2.8 inductancia de linea sin ejercicio.pptx
TRANSCRIPT
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INGENIERÍA ELECTROMECÁNICA
ASIGNATURA: SISTEMAS ELECTRICOS DE POTENCIA
2.8 Inductancia de línea de conductores compuestos.
PRESENTA:
IDALFI SANTANA MOJICA
SEMESTRE: AGOSTO-DICIEMBRE
Manzana 30, Lote 1, Col. El Limón, C.P. 40880, Zihautanejo, Gro.Tels. 755-554-48-51, 755-554-4852, 755-554-54-87, fax. Ext 110
www.itcostagrande.edu.ma e-mail : [email protected]
Subsecretaría de Educación Superior
Dirección General de Educación Superior Tecnológica
Instituto Tecnológico de la Costa Grande
NO. CONTROL
12570172
INSTITUTO TECNOLÓGICO DE LA COSTA GRANDE
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INTRODUCTION
In the evaluation of inductance, solid round conductors were considered. However, in practical transmission lines, stranded conductors are used. Also, for reasons of economy, most EHV lines are constructed with bundled conductors. In this section an expression is found for the inductance of composite conductors. The result can be used for evaluating the GMR of stranded or bundled conductors. It is also useful in finding the equivalent GMR and GMD of parallel circuits. Consider a single phase line consisting of two composite conductors (x) and (y) as shown in Figure 4.10.
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The current in (x) is (I) reference into the page, and the return current in (y) is (-I). Conductor (x) consists of N identical strands or semiconductors, each with radius (rX). Conductor (y) consists of M identical strands or semiconductors, each with radius (rY). The current is assumed to be equally divided among the semiconductors. The current per strand is (I/N) in x and (I/M) in Y. The application of (4.29) will result in the following expression for the total flux linkage of conductor (a).
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Using (4.29), the inductance of other subconductors in (x) are similarly obtained. For example, the inductance of the subconductors n is.
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The average inductance of any one subconductor in group x is
Since all the subconductors of conductor x are electrically parallel, the inductance of x will
Substituting the values of la, lb,lc...,ln in (4.47) results in
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• GMD is the mnthe root of the mnthe distances between n strands of conductor x m strands. GMRx is the n^2 root of the product of n^2 terms consisting of r´ of every strand times the distance from each strand to all other strands within group x.• The inductance of conductor y can also be similarly obtained. The
geometric mean radius GMRy will be different. The geometric mean distance GMD, however, is the same.