{"title":"Temperature dependence of resistance in Black's equation and in calibration for SWEAT and NIST structures: the parameter T/sub EO/","authors":"C. R. Crowell, C. Shih, K. Jonggook, V. Tyree","doi":"10.1109/IRWS.1999.830579","DOIUrl":null,"url":null,"abstract":"The equation for resistance R(T) at temperature T can be expressed in the form R(T)=(dR/dT).(T-T/sub EO/. When dR/dT is constant over the range of your experiment, T/sub EO/ is then a constant, the temperature at which R(T) extrapolates to zero. If we wish to express the corresponding relationship with /spl beta/(T/sub r/), the temperature coefficient of resistivity (TCR) at temperature T/sub r/, /spl beta/(T/sub r/) is defined in the form /spl beta/(T/sub r/)=(dR/dT/sub r/).(1/R(T/sub r/))=1/(T/sub r/-T/sub EO/). For both these equations it is desirable to use the Kelvin scale for T, especially when activation energy terms occur in the test under consideration. Our experimental measurements of temperature calibration have yielded T/sub EO/ values less than 40 degrees Kelvin, and with sufficient accuracy such that materials properties can be usefully determined provided that the test temperature is not too high. When /spl beta/(T/sub r/) is specified by an independent source, it is necessary that T/sub r/ be included in both theoretical and experimental cases.","PeriodicalId":131342,"journal":{"name":"1999 IEEE International Integrated Reliability Workshop Final Report (Cat. No. 99TH8460)","volume":"53 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1999-10-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"1999 IEEE International Integrated Reliability Workshop Final Report (Cat. No. 99TH8460)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/IRWS.1999.830579","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The equation for resistance R(T) at temperature T can be expressed in the form R(T)=(dR/dT).(T-T/sub EO/. When dR/dT is constant over the range of your experiment, T/sub EO/ is then a constant, the temperature at which R(T) extrapolates to zero. If we wish to express the corresponding relationship with /spl beta/(T/sub r/), the temperature coefficient of resistivity (TCR) at temperature T/sub r/, /spl beta/(T/sub r/) is defined in the form /spl beta/(T/sub r/)=(dR/dT/sub r/).(1/R(T/sub r/))=1/(T/sub r/-T/sub EO/). For both these equations it is desirable to use the Kelvin scale for T, especially when activation energy terms occur in the test under consideration. Our experimental measurements of temperature calibration have yielded T/sub EO/ values less than 40 degrees Kelvin, and with sufficient accuracy such that materials properties can be usefully determined provided that the test temperature is not too high. When /spl beta/(T/sub r/) is specified by an independent source, it is necessary that T/sub r/ be included in both theoretical and experimental cases.
温度T时电阻R(T)的方程可以表示为R(T)=(dR/dT)。(t t / sub EO /。当dR/dT在你的实验范围内保持恒定时,T/下标EO/就是一个常数,在这个温度下R(T)推断为零。如果我们希望表示与/spl β /(T/下标r/)的对应关系,则温度T/下标r/, /spl β /(T/下标r/)的电阻率温度系数(TCR)定义为/spl β /(T/下标r/)=(dR/dT/下标r/)。(1/R(T/ R /))=1/(T/ R /-T/ EO/)对于这两个方程,使用开尔文标度表示T是可取的,特别是在考虑的试验中出现活化能项时。我们对温度校准的实验测量已经产生了小于40开尔文的T/sub EO/值,并且具有足够的精度,因此只要测试温度不太高,就可以有效地确定材料的性能。当/spl beta/(T/sub r/)由独立源指定时,在理论和实验案例中都必须包含T/sub r/。