Y. Fukuyama, Norihiko Sakamoto, N. Kaneko, T. Kondo, J. Toyoizumi, T. Yudate
{"title":"The effect of the distribution of α-spots in the peripheral part of an apparent contact point on constriction resistance","authors":"Y. Fukuyama, Norihiko Sakamoto, N. Kaneko, T. Kondo, J. Toyoizumi, T. Yudate","doi":"10.1109/HOLM.2017.8088103","DOIUrl":null,"url":null,"abstract":"The constriction resistance resulting from the constriction of current flow is one of main components in the contact resistance of electrical contacts in connectors. When the current flow has a round-shaped section as a contact point, the constriction resistance can be calculated analytically; however, this is not the case for real contacts. In the apparent contact point between two electrodes, there are many real contact points called a-spots. Even in the apparent contact point, there is no current flow in other part than the a-spots. Thus, the area of apparent contact point is not equal to the total area of a-spots and its constriction resistance cannot be calculated. From some previous studies, it is suggested that the constriction resistance of the contact with a-spots concentrated on a peripheral part of its apparent contact point is lower than that of the other if the total area of a-spots is constant. We fabricated some contact-like-structures on Si chips with various distributions of \"a-spots\" along the peripheral part of their \"apparent contact point\" using nanofabrication technology and compared their constriction resistances with each other for examining the relation between the distribution of a-spots and constriction resistance. Our simplified samples have shown resistance values between the calculation results using the Holm's equation and the Greenwood's equation.","PeriodicalId":354484,"journal":{"name":"2017 IEEE Holm Conference on Electrical Contacts","volume":"58 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2017-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2017 IEEE Holm Conference on Electrical Contacts","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/HOLM.2017.8088103","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 3
Abstract
The constriction resistance resulting from the constriction of current flow is one of main components in the contact resistance of electrical contacts in connectors. When the current flow has a round-shaped section as a contact point, the constriction resistance can be calculated analytically; however, this is not the case for real contacts. In the apparent contact point between two electrodes, there are many real contact points called a-spots. Even in the apparent contact point, there is no current flow in other part than the a-spots. Thus, the area of apparent contact point is not equal to the total area of a-spots and its constriction resistance cannot be calculated. From some previous studies, it is suggested that the constriction resistance of the contact with a-spots concentrated on a peripheral part of its apparent contact point is lower than that of the other if the total area of a-spots is constant. We fabricated some contact-like-structures on Si chips with various distributions of "a-spots" along the peripheral part of their "apparent contact point" using nanofabrication technology and compared their constriction resistances with each other for examining the relation between the distribution of a-spots and constriction resistance. Our simplified samples have shown resistance values between the calculation results using the Holm's equation and the Greenwood's equation.