参数资料
型号: AC1059
厂商: Analog Devices Inc
文件页数: 5/8页
文件大小: 0K
描述: SOCKET FOR MODEL AD210 IC
标准包装: 1
附件类型: 插拔式插孔
适用于相关产品: AD210
AD210
REV. A
–5–
+0.04
+0.03
+0.02
+0.01
0
–0.01
–0.02
–0.03
–0.04
–10
–8
–6
–4
–2
0
+2
+4
+6
+8
+10
OUTPUT VOLTAGE SWING – Volts
+8
+6
+4
+2
0
–2
–4
–6
–8
ERROR
mV
ERROR
%
Figure 12. Gain Nonlinearity Error vs. Output
0.01
0.009
0.008
0.007
0.006
0.005
0.004
0.003
0.002
0.001
0.000
100
90
80
70
60
50
40
30
20
10
0
2
4
6
8
10
12
14
16
18
20
TOTAL SIGNAL SWING – Volts
ERROR
%
of
Signal
Swing
ERROR
ppm
of
Signal
Swing
Figure 13. Gain Nonlinearity vs. Output Swing
Gain vs. Temperature:
Figure 14 illustrates the AD210’s
gain vs. temperature performance. The gain versus temperature
performance illustrated is for an AD210 configured as a unity
gain amplifier.
400
200
0
–200
–400
–600
–800
–1000
–1200
–1400
–1600
–25
0
+25
+50
+70
+85
TEMPERATURE –
°C
GAIN
ERROR
ppm
of
Span
G = 1
Figure 14. Gain vs. Temperature
Phase Shift:
Figure 10 illustrates the AD210’s low phase shift
and gain versus frequency. The AD210’s phase shift and wide
bandwidth performance make it well suited for applications like
power monitors and controls systems.
60
20
–80
100
100k
10k
1k
10
40
–20
0
–60
–40
FREQUENCY – Hz
0
–20
–40
–60
–80
–100
–120
–140
PHASE
SHIFT
Degrees
GAIN
dB
φG = 1
φG = 100
Figure 10. Phase Shift and Gain vs. Frequency
Input Noise vs. Frequency:
Voltage noise referred to the input
is dependent on gain and signal bandwidth. Figure 11 illustrates
the typical input noise in nV/
√Hz of the AD210 for a frequency
range from 10 to 10 kHz.
60
40
0
100
10k
1k
10
50
20
30
10
FREQUENCY – Hz
NOISE
nV/
Hz
Figure 11. Input Noise vs. Frequency
Gain Nonlinearity vs. Output:
Gain nonlinearity is defined as the
deviation of the output voltage from the best straight line, and is
specified as % peak-to-peak of output span. The AD210B provides
guaranteed maximum nonlinearity of
±0.012% with an output span of
±10 V. The AD210’s nonlinearity performance is shown in Figure 12.
Gain Nonlinearity vs. Output Swing:
The gain nonlinearity
of the AD210 varies as a function of total signal swing. When
the output swing is less than 20 volts, the gain nonlinearity as a
fraction of signal swing improves. The shape of the nonlinearity
remains constant. Figure 13 shows the gain nonlinearity of the
AD210 as a function of total signal swing.
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