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AD627ARZ-REEL 参数 Datasheet PDF下载

AD627ARZ-REEL图片预览
型号: AD627ARZ-REEL
PDF下载: 下载PDF文件 查看货源
内容描述: [INSTRUMENTATION AMPLIFIER, 200uV OFFSET-MAX, 0.08MHz BAND WIDTH, PDSO8, MS-012AA, SOIC-8]
分类和应用: 放大器光电二极管
文件页数/大小: 25 页 / 1129 K
品牌: ADI [ ADI ]
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AD627  
THEORY OF OPERATION  
The AD627 is a true instrumentation amplifier, built using two  
feedback loops. Its general properties are similar to those of the  
classic two-op-amp instrumentation amplifier configuration but  
internally the details are somewhat different. The AD627 uses a  
modified current feedback scheme, which, coupled with interstage  
feedforward frequency compensation, results in a much better  
common-mode rejection ratio (CMRRꢀ at frequencies above  
dc (notably the line frequency of 50 Hz to 60 Hzꢀ than might  
otherwise be expected of a low power instrumentation amplifier.  
The inverting terminal gain of A± (±.25ꢀ times the gain of A2  
(−4ꢀ makes the gain from the inverting and noninverting  
terminals equal.  
The differential mode gain is equal to ± + R4/R3, nominally 5,  
and is factory trimmed to 0.0±% final accuracy. Adding an  
external gain setting resistor (RGꢀ increases the gain by an  
amount equal to (R4 + R±ꢀ/RG. The output voltage of the  
AD627 is given by  
V
OUT = [VIN(+ꢀ – VIN(−ꢀ] × (5 + 200 kΩ/RGꢀ + VREF  
(±ꢀ  
In Figure 35, A± completes a feedback loop that, in conjunction  
with V± and R5, forces a constant collector current in Q±. Assume  
that the gain-setting resistor (RGꢀ is not present. Resistors R2  
and R± complete the loop and force the output of A± to be equal  
to the voltage on the inverting terminal with a gain of nearly  
±.25. A2 completes a nearly identical feedback loop that forces  
a current in Q2 that is nearly identical to that in Q±; A2 also  
provides the output voltage. When both loops are balanced, the  
gain from the noninverting terminal to VOUT is equal to 5,  
whereas the gain from the output of A± to VOUT is equal to −4.  
Laser trims are performed on R± through R4 to ensure that  
their values are as close as possible to the absolute values in the  
gain equation. This ensures low gain error and high common-  
mode rejection at all practical gains.  
EXTERNAL GAIN RESISTOR  
R1  
100k  
R
R4  
100kΩ  
G
REF  
–IN  
R2  
25kΩ  
R3  
25kΩ  
+V  
+V  
S
S
2kΩ  
2kΩ  
+IN  
Q1  
Q2  
–V  
–V  
S
S
A1  
A2  
OUTPUT  
R5  
200kΩ  
R6  
200kΩ  
V1  
0.1V  
Figure 3±. Simplified Schematic  
Rev. D | Page 14 of 24  
 
 
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