Stability of Algorithms for Electro-Magnetic-Transient Simulation of Networks With Switches and Non-Linear Inductors

2020 ◽  
Vol 35 (1) ◽  
pp. 377-385
Author(s):  
Huanfeng Zhao ◽  
Shengtao Fan ◽  
Aniruddha M. Gole
1995 ◽  
Vol 10 (3) ◽  
pp. 1505-1510 ◽  
Author(s):  
Y. Kowada ◽  
I. Iyoda ◽  
N. Sato ◽  
A. Yamazaki ◽  
S. Matoba

1964 ◽  
Vol 19 (7-8) ◽  
pp. 825-827
Author(s):  
G. Braunss

It is shown that the non-linear term of the HEisENBERG-PAULi-equation can be interpreted as torsion of space-time in the following way. The wavefuinction is subjected to a (non-rigid) LORENTZ-transformation varying from point to point: ψ = Sψ'. If the matrix S=S(x) is chosen so that it satisfies the equation γλ(∂S/∂xλ) S-1+l2γλγ5 ψ̅ γλγ5ψ=0, than the non-linear term of the H.-P.-equation vanishes in the system x'; i. e.with (∂xλ/∂xμ′) γμ=S-1 γλ S one has 0=γλ(∂ψ/∂xλ) +l2γλγ5 ψ ψ̅ γλ γ5 ψ ≡ S γμ (∂ψ'/∂xμ′). This result holds also in the case where the H.-P.-equation contains still a term with γλ ψ̅ γλ ψ and/or γλ Αλ (Aλ = electro-magnetic potential), provided Aλ satisfies the LoRENTz-condition ∂Aλ/∂xλ=0. The proof is a follows: Taking a representation of S in the DIRAC-ring, the equation which determines S splits into 8 equations. Between these equations there exist 2 identities (which correspond to the PAULI—GuRSEY-transformation resp. LoRENTz-condition); so one finally has 6 equations for the determination of the 6 parameters of S.


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