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| Content Provider | IEEE Xplore Digital Library |
|---|---|
| Author | Lopez, A. Villasevil, F. Pindado, R. Noriega, G. Platzek, D. |
| Copyright Year | 2006 |
| Description | Author affiliation: Departamento Ingenieria Electron., Univ. Politecnica de Catalunya, Barcelona (Lopez, A.; Villasevil, F.) |
| Abstract | The understanding of the temperature profile in a semiconductor structure in each of its directions is essential for determining its intrinsic characteristics. By means of the use of tools like the microprobe, it is possible to find some of these characteristics [Plazek, D, et. al., 2003]. A problem with the microprobe is to know with precision the transient evolution of the initial temperature when it comes in contact with the sample. With the help of suitable mathematical models, it is possible to know the evolving temperature flux as a function of time and space. In the linear space and with the use of Laplacian solutions, a useful solution can be obtained. In this paper, a temperature fluctuation evolution model by discrete state-space has been developed. The most direct application is to develop valid algorithms to apply to support software. The impact in a thermoelectric system is basically to give improved knowledge of the temperature fluctuations throughout a semiconductor, taking into account more than one dimension. The verification of results using semiconductor compound samples used in thermoelectrics (BiTe, Skutterudite, etc.), allows us to determine graphically the thermoelectric properties that characterize them. By means of the use of thermal scanning and the use of thermocouples, it is possible to build up a function of the Seebeck coefficient in the measurement direction (microprobe). It is quite interesting to know the initial transitory measurements to characterize in an optimal way the results obtained from the thermal system (????). The diffusivity (beta) of the material is a parameter that modulates the exponential response of the system. By means of the use of a discrete-time system [Dominguez, S, et. al., 2001] it is possible to simplify the analysis and the development of the algorithms. There are few ways to do the sampling: (1) Conventional periodical sampling or uniform sampling. In this case the interval of sampling is a constant: t $_{k}$ = T (k = 0,1,2,...). (2) Sampling of multiple order: in this case $t_{k}$ will repeat periodically, where $t_{k+r}-t_{k}$ is a constant for all k. (3) Sampling of multiple order: in this case there is a simultaneous agreement of two sample operations in $t_{k}$ = $pT_{1}$ and $qT_{2}$ where $T_{1}$ and $T_{2}$ are constant and p and q are integer values. (4) Random sampling: in this case the instant moments of the sampling $t_{k}$ is a random variable. In this work a periodic sampling has been considered, with sampling time-collection: t(k) = kT (k = 0,1,2,... ) |
| Starting Page | 296 |
| Ending Page | 299 |
| File Size | 193739 |
| Page Count | 4 |
| File Format | |
| ISBN | 1424408105 |
| ISSN | 10942734 |
| DOI | 10.1109/ICT.2006.331373 |
| Language | English |
| Publisher | Institute of Electrical and Electronics Engineers, Inc. (IEEE) |
| Publisher Date | 2006-08-06 |
| Publisher Place | Austria |
| Access Restriction | Subscribed |
| Rights Holder | Institute of Electrical and Electronics Engineers, Inc. (IEEE) |
| Subject Keyword | Mathematical model Thermoelectricity Sampling methods Temperature Fluctuations Semiconductor materials Laplace equations Application software Software algorithms Algorithm design and analysis |
| Content Type | Text |
| Resource Type | Article |
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