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Group delay The measurement, in nanoseconds, of the time retardation created by a filter or circuit to any discrete signal that passes through it When the group delay varies across the passband significantly, as it does in tight Chebyshev filters (and to a certain extent in Butterworth filters), this will cause increased BER in digital radios This variation in the group delay, called group delay variations (GDV), is especially severe at the edges of a filter s passband, so any filter that has steep skirts and/or a high pole count will have a high GDV The problem can be lessened by widening the filter s passband beyond what is required by the signal; using fewer filter poles; or choosing a Butterworth type or, if selectivity specifications permit it, a Bessel filter response GDV is directly equated to the differential delay specification above Insertion loss The attenuation created in a filter within the center of its passband when the filter is terminated at its design impedance Measured in dB Insertion loss linearity The measure, in dB, in the variations in insertion loss with input power Primarily a problem with crystal filters Passband The band of frequencies from fLOW to fHIGH that a filter passes with 3 dB or less attenuation (fLOW and fHIGH are located at points where the insertion losses reach, typically, 3 dB) Measured in Hz Passband ripple The amplitude fluctuations within a filter s passband A ripple greater than 05 dB is usually considered unacceptable in digitally modulated radios Chebyshev is the dominant filter topology that contains ripple within its passband However, this ripple can be decreased to 01 dB or less by low-ripple Cheby designs Phase shift The measurement of the variation of the phase of a signal as it moves through a filter from its input to its output Poles Refers to the number of reactive components, inductors or capacitors, in a low-pass or high-pass filter; or the number of reactive pairs in a bandpass filter (for an all-pole filter) The filter s order matches its poles in an all-pole filter, and the number of poles governs the steepness of the filter s skirts Q (quality factor) The ratio of the center frequency to its bandwidth at its 3-dB-down points The narrower the bandwidth for the same center frequency, the higher the filter Q Q also refers to the quality factor of the individual components that make up the filter This is particularly important for inductors within the LC filter circuit, since the lower the individual Q s within each component, the higher the filter s insertion loss will be The stopbands will also have a poorer stopband attenuation characteristic, and the filter s response at the band edges will be more rounded than with high-Q components Return loss The measurement, expressed in decibels, of the difference between the signal power sent toward a filter s input and the strength of the RF signal power returned, or reflected, from the input back toward the.

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Downloaded from Digital Engineering Library @ McGraw-Hill (wwwdigitalengineeringlibrarycom) Copyright 2004 The McGraw-Hill Companies All rights reserved Any use is subject to the Terms of Use as given at the website

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Now that we ve explained the Atom model s idiosyncrasies, let s take a look at an example. Listing 7.3 shows how to parse an Atom newsfeed to the Atom WireFeed model.

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source Most filters can easily be designed with a return loss of 10 dB or higher With this value of return loss, only one-tenth the power incident to the filter s input will not be passed on to the load, but will be reflected back toward the original source Ripple The amount of amplitude variations in the passband of a filter Excessive ripple causes high BER in digital systems Measured in dB Ripple loss The distinction between the maximum and the minimum attenuation inside the filter s passband Shape factor Specifies the steepness of the skirts in a filter, and is measured as: BW (at 60 dB) BW (at 3 dB) A perfectly square shape factor would equal 1 Measured as a ratio Spurious responses Since the perfect component does not exist, any filter made of capacitors, inductors, and/or crystals can have areas within its stopband that supply less attenuation than planned, or create ripple within the filter s passband This is caused by undesired reactances from the component s own leads, as well as stray inductances and capacitances, resonating at various frequencies Crystal filters, especially those with the AT-cut, will have these responses at roughly odd integer multiples of the fundamental frequency, which can create unexpected consequences in the design of the communication system if not expected Distributed microwave filters can also have reentrance modes, which can allow a multitude of secondary passbands within the filter s expected stopband These effects can, if required, be ameliorated by supplemental LC filtering at the output of the crystal filter and in some of the lower-frequency distributed filters Stopband (reject band) The band of frequencies that bandpass, low-pass, high-pass, and bandstop filters attenuate to some predetermined level, usually 60 dB (but it can be much less) The stopband is the point on the attenuated side of the cutoff frequency Measured in Hz 61 Lumped Filters.

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