Page 273 - Complete Wireless Design
P. 273

Filter Design



            272  Chapter Six






                                                   Figure 6.1 A basic LC low-pass
                                                   filter.








                                                   Figure 6.2 A basic LC high-pass
                                                   filter.









                        Figure 6.3 An 8-pole low-pass filter.


                        throughout its entire operational passband. Two such filters are the T type
                        (Fig. 6.4) and pi type (Fig. 6.5) low-pass filters. The m derived is another filter
                        that displays a superior cutoff response, while maintaining a constant imped-
                        ance across most of its passband.
                          A bandpass filter will permit only a certain range of frequencies to pass
                        unattenuated between two points, while a bandstop, notch, or band-reject fil-
                        ter will severely attenuate a chosen set of frequencies between two points.
                        Unlike the above low-pass and bandpass filters, these are almost always of the
                        resonant, or tuned, form. However, by combining both a nonresonant low-pass
                        with a nonresonant high-pass filter, a bandpass attribute can be achieved.
                          Tuned filters work on the principle of resonance. Since an inductor’s reactance
                        will increase with frequency, while a capacitor’s reactance will decrease—and
                        considering that these are opposing qualities—a specific frequency in which X
                                                                                               L
                          X will soon be reached. At this point their opposite reactances will cancel.
                            C
                        This will cause, when a capacitor and inductor are in series, the RF current
                        through the circuit to be maximum and the impedance to be at a minimum.
                        Thus, the current will be able to reach very high levels, with the only impedi-
                        ment to this current being the small AC and DC resistance of the coil. In fact,
                        this resistance becomes very important in filter design, since the unloaded (com-
                        ponent) Q of a coil—being X /r , or the coil’s reactance divided by its resistance—
                                                 L e
                        severely impacts the filter’s insertion loss, the shape of its passband, and the
                        return loss. This unloaded Q is influenced by the skin effect, the wire type, wire
                        size, and losses within the coil forms. A very simple example of a basic series
                        bandpass is shown in Fig. 6.6, while a bandstop is seen in Fig. 6.7.



                   Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com)
                               Copyright © 2004 The McGraw-Hill Companies. All rights reserved.
                                Any use is subject to the Terms of Use as given at the website.
   268   269   270   271   272   273   274   275   276   277   278