{"title":"非箝位电感开关(UIS)测试中校正晶体管单脉冲雪崩能量(Eas)的电路电感测量","authors":"Jian-Hsing Lee;Ching-Ho Li;Chih-Cherng Liao;Gong-Kai Lin;Yu-Sheng Chiu;Chieh-Yao Chuang;Ke-Horng Chen","doi":"10.1109/TED.2024.3509398","DOIUrl":null,"url":null,"abstract":"The single-mode avalanche energy (\n<inline-formula> <tex-math>${E}_{\\text {as}}\\text {)}$ </tex-math></inline-formula>\n evaluated from the unclamped inductive-switching (UIS) test has been used in many application notes and literature as the ruggedness index of a transistor. The inductance is the key parameter for \n<inline-formula> <tex-math>${E}_{\\text {as}}$ </tex-math></inline-formula>\n calculation. From the in-circuit measurement, the inductance at the channel turn-off time (\n<inline-formula> <tex-math>${t}_{\\text {off}}\\text {)}$ </tex-math></inline-formula>\n is found smaller than the default inductance for the power transistor under the UIS test. However, most UIS testers still use the default inductance to calculate \n<inline-formula> <tex-math>${E}_{\\text {as}}$ </tex-math></inline-formula>\n. In this article, whether the inductance can keep constant during \n<inline-formula> <tex-math>${t}_{\\text {off}}$ </tex-math></inline-formula>\n for any transistor under any test condition of UIS and why it is smaller than the default inductance during \n<inline-formula> <tex-math>${t}_{\\text {off}}$ </tex-math></inline-formula>\n for air core inductors is investigated. Without the ferrite core, the magnetization (M) of the air core inductor during the UIS test is caused by the eddy currents, which increase with increasing current and decrease with decreasing current linearly. Therefore, the differential magnetization (dM/dH) is constant, resulting in two different inductances during channel turn-on time (\n<inline-formula> <tex-math>${t}_{\\text {on}}\\text {)}$ </tex-math></inline-formula>\n and turn-off time \n<inline-formula> <tex-math>${t}_{\\text {off}}$ </tex-math></inline-formula>\n.","PeriodicalId":13092,"journal":{"name":"IEEE Transactions on Electron Devices","volume":"72 1","pages":"317-322"},"PeriodicalIF":2.9000,"publicationDate":"2024-12-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"In-Circuit Inductance Measurement to Correct the Single-Pulse Avalanche Energy (Eas) of Transistor Under the Unclamped Inductive-Switching (UIS) Test\",\"authors\":\"Jian-Hsing Lee;Ching-Ho Li;Chih-Cherng Liao;Gong-Kai Lin;Yu-Sheng Chiu;Chieh-Yao Chuang;Ke-Horng Chen\",\"doi\":\"10.1109/TED.2024.3509398\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The single-mode avalanche energy (\\n<inline-formula> <tex-math>${E}_{\\\\text {as}}\\\\text {)}$ </tex-math></inline-formula>\\n evaluated from the unclamped inductive-switching (UIS) test has been used in many application notes and literature as the ruggedness index of a transistor. The inductance is the key parameter for \\n<inline-formula> <tex-math>${E}_{\\\\text {as}}$ </tex-math></inline-formula>\\n calculation. From the in-circuit measurement, the inductance at the channel turn-off time (\\n<inline-formula> <tex-math>${t}_{\\\\text {off}}\\\\text {)}$ </tex-math></inline-formula>\\n is found smaller than the default inductance for the power transistor under the UIS test. However, most UIS testers still use the default inductance to calculate \\n<inline-formula> <tex-math>${E}_{\\\\text {as}}$ </tex-math></inline-formula>\\n. In this article, whether the inductance can keep constant during \\n<inline-formula> <tex-math>${t}_{\\\\text {off}}$ </tex-math></inline-formula>\\n for any transistor under any test condition of UIS and why it is smaller than the default inductance during \\n<inline-formula> <tex-math>${t}_{\\\\text {off}}$ </tex-math></inline-formula>\\n for air core inductors is investigated. Without the ferrite core, the magnetization (M) of the air core inductor during the UIS test is caused by the eddy currents, which increase with increasing current and decrease with decreasing current linearly. Therefore, the differential magnetization (dM/dH) is constant, resulting in two different inductances during channel turn-on time (\\n<inline-formula> <tex-math>${t}_{\\\\text {on}}\\\\text {)}$ </tex-math></inline-formula>\\n and turn-off time \\n<inline-formula> <tex-math>${t}_{\\\\text {off}}$ </tex-math></inline-formula>\\n.\",\"PeriodicalId\":13092,\"journal\":{\"name\":\"IEEE Transactions on Electron Devices\",\"volume\":\"72 1\",\"pages\":\"317-322\"},\"PeriodicalIF\":2.9000,\"publicationDate\":\"2024-12-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"IEEE Transactions on Electron Devices\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://ieeexplore.ieee.org/document/10805753/\",\"RegionNum\":2,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE Transactions on Electron Devices","FirstCategoryId":"5","ListUrlMain":"https://ieeexplore.ieee.org/document/10805753/","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
In-Circuit Inductance Measurement to Correct the Single-Pulse Avalanche Energy (Eas) of Transistor Under the Unclamped Inductive-Switching (UIS) Test
The single-mode avalanche energy (
${E}_{\text {as}}\text {)}$
evaluated from the unclamped inductive-switching (UIS) test has been used in many application notes and literature as the ruggedness index of a transistor. The inductance is the key parameter for
${E}_{\text {as}}$
calculation. From the in-circuit measurement, the inductance at the channel turn-off time (
${t}_{\text {off}}\text {)}$
is found smaller than the default inductance for the power transistor under the UIS test. However, most UIS testers still use the default inductance to calculate
${E}_{\text {as}}$
. In this article, whether the inductance can keep constant during
${t}_{\text {off}}$
for any transistor under any test condition of UIS and why it is smaller than the default inductance during
${t}_{\text {off}}$
for air core inductors is investigated. Without the ferrite core, the magnetization (M) of the air core inductor during the UIS test is caused by the eddy currents, which increase with increasing current and decrease with decreasing current linearly. Therefore, the differential magnetization (dM/dH) is constant, resulting in two different inductances during channel turn-on time (
${t}_{\text {on}}\text {)}$
and turn-off time
${t}_{\text {off}}$
.
期刊介绍:
IEEE Transactions on Electron Devices publishes original and significant contributions relating to the theory, modeling, design, performance and reliability of electron and ion integrated circuit devices and interconnects, involving insulators, metals, organic materials, micro-plasmas, semiconductors, quantum-effect structures, vacuum devices, and emerging materials with applications in bioelectronics, biomedical electronics, computation, communications, displays, microelectromechanics, imaging, micro-actuators, nanoelectronics, optoelectronics, photovoltaics, power ICs and micro-sensors. Tutorial and review papers on these subjects are also published and occasional special issues appear to present a collection of papers which treat particular areas in more depth and breadth.