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An analysis of generation mechanisms of transitional peak current in sense‐emitter current for IGBTs with current sense and techniques to remove it
Author(s) -
Hagino Hiroyasu,
Yamada Tomihisa,
Uenishi Akio,
Tomomatsu Yoshifumi
Publication year - 1995
Publication title -
electrical engineering in japan
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.136
H-Index - 28
eISSN - 1520-6416
pISSN - 0424-7760
DOI - 10.1002/eej.4391150809
Subject(s) - sense (electronics) , current (fluid) , common emitter , overcurrent , electrical engineering , computer science , optoelectronics , materials science , engineering
It is important to remove the transitional peak current in sense‐emitter current which is due to dynamic current‐sharing during turn‐on for a design of IGBTs with current‐sense used protection against overcurrent and short circuit. But this analysis has been scarcely investigated. This paper clarifies generation mechanisms of the transitional peak current by simulations and experiments using a parallel operation model and reports on techniques to remove it. The following results were obtained. (1) In the two paralleling devices model which consists of a sense cell and main cells, the transitional peak current occurs during turn‐on when a sense cell turns on faster than main cells. In this case, the main parameters that effect dynamic currents imbalance are gate resistance (Rg) and gate threshold voltage (Vth). (2) In dynamic currents imbalance based on individual Rg and Vth among main cells, it may be treated as a two‐paralleling devices model which consists of a sense cell with Rgs and Vths, and main cells with average values Rgm and Vthm. (3) The transitional peak current can be removed by the design of Rgs and Vths in a sense cell are larger than average values of Rgm and Vthm in main cells. (4) On trial IGBTs with current sense Vths in a sense cell is different from the average‐value Vthm in main cells to change impurity concentrations of each channel. It was confirmed that the transitional peak current in sense‐emitter current can be removed by the design that Vths in a sense cell is larger than average value Vthm in main cells.

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