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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  
COMPONENT  
LEAD  
be a specific width, but it should form a continuous loop around  
both inputs. By setting the guard ring voltage equal to the volt-  
age at the noninverting input, parasitic capacitance is minimized  
as well. For further reduction of leakage currents, components  
can be mounted to the PC board using Teflon standoff insulators.  
V
V
SC2  
SC1  
+
SOLDER  
SURFACE MOUNT  
COMPONENT  
+
؊
؊
V
V
TS2  
TS1  
+
+
؊
؊
PC BOARD  
T
T
A2  
A1  
COPPER  
TRACE  
IF T  
V
T
, THEN  
A1  
A2  
V
V
OUT  
+ V  
V
+ V  
OUT  
TS1  
SC1  
TS2 SC2  
V
V
IN  
IN  
AD8552  
AD8552  
Figure 48. Mismatch in Seebeck Voltages Causes a  
Thermoelectric Voltage Error  
R
F
V
IN  
V
OUT  
R
1
AD8552  
V
OUT  
V
IN  
AD855x  
R
= R  
1
S
Figure 46. Guard Ring Layout and Connections to Reduce  
PC Board Leakage Currents  
A
= 1 + (R /R )  
F
1
V
NOTE: R SHOULD BE PLACED IN CLOSE PROXIMITY AND  
S
ALIGNMENT TO R TO BALANCE SEEBECK VOLTAGES  
1
V+  
R
R
2
Figure 49. Using Dummy Components to Cancel  
Thermoelectric Voltage Errors  
1
AD8552  
R
R
1
2
V
IN1  
V
IN2  
1/f Noise Characteristics  
Another advantage of autozero amplifiers is their ability to cancel  
flicker noise. Flicker noise, also known as 1/f noise, is noise inher-  
ent in the physics of semiconductor devices and increases 3 dB  
for every octave decrease in frequency. The 1/f corner frequency  
of an amplifier is the frequency at which the flicker noise is equal  
to the broadband noise of the amplifier. At lower frequencies,  
flicker noise dominates, causing higher degrees of error for sub-  
Hertz frequencies or dc precision applications.  
GUARD  
RING  
GUARD  
RING  
V
REF  
V
REF  
V؊  
Figure 47. Top View of AD8552 SOIC Layout with  
Guard Rings  
Other potential sources of offset error are thermoelectric voltages  
on the circuit board. This voltage, also called Seebeck voltage,  
occurs at the junction of two dissimilar metals and is proportional  
to the temperature of the junction. The most common metallic  
junctions on a circuit board are solder-to-board trace and solder-  
to-component lead. Figure 48 shows a cross-section diagram view  
of the thermal voltage error sources. If the temperature of the PC  
board at one end of the component (TA1) is different from the  
temperature at the other end (TA2), the Seebeck voltages will not  
be equal, resulting in a thermal voltage error.  
Because the AD855x amplifiers are self-correcting op amps,  
they do not have increasing flicker noise at lower frequencies.  
In essence, low frequency noise is treated as a slowly varying  
offset error and is greatly reduced as a result of autocorrection.  
The correction becomes more effective as the noise frequency  
approaches dc, offsetting the tendency of the noise to increase  
exponentially as frequency decreases. This allows the AD855x  
to have lower noise near dc than standard low-noise amplifiers  
that are susceptible to 1/f noise.  
This thermocouple error can be reduced by using dummy com-  
ponents to match the thermoelectric error source. Placing the  
dummy component as close as possible to its partner will ensure  
both Seebeck voltages are equal, thus canceling the thermo-  
couple error. Maintaining a constant ambient temperature on  
the circuit board will further reduce this error. The use of a  
ground plane will help distribute heat throughout the board and  
will also reduce EMI noise pickup.  
Intermodulation Distortion  
The AD855x can be used as a conventional op amp for gain/  
bandwidth combinations up to 1.5 MHz. The autozero correc-  
tion frequency of the device is fixed at 4 kHz. Although a trace  
amount of this frequency will feed through to the output, the  
amplifier can be used at much higher frequencies. Figure 50  
shows the spectral output of the AD8552 with the amplifier  
configured for unity gain and the input grounded.  
The 4 kHz autozero clock frequency appears at the output with  
less than 2 µV of amplitude. Harmonics are also present, but at  
reduced levels from the fundamental autozero clock frequency.  
The amplitude of the clock frequency feedthrough is proportional  
to the closed-loop gain of the amplifier. Like other autocorrection  
amplifiers, at higher gains there will be more clock frequency  
feedthrough. Figure 51 shows the spectral output with the ampli-  
fier configured for a gain of 60 dB.  
–12–  
REV. 0