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AD8551AR 参数 Datasheet PDF下载

AD8551AR图片预览
型号: AD8551AR
PDF下载: 下载PDF文件 查看货源
内容描述: 零漂移,单电源,轨到轨输入/输出运算放大器 [Zero-Drift, Single-Supply, Rail-to-Rail Input/Output Operational Amplifiers]
分类和应用: 运算放大器
文件页数/大小: 20 页 / 265 K
品牌: ADI [ ADI ]
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AD8551/AD8552/AD8554  
Broadband and External Resistor Noise Considerations  
The total broadband noise output from any amplifier is primarily  
a function of three types of noise: Input voltage noise from the  
amplifier, input current noise from the amplifier and Johnson  
noise from the external resistors used around the amplifier. Input  
voltage noise, or en, is strictly a function of the amplifier used.  
The Johnson noise from a resistor is a function of the resistance  
and the temperature. Input current noise, or in, creates an equiva-  
lent voltage noise proportional to the resistors used around the  
amplifier. These noise sources are not correlated with each other  
and their combined noise sums in a root-squared-sum fashion.  
The full equation is given as:  
Input Overvoltage Protection  
Although the AD855x is a rail-to-rail input amplifier, care should  
be taken to ensure that the potential difference between the in-  
puts does not exceed +5 V. Under normal operating conditions,  
the amplifier will correct its output to ensure the two inputs are at  
the same voltage. However, if the device is configured as a com-  
parator, or is under some unusual operating condition, the input  
voltages may be forced to different potentials. This could cause  
excessive current to flow through internal diodes in the AD855x  
used to protect the input stage against overvoltage.  
If either input exceeds either supply rail by more than 0.3 V, large  
amounts of current will begin to flow through the ESD protection  
diodes in the amplifier. These diodes are connected between the  
inputs and each supply rail to protect the input transistors against  
an electrostatic discharge event and are normally reverse-biased.  
However, if the input voltage exceeds the supply voltage, these  
ESD diodes will become forward-biased. Without current limit-  
ing, excessive amounts of current could flow through these diodes  
causing permanent damage to the device. If inputs are subject to  
overvoltage, appropriate series resistors should be inserted to  
limit the diode current to less than 2 mA maximum.  
1
2
)
2
en, TOTAL = en2 + 4kTr + i r  
(15)  
(
S
n S  
Where, en = The input voltage noise of the amplifier,  
in = The input current noise of the amplifier,  
rS = Source resistance connected to the noninverting  
terminal,  
k = Boltzmann’s constant (1.38 ϫ 10-23 J/K)  
T = Ambient temperature in Kelvin (K = 273.15 + °C)  
Output Phase Reversal  
The input voltage noise density, en of the AD855x is 42 nV/Hz,  
and the input noise, in, is 2 fA/Hz. The en, TOTAL will be domi-  
nated by input voltage noise provided the source resistance is less  
than 106 k. With source resistance greater than 106 k, the  
overall noise of the system will be dominated by the Johnson  
noise of the resistor itself.  
Output phase reversal occurs in some amplifiers when the input  
common-mode voltage range is exceeded. As common-mode volt-  
age is moved outside of the common-mode range, the outputs of  
these amplifiers will suddenly jump in the opposite direction to the  
supply rail. This is the result of the differential input pair shutting  
down, causing a radical shifting of internal voltages which results in  
the erratic output behavior.  
Because the input current noise of the AD855x is very small, in  
does not become a dominant term unless rS is greater than 4 G,  
which is an impractical value of source resistance.  
The AD855x amplifier has been carefully designed to prevent  
any output phase reversal, provided both inputs are maintained  
within the supply voltages. If one or both inputs could exceed  
either supply voltage, a resistor should be placed in series with  
the input to limit the current to less than 2 mA. This will ensure  
the output will not reverse its phase.  
The total noise, en, TOTAL, is expressed in volts per square-root  
Hertz, and the equivalent rms noise over a certain bandwidth  
can be found as:  
(16)  
en = en, TOTAL × BW  
Capacitive Load Drive  
Where BW is the bandwidth of interest in Hertz.  
The AD855x has excellent capacitive load driving capabilities  
and can safely drive up to 10 nF from a single +5 V supply.  
Although the device is stable, capacitive loading will limit the  
bandwidth of the amplifier. Capacitive loads will also increase  
the amount of overshoot and ringing at the output. An R-C  
snubber network, Figure 54, can be used to compensate the  
amplifier against capacitive load ringing and overshoot.  
For a complete treatise on circuit noise analysis, please refer to the  
1995 Linear Design Seminar book available from Analog Devices.  
Output Overdrive Recovery  
The AD855x amplifiers have an excellent overdrive recovery of  
only 200 µs from either supply rail. This characteristic is particu-  
larly difficult for autocorrection amplifiers, as the nulling amplifier  
requires a nontrivial amount of time to error correct the main am-  
plifier back to a valid output. Figure 23 and Figure 24 show the  
positive and negative overdrive recovery time for the AD855x.  
+5V  
V
AD855x  
OUT  
The output overdrive recovery for an autocorrection amplifier is  
defined as the time it takes for the output to correct to its final  
voltage from an overload state. It is measured by placing the  
amplifier in a high gain configuration with an input signal that  
forces the output voltage to the supply rail. The input voltage is  
then stepped down to the linear region of the amplifier, usually  
to half-way between the supplies. The time from the input signal  
step-down to the output settling to within 100 µV of its final  
value is the overdrive recovery time. Most competitors’ auto-  
correction amplifiers require a number of autozero clock cycles  
to recover from output overdrive and some can take several  
milliseconds for the output to settle properly.  
R
60⍀  
V
X
IN  
200mV p-p  
C
4.7nF  
L
C
X
0.47F  
Figure 54. Snubber Network Configuration for Driving  
Capacitive Loads  
Although the snubber will not recover the loss of amplifier band-  
width from the load capacitance, it will allow the amplifier to drive  
larger values of capacitance while maintaining a minimum of  
overshoot and ringing. Figure 55 shows the output of an AD855x  
driving a 1 nF capacitor with and without a snubber network.  
–14–  
REV. 0  
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