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ADA4817-2ACPZ-R2 数据表(PDF) 14 Page - Analog Devices

部件名 ADA4817-2ACPZ-R2
功能描述  Low Noise, 1 GHz FastFET Op Amps
PDF  24 Pages
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制造商  AD [Analog Devices]
网页  http://www.analog.com
标志 AD - Analog Devices

ADA4817-2ACPZ-R2 数据表(HTML) 14 Page - Analog Devices

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ADA4817-1/ADA4817-2
Rev. 0 | Page 14 of 24
The voltage error due to Ib+ and Ib– is minimized if RS = RF || RG
(though with the ADA4817-1/ADA4817-2 input currents in the
picoamp range, this is likely not a concern). To include common-
mode effects and power supply rejection effects, total VOS can be
modeled by
CMR
V
PSR
V
V
V
CM
S
nom
OS
OS
Δ
Δ
+
+
=
(11)
where:
is the offset voltage specified at nominal conditions.
ΔVS is the change in power supply from nominal conditions.
PSR is the power supply rejection.
ΔVCM is the change in common-mode voltage from nominal
conditions.
CMR is the common-mode rejection.
nom
OS
V
WIDEBAND OPERATION
The ADA4817-1/ADA4817-2 provides excellent performance as a
high speed buffer. Figure 38 shows the circuit used for wideband
characterization for high gains. The impedance at the summing
junction (RF || RG) forms a pole in the amplifier’s loop response
with the amplifier’s input capacitance of 1.5 pF. This pole can
cause peaking and ringing if its frequency is too low. Feedback
resistances of 100 Ω to 400 Ω are recommended, because they
minimize the peaking and they do not degrade the perfor-
mance of the output stage. Peaking in the frequency response
can also be compensated for with a small feedback capacitor
(CF) in parallel with the feedback resistor, or a series resistor
in the noninverting input as shown in Figure 42.
The distortion performance depends on a number of variables:
The closed-loop gain of the application
Whether it is inverting or noninverting
Amplifier loading
Signal frequency and amplitude
Board layout
The best performance is usually obtained in the G + 1
configuration with no feedback resistance, big output
load resistors, and small board parasitic capacitances.
DRIVING CAPACITIVE LOADS
In general, high speed amplifiers have a difficult time driving
capacitive loads. This is particularly true in low closed-loop
gains, where the phase margin is the lowest. The difficulty
arises because the load capacitance, CL, forms a pole with the
output resistance, RO, of the amplifier. The pole can be described
by the following equation:
L
O
P
C
R
f
1
=
(12)
If this pole occurs too close to the unity-gain crossover point,
the phase margin degrades. This is due to the additional phase
loss associated with the pole.
Note that such capacitance introduces significant peaking in the
frequency response. Larger capacitance values can be driven but
must use a snubbing resistor (RSNUB) at the output of the amplifier,
as shown in Figure 42. Adding a small series resistor, RSNUB,
creates a zero that cancels the pole introduced by the load
capacitance. Typical values for RSNUB can range from 10 Ω to
50 Ω. The value is typically based on the circuit requirements.
Figure 42 also shows another way to reduce the effect of the
pole created by the capacitive load (CL) by placing a capacitor
(CF) in the feedback loop parallel to the feedback resistor
Typical capacitor values can range from 0.5 pF to 2 pF.
Figure 43 shows the effect of adding a feedback capacitor
to the frequency response.
VIN
VOUT
0.1µF
0.1µF
10µF
+VS
–VS
49.9Ω
RL
0.1µF
CL
10µF
RF
RSNUB
CF
RG
Figure 42. RSNUB or CF Used to Reduce Peaking
THERMAL CONSIDERATIONS
With 10 V power supplies and 19 mA quiescent current, the
ADA4817-1/ADA4817-2 dissipate 190 mW with no load. This
implies that in the LFCSP, whose thermal resistance is 94°C/W
for the ADA4817-1and 64°C/W for the ADA4817-2, the junction
temperature is typically almost 25° higher than the ambient tem-
perature. The ADA4817-1/ADA4817-2 are designed to maintain
a constant bandwidth over temperature; therefore, an initial ramp
up of the current consumption during warm-up is expected. The
VOS temperature drift is below 12 μV/°C; therefore, it can change
up to 0.3 mV due to warm-up effects for an ADA4817-1/
ADA4817-2 in a LFCSP on 10 V. The input bias current
increases by a factor of 1.7 for every 10°C rise in temperature.
Heavy loads increase power dissipation and raise the chip
junction temperature as described in the Absolute Maximum
Ratings section. Care should be taken not to exceed the rated
power dissipation of the package.



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