Scaling of the Steady-State Load Flow Equations for Multi-Carrier Energy Systems

Conference Paper (2021)
Author(s)

A. S. Markensteijn (TU Delft - Numerical Analysis)

Johan Romate (Shell Global Solutions International B.V., TU Delft - Numerical Analysis)

Kees Vuik (TU Delft - Numerical Analysis)

Research Group
Numerical Analysis
Copyright
© 2021 A.S. Markensteijn, J.E. Romate, Cornelis Vuik
DOI related publication
https://doi.org/10.1007/978-3-030-55874-1_70
More Info
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Publication Year
2021
Language
English
Copyright
© 2021 A.S. Markensteijn, J.E. Romate, Cornelis Vuik
Research Group
Numerical Analysis
Bibliographical Note
Green Open Access added to TU Delft Institutional Repository ‘You share, we take care!’ – Taverne project https://www.openaccess.nl/en/you-share-we-take-care Otherwise as indicated in the copyright section: the publisher is the copyright holder of this work and the author uses the Dutch legislation to make this work public.@en
Pages (from-to)
713-721
ISBN (print)
978-3-030-55873-4
ISBN (electronic)
978-3-030-55874-1
Reuse Rights

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Abstract

Coupling single-carrier networks (SCNs) into multi-carrier energy systems (MESs) has recently become more important. Steady-state load flow analysis of energy systems leads to a system of nonlinear equations, which is usually solved using the Newton-Raphson method (NR). Due to various physical scales within a SCN, and between different SCNs in a MES, scaling might be needed to solve the nonlinear system. In single-carrier electrical networks, per unit scaling is commonly used. However, in the gas and heat networks, various ways of scaling or no scaling are used. This paper presents a per unit system and matrix scaling for load flow models for a MES consisting of gas, electricity, and heat. The effect of scaling on NR is analyzed. A small example MES is used to demonstrate the two scaling methods. This paper shows that the per unit system and matrix scaling are equivalent, assuming infinite precision. In finite precision, the example shows that the NR iterations are slightly different for the two scaling methods. For this example, both scaling methods show the same convergence behavior of NR in finite precision.

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