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dc.contributor.advisorGang Chen.en_US
dc.contributor.authorMonreal, Jorgeen_US
dc.contributor.otherMassachusetts Institute of Technology. Dept. of Materials Science and Engineering.en_US
dc.date.accessioned2008-09-03T14:44:54Z
dc.date.available2008-09-03T14:44:54Z
dc.date.copyright2007en_US
dc.date.issued2007en_US
dc.identifier.urihttp://hdl.handle.net/1721.1/42156
dc.descriptionThesis (M. Eng.)--Massachusetts Institute of Technology, Dept. of Materials Science and Engineering, 2007.en_US
dc.descriptionIncludes bibliographical references (leaves 77-78).en_US
dc.description.abstractThermoelectric properties have been known since the initial discovery in 1821 by Thomas Seebeck, who found that a current flowed at the junction of two dissimilar metals when placed under a temperature differential. This was followed by the discovery in 1834 by John Peltier, that the inverse was also true. That is, that a current applied to two dissimilar metals would yield a temperature differential. Interest in thermoelectrics laid dormant for almost 100 years and were primarily a laboratory curiosity. That interest was revived in the early 1900s with applications for remote power generation aboard satellites and several military applications. Thermoelectric devices, such as beverage coolers or thermocouples for temperature sensors, that tried to make use of these characteristics shortly followed. However, commercial success soon slowed down as efficiencies of the materials were not conducive to profitability. The effectiveness of a thermoelectric was described by a dimensionless figure of merit given by ZT=(S2a/ke+kp)T, where S is the Seebeck coefficient, T is the operational temperature, a is the electrical conductivity, ke is the electron contribution to thermal conductivity, and kp is the thermal conductivity due to phonon propagation across a crystal lattice. From the mid-1940s until the 1970s there was very slow progress in increased thermoelectric material efficiency, which culminated in a ZT=1 with (Bi2Te3). For approximately 30 years progress stagnated. In 1993, however, new ideas emerged that called for the fabrication of low dimensional structures to enhance electron conductivity while inhibiting phonon contribution to thermal conductivity. Advancements in material efficiency have made great progress since then.en_US
dc.description.abstract(cont.) Businesses are, once again, looking at thermoelectrics for potential commercial ventures. This thesis will begin with an examination of the theory behind thermoelectric properties, followed by an explanation of the methods used to assess thermoelectric device and material performance. It will then review some of the advancements made in low dimensional structures such as two-dimensional structures of quantum wells, one-dimensional nanowires, and zero-dimensional quantum dots. A market analysis of current commercial applications is presented. A proposed business model exploiting the power generation mode of thermoelectric devices is introduced. And, finally, an overview of the intellectual property landscape describes several patents relevant to the proposed business model.en_US
dc.description.statementofresponsibilityby Jorge Monreal.en_US
dc.format.extent83 leavesen_US
dc.language.isoengen_US
dc.publisherMassachusetts Institute of Technologyen_US
dc.rightsM.I.T. theses are protected by copyright. They may be viewed from this source for any purpose, but reproduction or distribution in any format is prohibited without written permission. See provided URL for inquiries about permission.en_US
dc.rights.urihttp://dspace.mit.edu/handle/1721.1/7582en_US
dc.subjectMaterials Science and Engineering.en_US
dc.titleThermoelectrics : material advancements and market applicationsen_US
dc.typeThesisen_US
dc.description.degreeM.Eng.en_US
dc.contributor.departmentMassachusetts Institute of Technology. Department of Materials Science and Engineering
dc.identifier.oclc228504510en_US


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