Datasheet

R
OUT
-
+
V
IN
R
F
C
F
R
IN
R
L
C
L
R
S
0
UNSTABLE
ROC = 40 dB/decade
STABLE
ROC ± 20 dB/decade
FREQUENCY (Hz)
GAIN
LM6211
SNOSAH2C FEBRUARY 2006REVISED MARCH 2013
www.ti.com
STABILITY OF OP AMP CIRCUITS
Stability and Capacitive Loading
The LM6211 is designed to be unity gain stable for moderate capacitive loads, around 100 pF. That is, if
connected in a unity gain buffer configuration, the LM6211 will resist oscillation unless the capacitive load is
higher than about 100 pF. For higher capacitive loads, the phase margin of the op amp reduces significantly and
it tends to oscillate. This is because an op amp cannot be designed to be stable for high capacitive loads without
either sacrificing bandwidth or supplying higher current. Hence, for driving higher capacitive loads, the LM6211
needs to be externally compensated.
Figure 35. Gain vs. Frequency for an Op Amp
An op amp, ideally, has a dominant pole close to DC, which causes its gain to decay at the rate of 20 dB/decade
with respect to frequency. If this rate of decay, also known as the rate of closure (ROC), remains at 20
dB/decade at the unity gain bandwidth of the op amp, the op amp is stable. If, however, a large capacitance is
added to the output of the op amp, it combines with the output impedance of the op amp to create another pole
in its frequency response before its unity gain frequency (Figure 35). This increases the ROC to 40 dB/decade
and causes instability.
In such a case a number of techniques can be used to restore stability to the circuit. The idea behind all these
schemes is to modify the frequency response such that it can be restored to a ROC of 20 dB/decade, which
ensures stability.
In the Loop Compensation
Figure 36 illustrates a compensation technique, known as ‘in the loop’ compensation, that employs an RC
feedback circuit within the feedback loop to stabilize a non-inverting amplifier configuration. A small series
resistance, R
S
, is used to isolate the amplifier output from the load capacitance, C
L
, and a small capacitance, C
F
,
is inserted across the feedback resistor to bypass C
L
at higher frequencies.
Figure 36. In the Loop Compensation
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