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AD830JR 参数 Datasheet PDF下载

AD830JR图片预览
型号: AD830JR
PDF下载: 下载PDF文件 查看货源
内容描述: 高速视频差动放大器 [High Speed, Video Difference Amplifier]
分类和应用: 放大器
文件页数/大小: 16 页 / 336 K
品牌: ADI [ ADI ]
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AD830  
UND ERSTAND ING TH E AD 830 TO P O LO GY  
V
V
X1  
T he AD830 represents Analog Devices’ first amplifier product  
to embody a powerful alternative amplifier topology. Referred to  
as active feedback, the topology used in the AD830 provides in-  
herent advantages in the handling of differential signals, differ-  
ing system commons, level shifting and low distortion, high  
frequency amplification. In addition, it makes possible the  
implementation of many functions not realizable with single op  
amp circuits or is superior to op amp based equivalent circuits.  
With this in mind, it is important to understand the internal  
structure of the AD830.  
G
M
X2  
I
I
X
A=1  
V
OUT  
Y
C
C
V
V
Y1  
G
M
Y2  
T he topology, reduced to its elemental form, is shown below in  
Figure 21. Nonideal effects such as nonlinearity, bias currents  
and limited full scale are omitted from this model for simplicity,  
but are discussed later. T he key feature of this topology is the  
use of two, identical voltage-to-current converters, GM, that  
make up input and feedback signal interfaces. T hey are labeled  
with inputs VX and VY, respectively. T hese voltage to current  
converters possess fully differential inputs, high linearity, high  
input impedance and wide voltage range operation. T his enables  
the part to handle large amplitude differential signals; they also  
provide high common-mode rejection, low distortion and negli-  
gible loading on the source. T he label, GM, is meant to convey  
that the transconductance is a large signal quantity, unlike in the  
front-end of most op amps. T he two GM stage current outputs  
IX and IY, sum together at a high impedance node which is char-  
acterized by an equivalent resistance and capacitance connected  
to an “ac common.” A unity voltage gain stage follows the high  
impedance node to provide buffering from loads. Relative to  
either input, the open loop gain, AOL, is set by the  
V
– V = V – V  
X2 Y Y1  
2
X1  
FOR V = V  
Y2  
OUT  
1
1 + S(C /G  
V
= (V – V + V  
)
Y1  
OUT  
X1  
X2  
)
M
C
Figure 22. Closed-Loop Connection  
Precise amplification is accomplished through closed-loop op-  
eration of this topology. Voltage feedback is implemented via  
the Y GM stage in which where the output is connected to the  
–Y input for negative feedback as shown in Figure 22. An input  
signal is applied across the X GM stage, either fully differentially  
or single-ended referred to common. It produces a current sig-  
nal which is summed at the high impedance node with the out-  
put current from the Y GM stage. Negative feedback nulls this  
sum to a small error current necessary to develop the output  
voltage at the high impedance node. T he error current is usually  
negligible, so the null condition essentially forces the Y GM  
output stage current to exactly equal the X GM output current.  
Since the two transconductances are identical, the differential  
voltage across the Y inputs equals the negative of the differential  
voltage across the X input; VY = –VX or more precisely  
transconductance, GM, working into the resistance, RP; AOL  
=
GM ϫ RP. T he unity gain frequency ω0 dB for the open loop gain  
is established by the transconductance, GM, working into the  
capacitance, CC; ω0 dB = GM/CC. T he open loop description of  
the AD830 is shown below for completeness.  
V
Y2–VY1 = VX1–VX2. T his simple relation provides the basis to  
easily analyze any function possible to synthesize with the  
AD830, including any feedback situation.  
T he bandwidth of the circuit is defined by the GM and the  
capacitor CC. T he highly linear GM stages give the amplifier a  
single pole response, excluding the output amplifier and loading  
effects. It is important to note that the bandwidth and general dy-  
namic behavior is symmetrical (identical) for the noninverting and  
the inverting connections of the AD830. In addition, the input im-  
pedance and CMRR are the same for either connections. T his is  
very advantageous and unlike in a voltage or current feedback  
amplifier, where there is a distinct difference in performance be-  
tween the inverting and noninverting gain. T he practical impor-  
tance of this cannot be overemphasized and is a key feature  
offered by the AD830 amplifier topology.  
V
X1  
X2  
G
M
V
I
I
X
Y
I
Z
A=1  
V
OUT  
I
I
I
= (V – V ) G  
X1 X2 M  
X
Y
Z
V
V
Y1  
= (V – V ) G  
Y1  
Y2  
M
C
R
G
C
P
M
= I + I  
X
Y
Y2  
G
R
M
P
A
=
OLS  
1 + S (C R )  
C
P
Figure 21. Topology Diagram  
REV. A  
–9–  
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