LM8261

SNOS469I – APRIL 2000 – REVISED MARCH 2013

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Figure 52. Input Stage Current vs. Differential Input Voltage

B) Output Stage

The output stage Figure 51 is comprised of complementary NPN and PNP common-emitter stages to permit

The frequency compensation circuit includes Miller capacitors from collector to base of each output transistor

high, and the Miller effect increases the effective value of the capacitors thereby stabilizing the Op Amp. Large

capacitive loads greatly decrease the high frequency gain of the output transistors thus lowering the effective

internal Miller capacitance - the internal pole frequency increases at the same time a low frequency pole is

created at the Op Amp output due to the large load capacitor. In this fashion, the internal dominant pole

compensation, which works by reducing the loop gain to less than 0dB when the phase shift around the feedback

loop is more than 180°C, varies with the amount of capacitive load and becomes less dominant when the load

capacitor has increased enough. Hence the Op Amp is very stable even at high values of load capacitance

resulting in the uncharacteristic feature of stability under all capacitive loads.

DRIVING CAPACITIVE LOADS

The LM8261 is specifically designed to drive unlimited capacitive loads without oscillations (See Settling Time

and Percent Overshoot vs. Cap Load plot, Figure 32). In addition, the output current handling capability of the

device allows for good slewing characteristics even with large capacitive loads (see Slew Rate vs. Cap Load

plots). The combination of these features is ideal for applications such as TFT flat panel buffers, A/D converter

input amplifiers, etc.

However, as in most Op Amps, addition of a series isolation resistor between the Op Amp and the capacitive

load improves the settling and overshoot performance.

Output current drive is an important parameter when driving capacitive loads. This parameter will determine how

fast the output voltage can change. Referring to the Slew Rate vs. Cap Load Plots (Figure 33, Figure 34,

Figure 35, and Figure 36), two distinct regions can be identified. Below about 10,000pF, the output Slew Rate is

solely determined by the Op Amp's compensation capacitor value and available current into that capacitor.

Beyond 10nF, the Slew Rate is determined by the Op Amp's available output current. Note that because of the

lower output sourcing current compared to the sinking one, the Slew Rate limit under heavy capacitive loading is

determined by the positive transitions. An estimate of positive and negative slew rates for loads larger than

100nF can be made by dividing the short circuit current value by the capacitor.

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