2002
DOI: 10.1109/16.974765
|View full text |Cite
|
Sign up to set email alerts
|

Applications of blow-up theory to thyristor turn-on

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

2007
2007
2007
2007

Publication Types

Select...
1

Relationship

0
1

Authors

Journals

citations
Cited by 1 publication
(1 citation statement)
references
References 13 publications
0
1
0
Order By: Relevance
“…Under forward‐blocking conditions ( U A >0), junction J 2 is reverse biased and the other two junctions are forward biased. On the stationary state, the above equation system can be reduced to the well‐known and simple equation (Paisana and Santos, 2002) where the positive feedback is evidenced: Equation 3 where I C0 is associated to the reversed biased junction J 2 and the new α ′ fp takes in consideration the changing of the cathode emitter efficiency due to the effect of the short emitter resistance R s . On the off state, the total dynamic current gain sum is α˜ T = α˜ fp + α˜ fn <1.…”
Section: The Model Equationsmentioning
confidence: 99%
“…Under forward‐blocking conditions ( U A >0), junction J 2 is reverse biased and the other two junctions are forward biased. On the stationary state, the above equation system can be reduced to the well‐known and simple equation (Paisana and Santos, 2002) where the positive feedback is evidenced: Equation 3 where I C0 is associated to the reversed biased junction J 2 and the new α ′ fp takes in consideration the changing of the cathode emitter efficiency due to the effect of the short emitter resistance R s . On the off state, the total dynamic current gain sum is α˜ T = α˜ fp + α˜ fn <1.…”
Section: The Model Equationsmentioning
confidence: 99%