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LT1353 数据表(PDF) 10 Page - Linear Technology |
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LT1353 数据表(HTML) 10 Page - Linear Technology |
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10 / 16 page ![]() 10 LT1352/LT1353 13523fa APPLICATIONS INFORMATION applications where DC accuracy must be maximized. The inputs can withstand transient differential input voltages up to 10V without damage and need no clamping or source resistance for protection. Differential inputs, however, generate large supply currents (tens of mA) as required for high slew rates. If the device is used with sustained differential inputs, the average supply current will in- crease, excessive power dissipation will result and the part may be damaged. The part should not be used as a comparator, peak detector or other open-loop applica- tion with large, sustained differential inputs. Under normal, closed-loop operation, an increase of power dis- sipation is only noticeable in applications with large slewing outputs and is proportional to the magnitude of the differential input voltage and the percent of time that the inputs are apart. Measure the average supply current for the application in order to calculate the power dissipation. 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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