Supplementary techniques for 2S-DIRK-based EMT simulations
-
Add time:08/28/2019 Source:sciencedirect.com
Electromagnetic transient (EMT) simulations are now often used for system studies including power electronics converters which control voltages and currents using switching devices. The trapezoidal method, used in Electro-Magnetic Transients Program (EMTP) for numerical integration, produces “fictitious” sustained numerical oscillation, when an inductor current or a capacitor voltage is suddenly changed especially by switching. To cope with this problem, the research group of the authors has proposed applying the two-stage diagonally implicit Runge–Kutta (2S-DIRK) method which is an inherently “oscillation-free” numerical integration method. In order to bring out full accuracy of the 2S-DIRK method, supplementary numerical techniques are required for the representation of voltage sources, current sources and switches. This paper illustrates these techniques with numerical examples.
We also recommend Trading Suppliers and Manufacturers of (-)-N-[[(2S)-1-Ethyl-2-pyrrolidinyl]methyl]-2-hydroxy-3-iodo-6-methoxybenzamide (cas 113716-48-6). Pls Click Website Link as below: cas 113716-48-6 suppliers
Prev:Beyond nPDFs effects: Prompt J/ψ and ψ(2S) production in pPb and pp collisions
Next:Crystal structure of mature 2S albumin from Moringa oleifera seeds) - 【Back】【Close 】【Print】【Add to favorite 】
- Related Information
- Crystal structure of mature 2S albumin from Moringa oleifera seeds08/29/2019
- Beyond nPDFs effects: Prompt J/ψ and ψ(2S) production in pPb and pp collisions08/27/2019
- Synthesis and preliminary evaluation of a novel glutamine derivative: (2S,4S)4-[18F]FEBGln08/26/2019
- Brief communicationPru du 2S albumin or Pru du vicilin?08/25/2019
- Structural insights into the molecular function of human [2Fe-2S] BOLA1-GRX5 and [2Fe-2S] BOLA3-GRX5 complexes08/24/2019
- Results from the CBC3 readout ASIC for CMS 2S-modules08/23/2019
- Measurement of Γee×Bμμ for ψ(2S) meson08/22/2019
- Measurement of prompt ψ(2S) production cross sections in proton–lead and proton–proton collisions at sNN=5.02TeV08/21/2019


