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 ...Show MoreMetadata
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.
Published in: 1999 IEEE International Integrated Reliability Workshop Final Report (Cat. No. 99TH8460)
Date of Conference: 18-21 October 1999
Date Added to IEEE Xplore: 06 August 2002
Print ISBN:0-7803-5649-7