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AD603ARZ 参数 Datasheet PDF下载

AD603ARZ图片预览
型号: AD603ARZ
PDF下载: 下载PDF文件 查看货源
内容描述: 低噪声, 90 MHz可变增益放大器 [Low Noise, 90 MHz Variable Gain Amplifier]
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: 20 页 / 602 K
品牌: ADI [ ADI ]
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AD603  
THEORY OF OPERATION  
continuous attenuation from 0 dB to 42.14 dB. It will help in  
The AD603 comprises a fixed-gain amplifier, preceded by a  
broadband passive attenuator of 0 dB to 42.14 dB, having a gain  
control scaling factor of 40 dB per volt. The fixed gain is laser-  
trimmed in two ranges, to either 31.07 dB (×35.8) or 50 dB  
(×358), or may be set to any range in between using one  
external resistor between Pin 5 and Pin 7. Somewhat higher  
gain can be obtained by connecting the resistor from Pin 5 to  
common, but the increase in output offset voltage limits the  
maximum gain to about 60 dB. For any given range, the  
bandwidth is independent of the voltage-controlled gain. This  
system provides an underrange and overrange of 1.07 dB in all  
cases; for example, the overall gain is −11.07 dB to +31.07 dB in  
the maximum bandwidth mode (Pin 5 and Pin 7 strapped).  
understanding the AD603 to think in terms of a mechanical  
means for moving this slider from left to right; in fact, its  
position is controlled by the voltage between Pin 1 and Pin 2.  
The details of the gain control interface are discussed later.  
The gain is at all times very exactly determined, and a linear-in-  
dB relationship is automatically guaranteed by the exponential  
nature of the attenuation in the ladder network (the X-AMP  
principle). In practice, the gain deviates slightly from the ideal  
law, by about 0.2 dB peak (see, for example, Figure 5).  
NOISE PERFORMANCE  
An important advantage of the X-AMP is its superior noise  
performance. The nominal resistance seen at inner tap points is  
41.7 Ω (one third of 125 Ω), which exhibits a Johnson noise  
spectral density (NSD) of 0.83 nV/√Hz (that is, √4kTR) at 27°C,  
which is a large fraction of the total input noise. The first stage  
of the amplifier contributes a further 1 nV/√Hz, for a total input  
noise of 1.3 nV/√Hz. It will be apparent that it is essential to use  
a low resistance in the ladder network to achieve the very low  
specified noise level. The signal’s source impedance forms a  
voltage divider with the AD603s 100 Ω input resistance. In  
some applications, the resulting attenuation may be  
This X-AMP structure has many advantages over former  
methods of gain control based on nonlinear elements. Most  
importantly, the fixed-gain amplifier can use negative feedback  
to increase its accuracy. Since large inputs are first attenuated,  
the amplifier input is always small. For example, to deliver a  
1 V output in the −1 dB/+41 dB mode (that is, using a fixed  
amplifier gain of 41.07 dB) its input is only 8.84 mV; thus the  
distortion can be very low. Equally important, the small-signal  
gain and phase response, and thus the pulse response, are  
essentially independent of gain.  
unacceptable, requiring the use of an external buffer or  
preamplifier to match a high impedance source to the low  
impedance AD603.  
Figure 29 is a simplified schematic. The input attenuator is a  
seven-section R-2R ladder network, using untrimmed resistors  
of nominally R = 62.5 Ω, which results in a characteristic  
resistance of 125 Ω 20ꢀ. A shunt resistor is included at the  
input and laser trimmed to establish a more exact input  
resistance of 100 Ω 3ꢀ, which ensures accurate operation  
(gain and HP corner frequency) when used in conjunction with  
external resistors or capacitors.  
The noise at maximum gain (that is, at the 0 dB tap) depends on  
whether the input is short-circuited or open-circuited: when  
shorted, the minimum NSD of slightly over 1 nV/√Hz is  
achieved; when open, the resistance of 100 Ω looking into the  
first tap generates 1.29 nV/√Hz, so the noise increases to a total  
of 1.63 nV/√Hz. (This last calculation would be important if the  
AD603 were preceded by, for example, a 900 Ω resistor to allow  
operation from inputs up to 10 V rms.) As the selected tap  
moves away from the input, the dependence of the noise on  
source impedance quickly diminishes.  
The nominal maximum signal at input VINP is 1 V rms ( 1.4 V  
peak) when using the recommended 5 V supplies, although  
operation to 2 V peak is permissible with some increase in HF  
distortion and feedthrough. Pin 4 (COMM) must be connected  
directly to the input ground; significant impedance in this  
connection will reduce the gain accuracy.  
Apart from the small variations just discussed, the signal-to-  
noise (S/N) ratio at the output is essentially independent of the  
attenuator setting. For example, on the −11 dB/+31 dB range,  
the fixed gain of ×35.8 raises the output NSD to 46.5 nV/√Hz.  
Thus, for the maximum undistorted output of 1 V rms and a  
1 MHz bandwidth, the output S/N ratio would be 86.6 dB, that  
is, 20 log (1 V/46.5 µV).  
The signal applied at the input of the ladder network is  
attenuated by 6.02 dB by each section; thus, the attenuation to  
each of the taps is progressively 0 dB, 6.02 dB, 12.04 dB,  
18.06 dB, 24.08 dB, 30.1 dB, 36.12 dB, and 42.14 dB. A unique  
circuit technique is employed to interpolate between these tap  
points, indicated by the slider in Figure 29, thus providing  
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