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The noise gure of a (ideal) passive attenuator at a temperature of T0 (290 K) equals its attenuation. This is because the available noise at the output of the attenuator is the available noise from the Thevenin resistance of the attenuator, presumably the same as the standard impedance of the cables at that point in the cascade. This is the same as the available noise from the source, at the input to the attenuator, during characterization. Thus the noises in Eq. (3.1) cancel and f becomes the ratio of input signal power to output signal power, which equals the attenuation. If we did a circuit-noise analysis of an attenuator, say a or T network, we would get the same results (but less ef ciently). We can do it either way (but must not add the two effects). The combined noise gure of a module preceded by an attenuator at T0 equals the module noise gure plus the attenuation. (The gain of the combination is, of course, lowered by the attenuation also.) To see this, write Eq. (3.14) for an attenuator followed by a module, using 1/g1 for the attenuation of the attenuator: f = f2 1 f2 1 + = . g1 g1 g1 (3.24) c# upc-a reader C# UPC-A Barcode Scanner Library - Read & Scan UPC-A Using ...
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