A symmetrical lattice is a two-port electrical wave filter in which diagonally-crossed shunt elements are present – a configuration which sets it apart from ladder networks. The component arrangement of the lattice is shown in the diagram below. The filter properties of this circuit were first developed using image impedance concepts, but later the more general techniques of network analysis were applied to it. There is a duplication of components in the lattice network as the "series impedances" (instances of Za) and "shunt impedances" (instances of Zb) both occur twice, an arrangement that offers increased flexibility to the circuit designer with a variety of responses achievable. It is possible for the lattice network to have the characteristics of: a delay network, an amplitude or phase correcting network, a dispersive network or as a linear phase filter, according to the choice of components for the lattice elements.
Configuration The basic configuration of the symmetrical lattice is shown in the left-hand diagram. A commonly used short-hand version is shown on the right, with dotted lines indicating the presence the second pair of matching impedances.
It is possible with this circuit to have the characteristic impedance specified independently of its transmission properties, a feature not available to ladder filter structures. In addition, it is possible to design the circuit to be a constant-resistance network for a range of circuit characteristics. The lattice structure can be converted to an unbalanced form (see below), for insertion in circuits with a ground plane. Such conversions also reduce the component count and relax component tolerances. It is possible to redraw the lattice in the Wheatstone bridge configuration (as shown in the article Zobel network). However, this is not a convenient format in which to investigate the properties of lattice filters, especially their behavior in cascade.
Basic properties
Results from image theory Filter theory was initially developed from earlier studies of transmission lines. In this theory, a filter section is specified in terms of its propagation constant and image impedance (or characteristic impedance). Specifically for the lattice, the propagation function, γ, and characteristic impedance, Zo, are defined by,
γ = ln ( Z a Z b + 1 Z a Z b − 1 ) = 2 artanh Z a Z b {\displaystyle \gamma =\ln \left(\ {\frac {\ {\sqrt {{\frac {\ Z_{\mathsf {a}}\ }{Z_{\mathsf {b}}}}+1\ }}\ }{\ {\sqrt {\ {\frac {\ Z_{\mathsf {a}}\ }{Z_{\mathsf {b}}}}-1\ }}\ }}\ \right)=2\ \operatorname {artanh} {\sqrt {{\frac {\ Z_{\mathsf {a}}\ }{Z_{\mathsf {b}}}}\ }}\qquad \;} and Z o = Z a ⋅ Z b {\displaystyle \;\qquad Z_{\mathsf {o}}={\sqrt {\ Z_{\mathsf {a}}\cdot Z_{\mathsf {b}}\ }}}
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