参数资料
型号: EVAL-PRAOPAMP-1RZ
厂商: Analog Devices Inc
文件页数: 3/4页
文件大小: 0K
描述: ADAPTOR BOARD SINGLE AMP 8SOIC
标准包装: 1
每 IC 通道数: 1 - 单
放大器类型: 通用
板类型: 裸(未填充)
已供物品:
已用 IC / 零件: 8-SOIC 封装

AN-732
at the positive input terminal of the ampli?er, denoted as
V+ = BL+. This continues until the capacitor voltage
reaches the positive threshold V TH , at which point
the bistable multivibrator switches to the other stable
state in which V O = L– and V+ = BL–. This is shown in
Figure 5.
The capacitor then begins to discharge, and its voltage,
V–, decreases exponentially toward L–. This continues
until V– reaches the negative threshold V TL , at which time
the bistable multivibrator switches to the positive output
state, and the cycle repeats itself.
It is important to note that the frequency of the square
wave being generated, f O , depends only on the external
components being used. Any variation in L+ will cause
V+ to vary in proportion, ensuring the same transition
time and the same oscillation frequency. The maximum
operating frequency is determined by the amplifier
speed, which can be increased signi?cantly by using
faster devices.
The lowest operating frequency depends on the practical
upper limits set by R7 and C9.
Using the name convention outlined on the PRA OPAMP
evaluation board, the circuit should be connected as
follows:
R L = 10k
C L = 2nF
GND
TIME (10 s/DIV)
Figure 8. Capacitive Load Drive with Resistor
EXTERNAL COMPENSATION TECHNIQUES
Series Resistor Compensation
The use of external compensation networks may be
required to optimize certain applications. Figure 6 is a
typical representation of a series resistor compensa-
tion for stabilizing an op amp driving capacitive load. The
stabilizing effect of the series resistor isolates the op amp
output and the feedback network from the capacitive
load. The required amount of series resistance depends
B = R4/(R4 + R9); feedback factor (noninverting input)
on the part used, but values of 5
to 50
are usually
T = 2R7
C9
ln((1 + B)/(1 – B)); period of oscillation
suf ?cient to prevent local resonance. The disadvantages
of this technique are a reduction in gain accuracy and
f O = 1/T; oscillation frequency
extra distortion when driving nonlinear loads.
V IN
R02
C L
R L
V OUT
V IN
R S
C S
C L
R L
V OUT
Figure 6. Series Resistor Compensation
R L = 10k
C L = 2nF
GND
TIME (10 s/DIV)
Figure 7. Capacitive Load Drive Without Resistor
REV. A
–3–
Figure 9. Snubber Network
GND
TIME (10 s/DIV)
Figure 10. Capacitive Load Drive Without Snubber
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