |
| 放大器类型： | 电压反馈 |
| 电路数： | 4 |
| 转换速率： | 600 V/µs |
| 增益带宽积： | 25MHz |
| 电流 - 输入偏压： | 120nA |
| 电压 - 输入偏移： | 200µV |
| 电流 - 电源： | 2mA |
| 电流 - 输出 / 通道： | 30mA |
| 电压 - 电源，单路/双路(±)： | ±2.5 V ~ 15 V |
| 工作温度： | -40°C ~ 85°C |
| 安装类型： | 表面贴装 |
| 封装/外壳： | 14-SOIC（0.154"，3.90mm 宽） |
| 供应商设备封装： | 14-SO |
| 包装： | 带卷 (TR) |
11
LT1358/LT1359
135859fb
Circuit Operation
The LT1358/LT1359 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 a 500
resistor. The input
voltage appears across the resistor generating currents
which are mirrored into the high impedance node. Comple-
mentary followers form an output stage which buffers the
gain node from the load. The bandwidth is set by the input
resistor and the capacitance on the high impedance node.
The slew rate is determined by the current available to
charge the gain node capacitance. This current is the
differential 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 curve of Slew Rate vs Input Level
illustrates this relationship. The LT1358/LT1359 are tested
for slew rate in a gain of –2 so higher slew rates can be
expected in gains of 1 and –1, and lower slew rates in
higher gain configurations.
The RC network across the output stage is bootstrapped
when the amplifier is driving a light or moderate load and
has no effect under normal operation. When driving a
capacitive load (or a low value resistive load) the network
is incompletely bootstrapped and adds to the compensa-
tion at the high impedance node. The added capacitance
slows down the amplifier which improves the phase
margin by moving the unity-gain frequency away from the
pole formed by the output impedance and the capacitive
load. The zero created by the RC combination adds phase
to ensure 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 LT1358/LT1359 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 under certain conditions. Maximum
junction temperature (TJ) is calculated from the ambient
temperature (TA) and power dissipation (PD) as follows:
LT1358N8: TJ = TA + (PD x 130°C/W)
LT1358S8: TJ = TA + (PD x 190°C/W)
LT1359N:
TJ = TA + (PD x 110°C/W)
LT1359S:
TJ = TA + (PD x 150°C/W)
LT1359S14: TJ = TA + (PD x 160°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 PDMAX is:
PDMAX = (V+ – V–)(ISMAX) + (V+/2)2/RL
Example: LT1358 in S8 at 70
°C, VS = ±15V, RL = 500
PDMAX = (30V)(2.9mA) + (7.5V)2/500 = 200mW
TJMAX = 70°C + (2 x 200mW)(190°C/W) = 146°C
APPLICATIO S I FOR ATIO
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