欢迎访问ic37.com |
会员登录 免费注册
发布采购

AD625JN 参数 Datasheet PDF下载

AD625JN图片预览
型号: AD625JN
PDF下载: 下载PDF文件 查看货源
内容描述: 可编程增益仪表放大器器 [Programmable Gain Instrumentation Amplifier]
分类和应用: 仪表放大器放大器电路光电二极管
文件页数/大小: 15 页 / 464 K
品牌: AD [ ANALOG DEVICES ]
 浏览型号AD625JN的Datasheet PDF文件第5页浏览型号AD625JN的Datasheet PDF文件第6页浏览型号AD625JN的Datasheet PDF文件第7页浏览型号AD625JN的Datasheet PDF文件第8页浏览型号AD625JN的Datasheet PDF文件第10页浏览型号AD625JN的Datasheet PDF文件第11页浏览型号AD625JN的Datasheet PDF文件第12页浏览型号AD625JN的Datasheet PDF文件第13页  
AD625
VOLTAGE NOISE – nV Hz
300
MULTIPLYING FACTOR
Any resistors in series with the inputs of the AD625 will degrade
the noise performance. For this reason the circuit in Figure 26b
should be used if the gains are all greater than 5. For gains less
than 5, either the circuit in Figure 26a or in Figure 26c can be
used. The two 1.4 kΩ resistors in Figure 26a will degrade the
noise performance to:
RTO NOISE
RTO OFFSET VOLTAGE
3
200
2
100
4
kTR
ext
+(4
nV/ Hz
)
2
=
7.9
nV
/
Hz
RESISTOR PROGRAMMABLE GAIN AMPLIFIER
10k 20k 30k 40k 50k 60k
FEEDBACK RESISTANCE –
RTO OFFSET VOLTAGE DRIFT
6
10k 20k 30k 40k 50k 60k
FEEDBACK RESISTANCE –
BANDWIDTH
10k
In the resistor-programmed mode (Figure 27), only three exter-
nal resistors are needed to select any gain from 1 to 10,000.
Depending on the application, discrete components or a
pretrimmed network can be used. The gain accuracy and gain
TC are primarily determined by the external resistors since the
AD625C contributes less than 0.02% to gain error and under
5 ppm/°C gain TC. The gain sense current is insensitive to
common-mode voltage, making the CMRR of the resistor pro-
grammed AD625 independent of the match of the two feedback
resistors, R
F
.
Selecting Resistor Values
1M
MULTIPLYING FACTOR
FREQUENCY – Hz
5
4
3
2
1
10k 20k 30k 40k 50k 60k
FEEDBACK RESISTANCE –
100k
20k
50k
10k
1
10
100
1k
FEEDBACK RESISTANCE –
As previously stated each R
F
provides feedback to the input
stage and sets the unity gain transconductance. These feedback
resistors are provided by the user. The AD625 is tested and
specified with a value of 20 kΩ for R
F
. Since the magnitude of
RTO errors increases with increasing feedback resistance, values
much above 20 kΩ are not recommended (values below 10 kΩ
for R
F
may lead to instability). Refer to the graph of RTO noise,
offset, drift, and bandwidth (Figure 28) when selecting the
feedback resistors. The gain resistor (R
G
) is determined by the
formula R
G
= 2 R
F
/(G – l).
G=
R
F
2R
F
+1
R
G
R
G
–INPUT
R
F
Figure 28. RTO Noise, Offset, Drift and Bandwidth vs.
Feedback Resistance Normalized to 20 k
Table I. Common Gains Nominally Within
Using Standard 1% Resistors
0.5% Error
GAIN
1
2
5
10
20
50
100
200
500
1000
4
8
16
32
64
128
256
512
1024
SENSE TERMINAL
R
F
20 kΩ
19.6 kΩ
20 kΩ
20 kΩ
20 kΩ
19.6 kΩ
20 kΩ
20.5 kΩ
19.6 kΩ
19.6 kΩ
20 kΩ
19.6 kΩ
20 kΩ
19.6 kΩ
20 kΩ
20 kΩ
19.6 kΩ
19.6 kΩ
19.6 kΩ
R
G
39.2 kΩ
10 kΩ
4.42 kΩ
2.1 kΩ
806
402
205
78.7
39.2
13.3 kΩ
5.62 kΩ
2.67 kΩ
1.27 kΩ
634
316
154
76.8
38.3
+INPUT
1
+GAIN
SENSE
RTI NULL
+V
S
RTI NULL
+GAIN DRIVE
4
5
A1
A2
2
3
16
15
–GAIN
SENSE
RTO
14 NULL
13
12
11
10k
10k
10k
10
9 +V
S
V
OUT
RTO
NULL
–GAIN DRIVE
NC 6
REF
7
10k
A3
–V
S
8
AD625
Figure 27. AD625 in Fixed Gain Configuration
A list of standard resistors which can be used to set some com-
mon gains is shown in Table I.
For single gain applications, only one offset null adjust is neces-
sary; in these cases the RTI null should be used.
The sense terminal is the feedback point for the AD625 output
amplifier. Normally it is connected directly to the output. If
heavy load currents are to be drawn through long leads, voltage
drops through lead resistance can cause errors. In these in-
stances the sense terminal can be wired to the load thus putting
REV. D
–9–