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AD8130ARMZ 参数 Datasheet PDF下载

AD8130ARMZ图片预览
型号: AD8130ARMZ
PDF下载: 下载PDF文件 查看货源
内容描述: 低成本的270 MHz差分接收器放大器 [Low Cost 270 MHz Differential Receiver Amplifiers]
分类和应用: 模拟IC信号电路放大器光电二极管PC
文件页数/大小: 40 页 / 634 K
品牌: ADI [ ADI ]
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AD8129/AD8130  
APPLICATIONS  
BASIC GAIN CIRCUITS  
TWISTED-PAIR CABLE, COMPOSITE VIDEO  
RECEIVER WITH EQUALIZATION USING AN AD8130  
The gain of the AD8129/AD8130 can be set with a pair of  
feedback resistors. The basic configuration is shown in Figure 132.  
The gain equation is the same as that of a conventional op amp:  
G = 1 + RF/RG. For unity-gain applications using the AD8130,  
RF can be set to 0 (short circuit), and RG can be removed (see  
Figure 133). The AD8129 is compensated to operate at gains of  
10 and higher; therefore, shorting the feedback path to obtain  
unity gain causes oscillation.  
The AD8130 has excellent common-mode rejection at its  
inputs. This makes it an ideal candidate for a receiver for signals  
that are transmitted over long distances on twisted-pair cables.  
Category 5 cables are very common in office settings and are  
extensively used for data transmission. These cables can also be  
used for the analog transmission of signals such as video.  
These long cables pick up noise from the environment they pass  
through. This noise does not favor one conductor over another  
and therefore is a common-mode signal. A receiver that rejects  
the common-mode signal on the cable can greatly enhance the  
signal-to-noise ratio performance of the link.  
+V  
AD8129/  
AD8130  
10μF  
0.1μF  
3
7
1
8
+V  
+
+
PD  
S
V
IN  
The AD8130 is also very easy to use as a differential receiver,  
because the differential inputs and the feedback inputs are  
entirely separate. This means that there is no interaction  
between the feedback network and the termination network,  
as there would be in conventional op amp types of receivers.  
6
V
OUT  
4
5
–V  
S
2
R
F
R
G
10μF  
0.1μF  
–V  
Another issue with long cables is that there is more attenuation  
of the signal at longer distances. Attenuation is also a function  
of frequency; it increases to roughly the square root of frequency.  
Figure 132. Basic Gain Circuit: VOUT = VIN (1 + RF/RG)  
+V  
For good fidelity of video circuits, the overall frequency  
response of the transmission channel should be flat vs.  
frequency. Because the cable attenuates the high frequencies, a  
frequency-selective boost circuit can be used to undo this effect.  
These circuits are called equalizers.  
AD8130  
10μF  
0.1μF  
3
7
+V  
1
8
+
+
PD  
S
V
IN  
6
V
OUT  
4
5
–V  
An equalizer uses frequency-dependent elements (Ls and Cs) to  
create a frequency response that is the opposite of the rest of the  
channel’s response to create an overall flat response. There are  
many ways to create such circuits, but a common technique is to  
put the frequency-selective elements in the feedback path of an  
op amp circuit. The AD8130 in particular makes this easier  
than other circuits, because, once again, the feedback path is  
completely independent of the input path and there is no  
interaction.  
S
2
10μF  
0.1μF  
–V  
Figure 133. An AD8130 with Unity Gain  
The input signal can be applied either differentially or in a  
single-ended fashion—all that matters is the magnitude of the  
differential signal between the two inputs. For single-ended  
input applications, applying the signal to the +IN with −IN  
grounded creates a noninverting gain, while reversing these  
connections creates an inverting gain. Because the two inputs  
are high impedance and matched, both of these conditions  
provide the same high input impedance. Thus, an advantage of  
the active feedback architecture is the ability to make a high  
input impedance inverting op amp. If conventional op amps are  
used, a high impedance buffer followed by an inverting stage is  
needed. This requires two op amps.  
The circuit in Figure 134 was developed as a receiver/equalizer  
for transmitting composite video over 300 meters of Category 5  
cable. This cable has an attenuation of approximately 20 dB at  
10 MHz for 300 meters. At 100 MHz, the attenuation is  
approximately 60 dB (see Figure 135).  
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