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LT1812CS8 Datasheet(PDF) 12 Page - Linear Technology |
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LT1812CS8 Datasheet(HTML) 12 Page - Linear Technology |
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12 / 16 page ![]() 12 LT1812 junction temperature (TJ) is calculated from the ambient temperature (TA) and power dissipation (PD) as follows: TJ = TA + (PD • θJA) (Note 9) Power dissipation is composed of two parts. The first is due to the quiescent supply current and the second is due to on-chip dissipation caused by the load current. The worst-case load induced power occurs when the output voltage is at 1/2 of either supply voltage (or the maximum swing if less than 1/2 supply voltage). Therefore PDMAX is: PDMAX = (V + – V –)(ISMAX) + (V +/2)2/RL or PDMAX = (V + – V –)(ISMAX) + (V + – VOMAX)(VOMAX/RL) Example: LT1812CS5 at 70 °C, VS = ±5V, RL = 100Ω PDMAX = (10V)(4.5mA) + (2.5V)2/100Ω = 108mW TJMAX = 70°C + (108mW)(250°C/W) = 97°C Circuit Operation The LT1812 circuit topology is a true voltage feedback amplifier that has the slewing behavior of a current feed- back amplifier. The operation of the circuit can be under- stood by referring to the Simplified Schematic. The inputs are buffered by complementary NPN and PNP emitter followers that drive a 300 Ω resistor. The input voltage appears across the resistor generating currents that are mirrored into the high impedance node. Complementary followers form an output stage that 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. 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 capacitive loads (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 which improves the phase margin by moving the unity- gain cross 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 the total phase lag does not exceed 180 degrees (zero phase margin) and the amplifier remains stable. In this way, the LT1812 is stable with up to 1000pF capacitive loads in unity gain, and even higher capacitive loads in higher closed-loop gain configurations. 1812 SS OUT +IN –IN BIAS CONTROL RB V+ V– SHDN R1 300 Ω CC RC C SCHEMATIC SI PLIFIED APPLICATIO S I FOR ATIO |
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