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AD623BN 参数 Datasheet PDF下载

AD623BN图片预览
型号: AD623BN
PDF下载: 下载PDF文件 查看货源
内容描述: 单电源,轨到轨,低成本仪表放大器 [Single Supply, Rail-to-Rail, Low Cost Instrumentation Amplifier]
分类和应用: 仪表放大器
文件页数/大小: 16 页 / 960 K
品牌: ADI [ ADI ]
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AD623  
Amplifying Signals with Low Common-Mode Voltage  
Because the common-mode input range of the AD623 extends  
0.1 V below ground, it is possible to measure small differential  
signals which have low, or no, common mode component. Fig-  
ure 50 shows a thermocouple application where one side of the  
J-type thermocouple is grounded.  
The voltages on these internal nodes are critical in determining  
whether or not the output voltage will be clipped. The voltages  
A1 and VA2 can swing from about 10 mV above the negative  
supply (V– or Ground) to within about 100 mV of the positive  
rail before clipping occurs. Based on this and from the above  
equations, the maximum and minimum input common-mode  
voltages are given by the equations  
V
+5V  
VCMMAX = V+ – 0.7 V – VDIFF × Gain/2  
0.1F  
VCMMIN = V– – 0.590 V + VDIFF × Gain/2  
These equations can be rearranged to give the maximum possible  
differential voltage (positive or negative) for a particular common-  
mode voltage, gain, and power supply. Because the signals on A1  
and A2, can clip on either rail, the maximum differential voltage  
will be the lesser of the two equations.  
R
J-TYPE  
THERMOCOUPLE  
G
AD623  
V
OUT  
1.02k⍀  
REF  
2V  
|VDIFFMAX| = 2 (V+ – 0.7 V – VCM)/Gain  
|VDIFFMAX| = 2 (VCM – V– +0.590 V)/Gain  
Figure 50. Amplifying Bipolar Signals with Low Common-  
Mode Voltage  
However, the range on the differential input voltage range is also  
constrained by the output swing. So the range of VDIFF may have  
to be lower according the equation.  
Over a temperature range from –200°C to +200°C, the J-type  
thermocouple delivers a voltage ranging from –7.890 mV to  
10.777 mV. A programmed gain on the AD623 of 100 (RG =  
1.02 k) and a voltage on the AD623 REF pin of 2 V, results in  
the AD623’s output voltage ranging from 1.110 V to 3.077 V  
relative to ground.  
Input Range Available Output Swing/Gain  
For a bipolar input voltage with a common-mode voltage that is  
roughly half way between the rails, VDIFFMAX will be half the  
value that the above equations yield because the REF pin will be  
at midsupply. Note that the available output swing is given for  
different supply conditions in the Specifications section.  
INPUT DIFFERENTIAL AND COMMON-MODE RANGE  
VS. SUPPLY AND GAIN  
Figure 51 shows a simplified block diagram of the AD623. The  
voltages at the outputs of the amplifiers A1 and A2 are given by  
the equations  
The equations can be rearranged to give the maximum gain for a  
fixed set of input conditions. Again, the maximum gain will be  
the lesser of the two equations.  
VA2 = VCM + VDIFF/2 + 0.6 V + VDIFF × RF/RG  
= VCM + 0.6 V + VDIFF × Gain/2  
GainMAX = 2 (V+ – 0.7 V – VCM)/VDIFF  
GainMAX = 2 (VCM – V– +0.590 V)/VDIFF  
VA1 = VCM VDIFF/2 + 0.6 V VDIFF × RF/RG  
= VCM + 0.6 V VDIFF × Gain/2  
Again, we must ensure that the resulting gain times the input  
range is less than the available output swing. If this is not the  
case, the maximum gain is given by,  
POS SUPPLY  
7
GainMAX = Available Output Swing/Input Range  
Also for bipolar inputs (i.e., input range = 2 VDIFF), the maxi-  
mum gain will be half the value yielded by the above equations  
because the REF pin must be at midsupply.  
INVERTING  
A1  
2
R
F
50k⍀  
4
50k⍀  
The maximum gain and resulting output swing for different  
input conditions is given in Table IV. Output voltages are refer-  
enced to the voltage on the REF pin.  
50k⍀  
50k⍀  
V
1
DIFF  
2
V
OUT  
6
R
A3  
50k⍀  
GAIN  
G
V
CM  
R
F
For the purposes of computation, it is necessary to break down  
the input voltage into its differential and common-mode compo-  
nent. So when one of the inputs is grounded or at a fixed voltage,  
the common-mode voltage changes as the differential voltage  
changes. Take the case of the thermocouple amplifier in Figure  
50. The inverting input on the AD623 is grounded. So when the  
input voltage is –10 mV, the voltage on the noninverting input is  
–10 mV. For the purposes of signal swing calculations, this input  
voltage should be considered to be composed of a common-mode  
voltage of –5 mV (i.e., (+IN + –IN)/2) and a differential input  
voltage of –10 mV (i.e., +IN – –IN).  
REF  
5
50k⍀  
8
7
V
DIFF  
2
A2  
3
NONINVERTING  
4
NEG SUPPLY  
Figure 51. Simplified Block Diagram  
REV. C  
–15–  
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