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Overhead conductor admittance

In this chapter, a theory of distributed-parameter circuits is explained starting from the approximate impedance and admittance formulas of an overhead conductor. The derivation of the approximate formulas is described from the viewpoint of the physical behavior of current and voltage on a conductor. [Pg.32]

It should be noted that the impedance and admittance in this equation become a matrix when a conductor system is composed of multiconductors. Remember that a single-phase cable is, in general, a multiconductor system because the cable consists of a core and a metallic sheath or a screen. In an overhead conductor, no conductor internal admittance y exists, except a... [Pg.33]

Impedance and Admittance Formulation of an Overhead Conductor System... [Pg.44]

Summarizing the earlier sections, the impedance and the admittance of an overhead conductor system are given in the following form ... [Pg.14]

This section explains impedance and admittance formulas of nonuniform lines, such as finite-length horizontal and vertical conductors based on a plane wave assumption. The formulas are applied to analyze a transient on a nonuniform line by an existing circuit theory-based simulation tool such as the EMTP [9,11]. The impedance formula is derived based on Neumann s inductance formula by applying the idea of complex penetration depth explained earlier. The admittance is obtained from the impedance assuming the wave propagation velocity is the same as the light velocity in free space in the same manner as an existing admittance formula, which is almost always used in steady-state and transient analyses on an overhead line. [Pg.138]


See other pages where Overhead conductor admittance is mentioned: [Pg.44]    [Pg.573]    [Pg.480]    [Pg.105]   
See also in sourсe #XX -- [ Pg.13 ]




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Admittance

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