Documentation Home Page HYPERSIM Home Page
Pour la documentation en FRANÇAIS, utilisez l'outil de traduction de votre navigateur Chrome, Edge ou Safari. Voir un exemple.

Skip to end of metadata
Go to start of metadata

You are viewing an old version of this content. View the current version.

Compare with Current View Version History

« Previous Version 2 Current »

INTRODUCTION


The HYPERSIM Transformer tools accurately reproduce the behavior of a three-phase linear model, two or three winding transformers at power frequency located in each parameter form of Z-based transformer components respectively.

Three-limb core - three windings

Three-limb core: three windings

  • HYPERSIM works with an Inductance matrix transformer model. This model represents only a three-limb or five-limb core. The three single-phase cores are not actually supported (Z0 = Z1).
  • Each single-phase transformer is modeled by 3 coupled windings.
  • A 3-leg 3-windings transformer with Z0 different from Z1 is modeled by 9 coupled windings ordered in the [L] and [R] matrices in the next section.
  • For a 3-leg 2-windings transformer, the transformer is modeled by 6 coupled windings ordered in the [L] and [R] matrices in the next section.

Inductance Matrix Transformer Model

The inductance matrix transformer model implements this relationship equation:

Where R1 to R9 represent the winding resistances. Lii represents the self-inductance and the Lij represents the mutual inductance.
The calculation of the inductance matrix transformer is performed by these equations.

Positive-Sequence and Mutual Reactances

The zero-sequence self reactances

and mutual reactance

are also computed using similar equations.

Q1iThree-phase reactive power absorbed by winding i at no load when winding i is excited by a positive-sequence voltage Vnomi with winding j open
Q1jThree-phase reactive power absorbed by winding j at no load when winding j is excited by a positive-sequence voltage Vnomj with winding i open
X1ijpositive-sequence short-circuit reactance seen from winding i when winding j is short-circuited
Vnomi, Vnomjnominal line-line voltages of windings i and j


If we extend the two 2x2 reactance matrices in positive-sequence and in zero-sequence, to a 6x6 matrix, and replace the four scalar terms by a 3x3, we have this matrix:

Where the self and mutual terms are given by:

To model the core losses (P1 and P0 in positive and zero-sequence), additional shunt resistances are connected between windings.

The resistances equation is:

The default parameters are for a three-phase 3-windings transformer.

Enter your own transformer parameters in the Transformer data Tab in the Z-based parameter form, under Parameters Tab.

See Transformer Data Tab | GUI & Toolbox Icons











  • No labels