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March 2010 Issue: Technical Feature

Ultra-fast, Simpler and More Accurate Noise Parameter Measurements

Noise parameters are required to design circuits to minimize the effect of noise, but noise parameters have traditionally been very slow and complex to measure. Now a new, ultra-fast method is shown, which is over two orders of magnitude faster, more accurate and simpler, requiring less operator skill to make the measurement.

Electrical noise is created naturally by almost any type of device. In circuits that need to amplify and process very low level signals, noise can interfere with the desired signal, causing degraded or complete loss of reception. This is significant for any wireless receiver, often being the limiting factor on reception quality and range. Much of the interfering noise can be generated by the components in the receiver circuit itself.


There are two approaches that can reduce the effect of noise. The first is to increase the transmitted signal level so that the receiver noise becomes insignificant. However, this is usually not practical because of cost, power, size, weight, safety, or regulatory limitations. The other approach is to reduce the noise generated by the receiver circuitry. This is generally the only cost-effective and practical option available.

Figure 1 Noise figure is defined in terms of input and output signal-to-noise ratios.

Noise figure is a measure of noise generated by a circuit. It is defined as the input signal-to-noise ratio divided by the output signal-to-noise ratio. It can be expressed as a ratio, sometimes called noise factor, or in dB, as shown in Equation 1 and illustrated in Figure 1. For an ideal, noise-free device, the input and output signal-to-noise ratios would be equal, giving a noise figure ratio of one. In any real device, some noise is added, so the noise figure ratio is always greater than one. One of the objectives for circuit designers is to make the noise figure as low as possible to minimize the adverse effects of noise in the system.

At microwave frequencies, the primary type of noise is thermal noise, which is generated by any resistance in the circuit, or by the active devices used to amplify signals. Resistance is due to discrete resistors or the resistivity of lossy components. The available noise power produced by a resistance is given by Equation 2:

where
Pn = available noise power
k = Boltzmann’s constant
T = temperature in Kelvin
B = bandwidth of the system


     

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This month's Cover Story:

The MIMO Antenna: Unseen, Unloved, Untested! -- August 5, 2010



Global Maritime Satellite Communications Market Passes $1 B -- September 2, 2010

Cree Demonstrates 150-mm Silicon Carbide Substrates -- September 2, 2010

The Defence/Security Executive Forum at EuMW 2010 -- September 2, 2010

WIN and Presto Engineering Announce Strategic Collaboration -- September 2, 2010

Agilent Launches Measurement Applications, Expands LTE Leadership -- September 2, 2010

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