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The '''star-mesh transform''' (or '''star-polygon transform''') is a mathematical technique to transform a [[network analysis (electrical circuits)|resistive network]] into an equivalent network with one less node.
The '''star-mesh transform''' (or '''star-polygon transform''') is a mathematical technique to transform a [[network analysis (electrical circuits)|resistive network]] into an equivalent network with one less node. The equivalence follows from the [[Schur complement]] identity applied to the Kirchhoff matrix of the network.


[[File:Star-mesh transform.svg|400px|center]]
[[File:Star-mesh transform.svg|400px|center]]
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* {{Cite doi|10.1109/TCT.1973.1083633}}
* {{Cite doi|10.1109/TCT.1973.1083633}}
* {{Cite doi|10.1109/TCT.1961.1086832}}
* {{Cite doi|10.1109/TCT.1961.1086832}}
* E.B. Curtis, D. Ingerman, J.A. Morrow. Circular planar graphs and resistor networks. Linear Algebra and its Applications. Volume 283, Issues 1–3, 1 November 1998, Pages 115–150.


[[Category:Electrical circuits]]
[[Category:Electrical circuits]]

Revision as of 00:34, 9 June 2012

The star-mesh transform (or star-polygon transform) is a mathematical technique to transform a resistive network into an equivalent network with one less node. The equivalence follows from the Schur complement identity applied to the Kirchhoff matrix of the network.

Given the impedances between the star node (to be eliminated) and N other nodes, the transform yields equivalent impedances between these other nodes:

The transform replaces N resistors with resistors. For , the result is an increase in the number of resistors, so the transform has no general inverse without additional constraints.

It is possible, though not necessarily efficient, to transform an arbitrarily complex two-terminal resistive network into a single equivalent resistor by repeatedly applying the star-mesh transform to eliminate each non-terminal node.

Special cases

  • N = 1: For a single dangling resistor, the transform eliminates the resistor.
  • N = 2: For two resistors, the "star" is simply the two resistors in series, and the transform yields a single equivalent resistor.
  • N = 3: The special case of three resistors is better known as the Y-Δ transform. Since the result also has three resistors, this transform has an inverse Δ-Y transform.

See also

References

  • Attention: This template ({{cite doi}}) is deprecated. To cite the publication identified by doi:10.1109/TCT.1973.1083633, please use {{cite journal}} (if it was published in a bona fide academic journal, otherwise {{cite report}} with |doi=10.1109/TCT.1973.1083633 instead.
  • Attention: This template ({{cite doi}}) is deprecated. To cite the publication identified by doi:10.1109/TCT.1961.1086832, please use {{cite journal}} (if it was published in a bona fide academic journal, otherwise {{cite report}} with |doi=10.1109/TCT.1961.1086832 instead.
  • E.B. Curtis, D. Ingerman, J.A. Morrow. Circular planar graphs and resistor networks. Linear Algebra and its Applications. Volume 283, Issues 1–3, 1 November 1998, Pages 115–150.