Dissertations / Theses on the topic 'Thermoelectric System'
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Muto, Andrew (Andrew Jerome). "Thermoelectric device characterization and solar thermoelectric system modeling." Thesis, Massachusetts Institute of Technology, 2011. http://hdl.handle.net/1721.1/71506.
Full textCataloged from PDF version of thesis.
Includes bibliographical references (p. 152-155).
Recent years have witnessed a trend of rising electricity costs and an emphasis on energy efficiency. Thermoelectric (TE) devices can be used either as heat pumps for localized environmental control or heat engines to convert heat into electricity. Thermoelectrics are appealing because they have no moving parts, are highly reliable, have high power densities, and are scalable in size. They can be used to improve the overall efficiency of many systems including vehicle waste heat, solar thermal, HVAC, industrial waste heat, and remote power for sensor applications. For thermoelectric generators to be successful, research progress at the device level must be made to validate materials and to guide system design. The focus of this thesis is thermoelectric device testing and system modeling. A novel device testing method is developed between room temperature range and 230°C. The experimental technique is capable of directly measuring an energy balance over a single leg, with a large temperature of 2-160°C. The technique measures all three TE properties of a single leg, in the same direction, with significantly less uncertainty than other methods. The measurements include the effects of temperature dependent properties, side wall radiation loss, and contact resistance. The power and efficiency were directly measured and are within 0.4 % and 2 % of the values calculated from the property measurements. The device property measurement was extended to higher temperatures up to 600°C. The experimental system uses an inline unicouple orientation to minimize radiation losses and thermal stress. Two major experimental challenges were the construction of a high temperature calibrated heater and a thermocouple attachment technique. We investigated skutterudite materials which are of interest to many research groups due to their high thermoelectric figure-of-merit (ZT), and good thermomechanical properties. Unlike room temperature Bi2Te 3 devices, skutterudite module construction techniques are not well established and were a major challenge in this work. Skutterudite device samples were fabricated by a direct bonding method in which a rigid electrode is sintered directly to the TE powder during press. Compatible electrode materials were identified and evaluated based on thermal stress, parasitic electrical/thermal resistance, chemical stability and ease of prototype fabrication. The final electrodes solutions were Co2 Si with the P-type and CoSi2 with the N-type. The direct hot press process was modified into what we call a hybrid hot press to produce device samples with strong bonds and no cracks. Preliminary accelerated aging tests were conducted to evaluate the long term chemical stability of the TE-electrode contacts. We demonstrated ZTff = 0.74 for the N-type between 52°C and 595°C corresponding to 11.7% conversion efficiency and Zlff = 0.51 for the P-type between 77°C and 600°C corresponding to 8.5% efficiency. The maximum efficiency of the NP unicouple was measured to be 9.1% at ~550°C. The effective ZT and efficiency measurement includes electrical contact resistance, and parasitic thermal/electrical resistance in the electrodes, and heat losses at the sides of the legs. Thus we have included all the parasitic loss effects that are present in a real unicouple. The efficiency values measured in this work are among the highest recorded for a skutterudite unicouple. The TE-electrode combinations meet all the criteria for device testing and offer a practical, manufacturable solution for module construction. Solar thermal power generation is fast becoming cost competitive for utility scale electricity with 380 MW electric currently installed. Parabolic trough concentrators have proven economical and reliable but their efficiency is limited by the maximum temperature of the heated fluid. We explored the idea of a solar thermoelectric topping cycle (STET) in which a thermoelectric generator (TEG) is added at high temperature to increase the overall efficiency of the solar Rankine cycle. In this design the perimeter of the receiver tube is covered with thermoelectrics so that the absorber temperature is raised and the energy rejected from the TEG is used to heat the fluid at its originally specified temperature. A heat transfer analysis was carried out to determine the overall system efficiency. A parametric study was performed to identity design constraints and put bounds on the total system efficiency. The system performance was simulated for all conceivable concentrations and fluid temperatures of a solar thermal trough. As the absorber temperature increases more power is generated by the TEG but is offset by a rapidly decreasing absorber efficiency which results in only a marginal increase in net power. It was concluded that for the proposed STET to increase the system efficiency of a state of the art trough system by 10% requires a ZI =3 TEG, which is well beyond the state-of-the-art thermoelectric materials.
by Andrew Muto.
Ph.D.
Al-Madhhachi, Hayder. "Solar powered thermoelectric distillation system." Thesis, Cardiff University, 2017. http://orca.cf.ac.uk/107598/.
Full textWang, Jue. "System Design, Fabrication, and Characterization of Thermoelectric and Thermal Interface Materials for Thermoelectric Devices." Diss., Virginia Tech, 2018. http://hdl.handle.net/10919/83546.
Full textPh. D.
Thompson, Megan Elizabeth Dove. "Fabrication and Testing of a Heat Exchanger Module for Thermoelectric Power Generation in an Automobile Exhaust System." Thesis, Virginia Tech, 2013. http://hdl.handle.net/10919/19233.
Full textThis study focuses on developing efficient heat exchanger modules for the cold side of the TEG through the analysis of experimental data. The experimental set up mimics conditions that were previously used in a computational fluid dynamics (CFD) model. This model tested several different geometries of cold side sections for the heat exchanger at standard coolant and exhaust temperatures for a typical car. The test section uses the same temperatures as the CFD model, but the geometry is a 1/5th scaled down model compared to an full-size engine and was fabricated using a metal-based rapid prototyping process. The temperatures from the CFD model are validated through thermocouple measurements, which provide the distribution of the temperatures across the TEG. All of these measurements are compared to the CFD model for trends and temperatures to ensure that the model is accurate. Two cold side geometries, a baseline geometry and an impingement geometry, are compared to determine which will produce the greater temperature gradient across the TEG.
Master of Science
Christian, Corey D. (Corey Dwight). "Breaking the thermo-mechanical coupling of thermoelectric materials : determining the viability of a thermoelectric generator." Thesis, Massachusetts Institute of Technology, 2019. https://hdl.handle.net/1721.1/121790.
Full textCataloged from PDF version of thesis.
Includes bibliographical references (pages 69-70).
Thermoelectric power generators (TEGs) convert a temperature difference into electricity. This temperature difference can be created from waste heat. Since up to 50% [1] of US industrial energy input is lost as waste heat, an economical means of recovering waste heat and converting it into useful electricity could represent significant energy savings. Coupled with our integrative system design which involves creating application specific thermoelectric arrays, this technology can also help enable low power generation for off-grid needs in the developing world. Although conversion efficiencies as high as 20.9% [2] (heat to electrical energy) have been predicted from simulations of TEGs systems, in practice the efficiencies are typically only a few percent. Moreover, conventional systems often require expensive components to manage heat flow through the system.
As a result of the low efficiency and high system cost, electricity generated by thermoelectric energy harvesting from waste heat is currently not competitive with conventional electricity generation on a dollars-per-watt basis. This realization has led researchers to not only focus on increasing TEG device efficiency limits but to devise cheaper manufacturing processes and methods. A system design constraint that has not been fully investigated is the coupling of thermal and mechanical properties in thermoelectric materials. The extent to which this coupling affects the performance of the TEGs will be studied. This thesis develops an approach for decoupling the thermal and mechanical properties and tests it through a variety of simulations. We propose a mechanically compliant attachment strategy which could be integrated in various waste heat recovery applications.
The strategy involves breaking the thermal and mechanical bond formed by the brittle thermoelectric elements and its substrate. Copper wire, which is more pliable, is then used to connect the thermoelectric element to the substrate. A system analysis was performed for waste heat recovery from a vehicles exhaust pipe. We found that utilizing the proposed strategy should not only lead to increased mechanical compliance but can also lead to cost savings on a dollars-per-watt basis. We found that 84% power retention could be obtained when up to 16x less material is used under most apparent conditions¹.
by Corey D. Christian.
S.M. in Engineering and Management
S.M.inEngineeringandManagement Massachusetts Institute of Technology, System Design and Management Program
Omer, Siddig Adam. "Solar thermoelectric system for small scale power generation." Thesis, Loughborough University, 1997. https://dspace.lboro.ac.uk/2134/7440.
Full textKarim, Nejad Aliabadi Parya. "Development of thermoelectric cooling system for tissue ablation." Thesis, University of Birmingham, 2017. http://etheses.bham.ac.uk//id/eprint/7536/.
Full textZheng, Xiaofeng. "Exploration and development of domestic thermoelectric cogeneration system." Thesis, University of Nottingham, 2013. http://eprints.nottingham.ac.uk/29922/.
Full textBorgström, Fredrik, and Jonas Coyet. "Waste heat recovery system with new thermoelectric materials." Thesis, Linköpings universitet, Mekanisk värmeteori och strömningslära, 2015. http://urn.kb.se/resolve?urn=urn:nbn:se:liu:diva-125716.
Full textYamamoto, Masahiro, Hiromichi Ohta, and Kunihito Koumoto. "Thermoelectric phase diagram in a CaTiO3- SrTiO3 - BaTiO3 system." American Institute of Physics, 2007. http://hdl.handle.net/2237/8769.
Full textKiflemariam, Robel. "Heat-Driven Self-Cooling System Based On Thermoelectric Generation Effect." FIU Digital Commons, 2015. http://digitalcommons.fiu.edu/etd/2281.
Full textUrbani, Matteo. "Characterization of thermoelectric commercial modules using a module test system." Master's thesis, Alma Mater Studiorum - Università di Bologna, 2013. http://amslaurea.unibo.it/6447/.
Full textMakki, Adham. "Innovative heat pipe-based photovoltaic/thermoelectric (PV/TEG) generation system." Thesis, University of Nottingham, 2017. http://eprints.nottingham.ac.uk/43330/.
Full textAdinolfi, Borea Riccardo. "Experimental investigation on working parameters of a Thermoelectric Generator-based system." Master's thesis, Alma Mater Studiorum - Università di Bologna, 2022. http://amslaurea.unibo.it/25506/.
Full textVerma, Darpan. "Hybrid Solar Energy System with integrated Concentration Photovoltaic Cells and Thermoelectric Devices." University of Cincinnati / OhioLINK, 2019. http://rave.ohiolink.edu/etdc/view?acc_num=ucin1553613351859182.
Full textLangham, Ryan C. "Feasibility study and system architecture of radioisotope thermoelectric generation power systems for usmc forward operating bases." Monterey California. Naval Postgraduate School, 2013. http://hdl.handle.net/10945/34695.
Full textThis study sought to identify the feasibility of utilizing a radioisotope thermal (thermoelectric/stirling) generator to provide power to a deployed USMC Expeditionary Force. The conceptual system architecture was constructed through use of the systems engineering process, identifying necessary subsystems and integration boundaries. Radioisotope comparison was then performed, utilizing weighted design factors. It was determined that Sr-90, Cs-137, and Cm-244 would be the most effective fuel sources for this mission area. By analyzing current thermoelectric technology, it was determined that maximum system efficiency is limited to 1015 percent when utilizing available lead telluride thermoelectrics. Barriers to development of identified physical subsystem components were then identified, including health and environmental hazards of potential isotopes, as well as shielding criteria. The system development was found to be feasible and additional design work and development work is proposed.
Badr, Lamya. "A Comparative Study of Cooling System Parameters in U.S. Thermoelectric Power Plants." Thesis, Virginia Tech, 2010. http://hdl.handle.net/10919/72990.
Full textMaster of Science
Hashim, Hasan. "Full-spectrum solar energy harvesting using nanotechnology-enabled photovoltaic/thermoelectric hybrid system." Thesis, Cardiff University, 2015. http://orca.cf.ac.uk/87143/.
Full textPRADERE, GUILLAUME LOUIS. "PERFORMANCE SIMULATION OF A THERMOELECTRIC PLANT PREHEATING DIESEL ENGINE SYSTEM VIA SOLAR ENERGY." PONTIFÍCIA UNIVERSIDADE CATÓLICA DO RIO DE JANEIRO, 2017. http://www.maxwell.vrac.puc-rio.br/Busca_etds.php?strSecao=resultado&nrSeq=31824@1.
Full textCOORDENAÇÃO DE APERFEIÇOAMENTO DO PESSOAL DE ENSINO SUPERIOR
PROGRAMA DE EXCELENCIA ACADEMICA
Este trabalho tem por objetivo principal a avaliação de desempenho de um sistema piloto de preaquecimento dos motores da central termelétrica Gera Maranhão, via energia solar térmica, em Miranda do Norte, Maranhão, através de uma simulação numérica. Cinco subsistemas independentes, cada um responsável pelo preaquecimento de um motor Wartsila 20V32 de 8,73 MW, foram construídos, somando um total de 500 coletores solares instalados e uma superfície de captação solar total de 1000 metros quadrados. Uma estação meteorológica com sensores de radiação solar global, difusa, direta e temperatura ambiente foi posicionada do lado dos sistemas para medir as condições ambientais na região. A simulação do desempenho do sistema solar foi efetuada ao longo de um ano com dados de radiação solar da estação meteorológica de Buriticupu, no Maranhão, dados que mais se aproximam dos dados disponíveis de Miranda do Norte. Correlações para transformar a radiação global medida numa superfície horizontal para uma superfície inclinada foram selecionadas após uma revisão bibliográfica dentre as disponíveis na literatura. Diferentes cenários de controle do acionamento das bombas de água foram comparados a fim de determinar a melhor configuração de operação. A influência da temperatura de preaquecimento dos motores no desempenho do sistema solar foi avaliada também. Os resultados da simulação foram comparados com os resultados obtidos via o método F-CHART. Uma participação média anual da energia solar de 11,5 por cento foi encontrada para o preaquecimento dos motores levando a uma redução de 24693 kg/ano de óleo combustível usado na caldeira do sistema de preaquecimento dos motores da usina termelétrica.
The present work has as main objective the performance evaluation of a pilot system for preheating the engines of Gera Maranhão power plant, in Miranda do Norte, state of Maranhão, via thermal solar energy using a numerical simulation. Five independent subsystems, each one responsible for the preheating of a Wartsila 20V32 internal combustion engine of 8.73 MW, were installed. These systems amount five hundred solar collectors, with a total solar collecting area of 1000 square meters. A meteorological station with sensors for global, diffusive and beam solar radiation, as well as ambient temperature recorders, was placed by the side of the system in mode to measure ambient condition in the area. The simulation of the solar system performance was processed over a year with data of solar radiation for a meteorological station of Buriticupu, state of Maranhão, Brazil. Correlations to transform the global radiation measured on a horizontal plane to a sloped plane were selected, following a selection from a literature review. For the control of the water pumps, different scenarios were compared in order to determine the best operational configuration. The influence of engine preheating temperature in the performance of the solar system was also evaluated. Simulation results were compared with results obtained with the F-CHART method. An annual average solar energy contribution of 11.5 percent was found for the preheating of the engines. This resulted in a reduction of 24693 kg per year of fuel oil used in the boiler of the traditional preheating system of the power plant.
Schriefer, Timothy. "The viability of a thermoelectric fuel conditioning system for a diesel engine utilizing biodiesel /." Online version of thesis, 2008. http://hdl.handle.net/1850/7508.
Full textTaylor, Stephen H. "Analytical Modeling and Optimization of a Thermoelectric Heat Conversion System Operating Betweeen Fluid Streams." BYU ScholarsArchive, 2011. https://scholarsarchive.byu.edu/etd/2813.
Full textMativo, John M. "System Design of Composite Thermoelectrics for Aircraft Energy Harvesting." University of Dayton / OhioLINK, 2020. http://rave.ohiolink.edu/etdc/view?acc_num=dayton1607959975788155.
Full textSchoenfeld, Jonathan Michael. "Integration of a thermoelectric subcooler into a carbon dioxide transcritical vapor compression cycle refrigeration system." College Park, Md.: University of Maryland, 2008. http://hdl.handle.net/1903/8726.
Full textThesis research directed by: Dept. of Mechanical Engineering. Title from t.p. of PDF. Includes bibliographical references. Published by UMI Dissertation Services, Ann Arbor, Mich. Also available in paper.
Chen, Jie. "Design and analysis of a thermoelectric energy harvesting system for powering sensing nodes in nuclear power plant." Thesis, Virginia Tech, 2016. http://hdl.handle.net/10919/64792.
Full textMaster of Science
Palu, Ivo. "Impact of wind parks on power system containing thermal power plants = Tuuleparkide mõju soojuselektrijaamadega energiasüsteemile /." Tallinn : TUI Press, 2009. http://digi.lib.ttu.ee/i/?443.
Full textSklar, Akiva A. "A Numerical Investigation of a Thermodielectric Power Generation System." Diss., Georgia Institute of Technology, 2005. http://hdl.handle.net/1853/14020.
Full textBörner, Floriana-Dana, Max Schreier, Bing Feng, Wolfgang Lippmann, Hans-Peter Martin, Alexander Michaelis, and Antonio Hurtado. "Development of laser-based joining technology for the fabrication of ceramic thermoelectric modules." Cambridge University Press, 2014. https://tud.qucosa.de/id/qucosa%3A39033.
Full textMilani, Dia. "Modelling framework of solar assisted dehumidification system to generate freshwater from "Thin air"." Thesis, The University of Sydney, 2012. http://hdl.handle.net/2123/13581.
Full textNamakian, Mohsen. "Mild Hybrid System in Combination with Waste Heat Recovery for Commercial Vehicles." Thesis, Linköpings universitet, Maskinkonstruktion, 2013. http://urn.kb.se/resolve?urn=urn:nbn:se:liu:diva-93997.
Full textPandit, Jaideep. "Numerical and Experimental Design of High Performance Heat Exchanger System for A Thermoelectric Power Generator for Implementation in Automobile Exhaust Gas Waste Heat Recovery." Diss., Virginia Tech, 2014. http://hdl.handle.net/10919/47919.
Full textPh. D.
Choi, Sung In. "Smart Localized Heating Control System With Human Movement Tracking." Master's thesis, Temple University Libraries, 2016. http://cdm16002.contentdm.oclc.org/cdm/ref/collection/p245801coll10/id/407171.
Full textM.S.E.E.
According to the U.S. energy consumption survey in 2012, about 25% of the commercial and 42% of the residential building energy were used for heating. Despite the development of new and more efficient Heating, Ventilation, and Air Conditioning (HVAC) systems over the years, the high energy consumption in heating is still one of the major energy efficiency issues. Studies showed that decreasing HVAC operating temperature set points by 4°F will result in energy savings of 15% or more. Thus, the smart localized heating control (SLHC) system was designed and prototyped to provide localized heat directly to a person so that HVAC can run at a lower temperature set point. SLHC detects human movement and delivers the heat based on the result of the target location estimation and temperature measurement feedback. To detect the human movement, image processing techniques were used; image segmentation, mass center detection, background subtraction using the Mixture of Gaussian model, and human feature detection. In SLHC, a near-infrared heater and a tracking function were used to provide an instant and a direct heat to the person in order to minimize wasting energy. The SLHC system is divided into the sensing and processing (SP) and the heating and regulating (HR) subsystem. The SP’s primary function is to process captured video images and measured temperature data. SP also generates and sends the heater operating signal to HR. HR purposes to control the heater’s direction and power based on the signal. The communication between SP and HR was established through Wi-Fi enabled development platform. The SLHC prototype successfully processed the sensing data and transmitted the control signal. The result shows that it detected human movement and estimated the person’s location in 3D space within 10% margin of error. Also, it delivered the focused heat to the surface of the human body and increased the temperature by 10.0°F in 3 minutes at the distance of 1.5m away from the heater. This cost-effective, wireless, and localized heating system demonstrates the potential to improve energy efficiency in buildings.
Temple University--Theses
Tang, Ming Y. 1979. "Characterization and modeling of nanocomposite thermoelectric materials system bismuth antimony telluride ((Biy̳Sb1̳-̳y̳)2̳Te3̳) as a function of temperature and magnetic field." Thesis, Massachusetts Institute of Technology, 2011. http://hdl.handle.net/1721.1/68496.
Full textCataloged from PDF version of thesis. In title ((Biy̳Sb1̳-̳y̳)2̳Te3̳) on title page, double-underscored characters appear as subscript.
Includes bibliographical references (p. 185-188).
This thesis looks at (BiySb1-y)2Te3 nanocomposites as an example of the currently available nano systems. In this thesis, (BiySb-y)2Te3 nanocomposites are characterized from ~325K down to ~3K. Advantages of this low temperature regime include the minimization of lattice vibrations and the decreasing of ke with decreasing temperature. As a result, nano effects on IL could be better observed and characterized in this low temperature regime. We are also interested in studying the effect of an applied magnetic field on the conduction carriers in this low temperature regime. We like to find out whether an applied magnetic field could impede the carriers' heat conducting ability more than their current conducting ability. Therefore, a magnetic field effect study is also carried out to see whether any improvement in ZT could be achieved by the applying of a magnetic field. The measurement system used in this thesis is QD PPMS. Only the ACT and TTO options of the QD PPMS apparatus are used for measurements in this thesis. Under the ACT option, Hall and 4-pt p measurements on the same sample are performed. On the other hand, Kti, S, and 2-pt p measurements are performed simultaneously on the same sample under the TTO option. Both the ACT and TTO options use an AC current instead of a DC current during p measurement to eliminate any unwanted Seebeck voltage. Since the ability to perform correct measurements on thermoelectric samples is not a trivial task, benchmarking with known results is a must. In this thesis, I calibrate our QD PPMS against both the manufacturer's results and the published data, and demonstrate that our measurement system gives accurate results. I also benchmark our nt, results under a magnetic field using a pyrex sample. Our results confirm that the QD PPMS apparatus does not introduce artifacts under an applied magnetic field. Thus, any changes observed under the QD PPMS apparatus measurements in an applied magnetic field would be expected to be solely due to the sample. Lastly, no measurable difference is found between our 2-pt p (TTO) and 4-pt p (ACT) measurements. A total of eight (BiySb1-y) 2Te3 samples are measured in this thesis. The sample set includes: (a) one bulk ingot sample manufactured by Marlow (Ingot), (b) four nanocomposite samples (XY21, XY146, XY144, and GJ99) made by collaborators from Boston College (BC) where the letters simply indicate the sample maker's initials, and (c) three nanocomposite samples (0%, 40%, and 100%) made by collaborators from Nanyang Technological University (NTU) in Singapore, where the % denotes the weight % of the nanoinclusions prepared via melt spinning [1] in the sample. All the nanocomposite samples in this thesis are made solely for research uses and are purposely fabricated under conditions different than those used for the best samples previously reported [2, 1]. Although BC and NTU use different starting materials, different fabrication machines, and different fabrication parameters, the resulting densities of the nanocomposites from the ball-milled nanopowders alone (XY21, XY146, XY144, GJ99, and 0%) are almost identical. Moreover, the addition of nanoinclusions prepared via melt spinning decreases the sample mass density somewhat.
(cont.) From the XRD measurement results, we notice that (a) both the NTU and BC samples have the same XRD peak locations, (b) the NTU samples have a lower intensity for peaks (1 0 10) and (1 1 0), and (c) the NTU samples have a higher intensity for peaks (0 0 g) where g is an integer. Comparing the XRD patterns with the reference database, the difference in peak intensities is a good indication that the NTU samples are not completely randomized and have internal preferred orientations. From the SEM images, we notice that the NTU samples and the BC samples are markedly different. For example, the BC samples are shown to have grains in the pm range with a small grain size distribution. On the other hand, the grain sizes of the NTU samples decreases with the addition of nanoinclusions prepared via melt spinning. Moreover, the NTU samples have a wider grain size distribution that ranges from nm to pum. This observed difference is believed to arise from the difference in the fabrication techniques used by the BC and NTJ teams. Temperature-dependent hta, S, and p measurements, along with the carrier concentration measurements, are performed on all samples. All samples are found to be p-type materials. Transport measurements are performed both // and I to the press direction for the nanocomposite samples, and only // to the growth direction for the Ingot sample. Anisotropic behavior is observed in ~tha nd p for all the nanocomposite samples investigated, with the anisotropy being always higher in p than in th . On the other hand, S is found to be isotropic. Thus, care needs be taken during the fabrication process to ensure that no unwanted anisotropic behavior is introduced. Common p and S features among all samples include: (a) a dramatic decrease in the peak value of sth for the nanocomposite samples when compared with the Ingot //'s value, (b) constant slope &S/&T for T < 20K, (c) constant slope &S/ln(T) of ~ 130-140pV/ln(K) for 200K < T < 300K, (d) close-to-zero slope in p for T < 20K, and (e) p cx T'.1 0 for 200K < T < 300K. From the measured stl, S, and p data, the mobility pp, hole mean free path e, and phonon mean free path Eph are computed. It is found that nanocomposite approach decreases lp, fe, and Eph. Moreover, the pp, fe, and E values are always lower in the // direction for the nanocomposite samples than in the I direction. Furthermore, 4e in general is in the nm range while eph ranges from pm to nmn as the temperature increases. Therefore, if one wants to decrease the sl,, a possible solution is to decrease f further. However, in order not to affect the p too much, the lower limit for f should be in the nm range. As a result, decreasing f would have the biggest effect on Kth in the low temperature regime. Using the Kth and - data, KL is extracted through the intercept method (see Section 3.5.3). This method only makes sense if all the samples have similar f. Since pressure is coining from top and bottom during the fabrication process for the nanocomposite samples, my samples are expected not to behave as the same materials system along the // direction. However, for the I direction, they can be considered as a same materials system since no pressure is applied. The 40% and 100% samples are believed to deviate from the results for the 0% sample because of the presence of nanoinclusions in them. rlLL is found to be 0.76W/mn-K for the 40% sample at 297K. When I compare this value with previously determined values for Bi 2Te3 (1.4W/in-K [3]) and (Bio.3Sbo. 7)2Te3 (0.9W/m-K [4]) alloy at 300K, these results confirm that the nanocomposite approach does indeed lower the lattice thermal conductivity. The semi-classical model is then used to interpret the various transport coefficients (o- = 1/p, S, and t;e) and is based on the Boltzmann Transport Equation (BTE) under the relaxation time approximation (RTA). Acoustic phonon scattering, ionized impurity atom scattering, neutral impurity atom scattering, alloy scattering for a 3-atom II"_1II system, point defect scattering, grain boundary scattering, and polar optical phonon scattering are considered for the electrons. On the other hand, boundary scattering, point defect / alloy scattering, and Umklapp scattering are considered for the phonons. We find that for holes, point defect scattering dominates at low T, while acoustic phonon scattering dominates around 300K. As for phonons, boundary and point defect scattering mechanisms dominate at low T, while point defect and Umklapp scattering mechanisms dominate at high T (~300K). We also find that the nano approach increases the crossover temperature Tcross. For the electron model, we observe that the deformation potential (DA) seems to be both process dependent and materials dependent. We see that DA changes from the BC samples to the NTU samples (process dependent). Moreover, DA changes in the NTU samples when going from 0% to 100% (materials dependent). From the electron model, the ionized impurity atom concentration Ni and the neutral impurity atom concentration No reflect the somewhat anisotropic behavior of all the samples investigated. Lastly, f seems to play little role in the determination of p. For the phonon model, we observe that C plays a rather important role in the determination of r1L, especially at low temperatures. The value of C seems to be consistently lower for the BC samples than for the NTU sample (0%) for the nanocomposite samples made solely from ball-milled nanoparticles. We also see that the Umklapp scattering contribution (B') has a materials dependent factor, where B' decreases from 10x101'8s/K for the nanoparticle nanocomposite samples to e 4x1018 s/K for (cont.) the nanocomposite sample made using 100% nanoinclusions prepared via melt spinning.
Furthermore, we see that the point defect contribution (A') reaches the highest value when both the nanoparticles and nanoinclusions prepared via melt spinning are present in the nanocomposite samples (e.g. the 40% sample), similar to the alloying effect on the thermal conductivity. In general, it is desirable to increase the values of A' and B', resulting in a decrease in the KL values. However, care needs to be taken to ensure that the phonon parameters are independent of the electron parameters so that no adverse effect on ZT would result. The determination of L is also carried out based on my electron model findings. We observe that L is isotropic. Moreover, L for each sample investigated reaches the same value of 2.44x10-8 W-Ohm/K2 as T -> OK (completely degenerate limit of (+_ )2). Furthermore, the higher the hole concentration the sample has, the higher its C value is at a given temperature. Lastly, I find that a lower f leads to higher ZT values at 297K for the BC nanocomposite samples measured in the _L direction. On the other hand, a lower f leads to lower ZT values at 297K for the NTU nanocomposite samples measured in both the // and _L directions. From the magnetic field studies on the Ingot and on the 40% samples, few important facts are demonstrated. First, an applied magnetic field can be used to effectively increase the ZT of (BiySbpy)2Te3 , especially at temperatures below 200K. Use of a magnetic field might theoretically extend the effective temperature ranges over which (BiySb-y)2Te3 materials can be used for refrigeration. Second, the data under various applied B fields allow me to confidently calculate the C value below the temperature ranges where a plateau has occurred. Third, the data under various applied B fields serve as an important guideline for both validating any electron model and extrapolating values for L above the plateau occurrence temperatures. As a result, this allows me to get some insights into the temperature dependence of L (see Figure 4-14). Fourth, from the magnetic field dependent transport studies on our samples, we observe that the applied B field pushes away the holes more effectively in the Ingot // than the holes in the nanocomposite samples. We also find that the VvtIplateau values obtained under the magnetic field study serve as a more realistic and practical limit for KL. Lastly, from the magnetic field-dependent studies, we find that having point defects as the dominant scattering mechanism for the carriers results in an increase in ZT under an applied magnetic field. It would be extremely useful if one can make a sample such that the point defect dominant regime is extended to higher temperatures, resulting in a shift of the increase in the ZT ratio regime to a temperature range closer to room temperature (300K). However, care needs to be taken to ensure that such modifications would result in an increase in the ZT values under an applied magnetic field.
by Ming Y. Tang.
Ph.D.
Jarumongkonsak, Pornput. "Development and performance investigation on solar-powered thermoelectric radiant cooling in building-integrated system for a bedroom under hot and humid climate." Thesis, University of Nottingham, 2016. http://eprints.nottingham.ac.uk/33629/.
Full textJain, Akshay. "Feasibility of using Waste Heat as a power source to operate Microbial Electrolysis Cells towards Resource Recovery." Diss., Virginia Tech, 2020. http://hdl.handle.net/10919/97977.
Full textDoctor of Philosophy
An average person produces about 50-75 gallons of wastewater every day. In addition to the households, wastewater is generated from industries and agricultural practices. As the population increases, the quantity of wastewater production will inevitably increase. To keep our rivers and oceans clean and safe, it is essential to treat the wastewater before it is discharged to the water bodies. However, the conventional wastewater treatment is a very energy (and thus cost) intensive process. For low-income and developing parts of the world, it is difficult to adapt the technology everywhere in its present form. Furthermore, as the energy is provided mostly by fossil fuels, their limited reserves and harmful environmental effects make it critical to find alternative methods that can treat the wastewater at a much lower energy input. For a circular and sustainable economy, it is important to realize wastewater as a resource which can provide us energy, nutrients, and water, rather than discard it as a waste. Bioelectrochemical systems (BES) is an emerging technology that can simultaneously treat wastewater and recover resources in the form of electricity/hydrogen gas, and nitrogen and phosphorus compounds. Microbial electrolysis cell (MEC) is a type of BES that is used to treat wastewater and generate hydrogen gas. An additional voltage is supplied to the MEC for producing hydrogen. In the long run, this may not be sustainable as it relies on fossil fuels to provide that additional energy. Thus, it is important to explore alternative renewable resources that can provide energy to power MEC. Waste heat is a byproduct of many industrial processes and widely available. This was utilized as a renewable resource by converting waste heat to electricity using a device called thermoelectric generator (TEG). TEG converted simulated waste heat from an anaerobic digester to power an MEC. The mutual benefit for MEC and TEG was also explored by connecting the system electrically and hydraulically. Cost-estimation of the system was performed to understand the economic viability and functions of the system were developed. The present system provides a sustainable method for wastewater treatment and resource recovery which can play an important role in human health, social and economic development and a strong ecosystem.
Landis, Adam. "Optimization of a paraffin cooling system for an automated tissue embedding center." Ohio : Ohio University, 2004. http://www.ohiolink.edu/etd/view.cgi?ohiou1177528419.
Full textLiu, Shuhao. "Electronic Transport in Functional Materials and Two-Dimensional Hole System." Case Western Reserve University School of Graduate Studies / OhioLINK, 2018. http://rave.ohiolink.edu/etdc/view?acc_num=case1522893320666086.
Full textKim, Sunphil. "P-type thermoelectric materials for waste heat recovery system: P-type Mg2Sn1-xSix and Pb1-x-yEuxSe:Nay." The Ohio State University, 2014. http://rave.ohiolink.edu/etdc/view?acc_num=osu1405345044.
Full textSettaluri, Krishna Tej. "Body powered thermoelectric systems." Thesis, Massachusetts Institute of Technology, 2012. http://hdl.handle.net/1721.1/76819.
Full textThis electronic version was submitted by the student author. The certified thesis is available in the Institute Archives and Special Collections.
Cataloged from student-submitted PDF version of thesis.
Includes bibliographical references (p. 107-111).
Great interest exists for and progress has be made in the effective utilization of the human body as a possible power supply in hopes of powering such applications as sensors and continuously monitoring medical devices [1]. This report furthers into the area of thermal energy harvesting, which focuses on using the temperature differential generated between the human body and the ambient environment to generate power. More specifically, a body-powered, thermoelectric-based power supply and system will be introduced and examined, with hopes that this technology will be utilized alongside low-power, medical monitoring applications in order to achieve self-sufficiency. This report also analyzes the performance of existing thermoelectric-based body-powered energy harvesting applications and compares that with the new design introduced in this work. The new designs were able to output upwards of 25[mu]W/cm2 or, equivalently, 280µW for the entire heat sink system. Additionally, this report details the physics associated with thermoelectric modules, addresses the issues with modern thermoelectric heat-sinks, introduces two new types of wearable, conformal heat sinks, quantifies the performance of the body-powered thermoelectric supply, tests a flexible EKG processing board, and analyzes future paths for this project.
by Krishna Tej Settaluri.
M.Eng.
Smith, Kevin D. "An investigation into the viability of heat sources for thermoelectric power generation systems /." Online version of thesis, 2009. http://hdl.handle.net/1850/8266.
Full textSchlenker, Aaron Paul. "Integrated optimization of thermoelectric systems." Thesis, Massachusetts Institute of Technology, 2020. https://hdl.handle.net/1721.1/127119.
Full textCataloged from the official PDF of thesis.
Includes bibliographical references (pages 99-103).
Thermoelectric devices present unique opportunities for sustainable energy conversion. While research efforts have remarkably improved material capabilities over the past several decades, material advancement alone is insufficient to realize the full potential of thermoelectric technology [25, 24, 39, 14]. Here, an integrated perspective is applied to thermoelectric technology to identify potential system improvements. The traditional thermoelectric architecture is dissected to identify limitations. It is found that the coupling of the device height to the thermoelectric element height imposed by the architecture can significantly hinder performance. A novel distributed architecture, which de-couples the device and element heights, is theorized to address these limitations. A modeling program incorporating device parameters and external conditions is developed to simulate and optimize the system architecture. The new architecture is shown to out-perform the traditional architecture in both a broad range of general generation and refrigeration conditions and the specific application of a phase-change material thermoelectric generator. The results signal the importance and potential value of an integrated approach to thermoelectric system design.
by Aaron Paul Schlenker.
S.M.
S.M. Massachusetts Institute of Technology, Department of Mechanical Engineering
Chin, Chi-Jen, and 秦志仁. "Design and Amplication of Thermoelectric Cooler System." Thesis, 1994. http://ndltd.ncl.edu.tw/handle/70412126707241355439.
Full text國立臺灣大學
機械工程研究所
82
The purpose of present study is to develop the design technique thermoelectric cooler system.The present study provides the optimal design analysis and establishes a design tool to manufacture the thermoelectric cooler system. In order to investigate the characteristics of thermoelectric module, the auto-measurement performance equipment has been set up. The characteristic equation derived from measured data can serve as the fundemental of developing system analysis with comparing the experimental testification of present module and the pratical application of cooling linear compressor ,the results are quite satisfatory both in direction of precision and practicality.
Xiao, Sheng-Xue, and 蕭聖學. "Thermoelectric Properties in Multiple Quantum Dot System." Thesis, 2010. http://ndltd.ncl.edu.tw/handle/31787145723783230112.
Full text國立中央大學
電機工程研究所
98
The electrical conductance, thermal conductance, thermal power and figure of merit (ZT) of semiconductor quantum dots (QDs) embedded into an insulator matrix connected with metallic electrodes are theoretically investigated in the Coulomb blockade regime. The multilevel Anderson model is used to simulate the multiple QDs junction system. The charge and heat currents in the sequential tunneling process are calculated by the Keldysh Green function technique. In the linear response regime the ZT values are still very impressive in the small tunneling rates case, although the effect of electron Coulomb interaction on ZT is significant.
Yang, Bo-Jiun, and 楊柏俊. "Study of Thermoelectric Material Appliedto Geothermal System." Thesis, 2016. http://ndltd.ncl.edu.tw/handle/52211420368530277627.
Full text國立臺灣大學
機械工程學研究所
104
In recent years, the problem of shortage of energy is growing up, therefore, waste heat recovery have become a very important issue. And the thermoelectric material plays an important role in this issue. A geothermal plant, since the heat is lost in the pipeline, we can use the thermoelectric material to recover the waste heat, and utilize dissipated heat as a stable heat source. The aim of this study is to simulate the situation of the waste heat recovery with the geothermal module. In this thesis, the experiment and simulation are discussed. In the experiment, we investigate the case of waste heat recovery with single thermoelectric generator, followed by the geothermal module. In the simulation, we simulated the single thermoelectric generator by the Thermoelectric module in the Ansys Workbench, followed by the geothermal module which was simulated by the Fluent and the Thermoelectric module in the Ansys Workbench. Finally, we compared and discussed the experimental and simulated data. The result shows that the thermoelectric generator TEG616-6 provided by ITRI is a high-performance thermoelectric generator,. The open circuit voltage, output power, and the internal resistance of the thermoelectric generator all increase with the elevating temperature of the high-temperature side,. When the high-temperature side was at 200℃,and the low temperature side was at 30℃, the output power can reach 5.42W, the power density was 3387.5W⁄m^2 , and the efficiency was about 5%. In terms of geothermal module, when the hot water side was at 90 ℃, and the cold water side was at 25℃, the output power can reach 2.6529W, and the power density was 414.515W⁄m^2 ,. In the simulation of the single thermoelectric generator, according to the verification process,the electrical resistivity can be predict by the first order regression analysis with intermetallic layer modification,. The seebeck coefficient and thermal conductivity can be predict by the secondary order regression analysis. In the simulation of the geothermal module, we utilized the turbulence model and the steady energy model to approach the practical situation. After comparing the experimental data with the simulated data, it shows the error is very small. In the end of the thesis, we can predict the performance of the geothermal module with the hot water temperature exceeding 100℃,. The simulation result shows that when the hot water side was at 100℃, 125℃, 150℃, 175℃ and 200℃as well as the cold water side was at 25℃, the maximum output power can reach 3.68W,5.55W, 8.68W, 13.92W and 18.66W.
Chang, Shun-Pin, and 張舜品. "Thermoelectric Conversion System with Dimmable LED Lighting." Thesis, 2015. http://ndltd.ncl.edu.tw/handle/8xzd4q.
Full text國立臺北科技大學
電機工程系所
103
In this thesis, a step-up converter is presented, which possesses a high voltage gain, continuous input current and galvanic isolation. After this, the proposed converter is applied to a thermoelectric conversion system along with stable tracking based on three-point-weighting method, so as to upgrade output power of the thermoelectric module. For LED dimming to be considered, a switched LED module is used to adjust the number of LEDs in the LED string so as to achieve a dimmable function. Moreover, a field programmable gate array (FPGA) chip, named EP1C3T100C8N made by Altera Co., is used as a control kernel, so as to realize the maximum power tracking and LED dimming. Finally, several thermoelectric modules, manufactured by Kryotherm Co., are used to verify the effectiveness of the proposed electric thermoelectric conversion system.
Tsai, Rung-Je, and 蔡榮哲. "Optmal Design and Control of ThermoElectric Generator System." Thesis, 2010. http://ndltd.ncl.edu.tw/handle/35614315215824472415.
Full text臺灣大學
機械工程學研究所
98
This thesis aims to design-ThermoElectric Generator System. The ThermoElectric Generator System generates power by temperature difference. The hot side uses a heater to simulate exhaust heat. The cooling side is particularly designed utilizing the passive heat sink tech, Loop Heat Pipe. As a result, the system achieves the goal of electricity generation. The study discusses the Maximum Power Point Trick controller in order to maintain the maximum power exportation. Then, the final step is about to research the design of ThermoElectric Generator System with near Maximum Power Point Operation (nMPPO), According to testing result of the study, As long as the temperature of hot side of ThermoElectric Generator System(TEGS) stays within 150℃~210℃, the transformative efficiency of nMPPO will higher than the one of MPPT. Finally, the study analyses the proper usage of the MPPT and the nMPPO. First, the usage of MPPT is suitable for using when the temperature range of hot side is higher than 150℃~210℃. In addition, the MPPT is not affected by systematic ageing effect. It can be used for a long time. Second, the usage of nMPPO is suitably used when the hot side is within 150℃~210℃. Moreover, the time which it is able to be used is much shorter.
Chien, Po-yin, and 簡伯因. "Polarity effect in SAC305/bismuth telluride thermoelectric system." Thesis, 2013. http://ndltd.ncl.edu.tw/handle/70298615362664772284.
Full text國立中央大學
化學工程與材料工程學系
101
This study investigates electromigration in Bi2Te3 thermoelectric (TE) material systems and the effectiveness of the diffusion barrier under current. The influences of the interfacial reaction by electromigration and Peltier effect were decoupled in this research. n- and p-type Bi2Te3 were connected to SAC305 solders and different current densities at various temperatures were applied. The Bi2Te3 samples were fabricated by the Spark Plasma Sintering (SPS) technique and electroless Ni-P was deposited at the solder/TE interfaces. The results elucidate the importance of the Ni diffusion barrier to the joint reliability. Different intermetallic compound (IMC) layers including (Cu, Ni)6Sn5 and NiTe formed at solder/Ni-P and Ni-P/substrate interfaces, respectively. The results show that the mechanism of compound growth was dominated by electromigration at low current density and dominated by Peltier effect at high current density.
KO, HUNG-PIN, and 柯鴻彬. "Using Thermoelectric Cooling Module to Dish Dryer System." Thesis, 2013. http://ndltd.ncl.edu.tw/handle/9g7h3b.
Full text國立虎尾科技大學
光電與材料科技研究所
101
This thesis indicates those based on the current household dish dryer in the market and modify it. We change its heater from current general circuit heater to thermoelectric cooling module heat surface. We discuss the possibilities to apply thermoelectric cooling module on the dish dryer. This experiment is that we use single TEC1-12706 thermoelectric cooling module and two pieces of thermoelectric cooling modules as heat source, and assist with a cross flow fan as adjustment the direction of air flow out, which makes the dish dryer air flow circulation smoothly, and has well-distributed effect. According to the experiment data, 2 pieces of thermoelectric cooling modules do not have better dryer performance than single thermoelectric cooling module. If it requests better dryer speed, it requires thermoelectric cooling module with higher watt. In half-closed space, adjusting the angle of air flow out of cross flow fan cannot make the dryer speed quicker, but it can maintain the temperature in the space averagely. Hot air recycle system can make hot air to re-use and recycle again which makes the temperature of the space to keep in a certain range. It does not have impact on the dryer efficiency due to heat spreading which causes temperature continuously going down.
吳欣潔. "Phase equilibria, microstructures and thermoelectric properties of the quaternary Pb-Ag-Sb-Te thermoelectric material system." Thesis, 2012. http://ndltd.ncl.edu.tw/handle/01320463603103743597.
Full text國立清華大學
化學工程學系
101
Thermoelectric material has been recognized as a promising candidate in the application of sustainable energy. The quaternary Pb-Ag-Sb-Te system has attracted much attention because it contains high-zT AgPb18SbTe20 (zT>2 at 800K), PbTe and AgSbTe2. The phase stability, microstructural evolution and resultant electrical/thermal transport properties of quaternary Pb-Ag-Sb-Te and the constituent systems (Ag-Sb-Te, Pb-Sb-Te and Ag-Pb-Te) are investigated. The liquidus projections of both ternary Ag-Pb-Te and Pb-Sb-Te systems are constructed. In particular, the Ag-Pb-Te ternary-eutectic alloy, with composition of Ag-4.3at%Pb-62.6at%Te, forms a partially aligned nano-sized lamellar microstructure, which comprises both the PbTe and Ag5Te3 phases, and an additional dotted PbTe of 200-600nm. This particular ternary-eutectic alloy is unidirectionally solidified using the Bridgman method, resulted in a nanostructured composite with an extremely low thermal conductivity(κ) of 0.3 W/mK and a zT peak of 0.41 at 400K. The phase diagrams of ternary Ag-Sb-Te system are constructed as well, including the 400℃ and 250℃ isothermal sections and the liquidus projection. The ternary AgSbTe2 is stabilized at 400℃ but not at 250℃, with homogeneity region of 49.0-53.0at%Te and 28.0-30.0at%Sb. The nano-scaled microstrucutre and crystal structures of the non-stoimeteric AgSbTe2 are analyzed by the transmission electron microscope (TEM). In particular, an ordered array of nano-wire microstructure, comprising a 200nm Ag2Te and a matrix of AgSbTe2+δ-Sb2Te, was resulted from a Class I reaction: L=AgSbTe2+Ag2Te+δ-Sb2Te with liquid composition of Ag-40at%Sb-36.0at%Te at 496.5℃. To understand and guide production of uniform bulk samples of this composite, the liquidus projection of quaternary Pb-Ag-Sb-Te system at 36.0at%Te isoplethal section is constructed experimentally using quenched samples. High-resolution transmission electron microscopy (TEM) confirms that these three phases are simultaneously present at the nanometer scale. Furthermore, unidirectional solidification experiments of the ternary eutectic alloy using the Bridgman method are carried out to examine the alloy's solidification behaviors. Pb-alloyed AgSbTe2 (PbxAg20Sb30-xTe50, x=3,4,5 and 6) are also unidirectionally solidified using the modified Bridgman method. The as-solidified 5at%Pb and 6at%Pb alloys, which exhibit high phase purity of AgSbTe2, contain grain-boundary inhomogeneity and nano-precipitates of δ-Sb2Te, leading to an extremely low thermal conductivity (κ) of 0.3-0.4 W/mK. A peak zT of 0.7-0.8 is found in as-solidified 5at% specimen at 425K. However, after annealing at 673K, the zT peak of 5at%Pb(annealed) decreases to 0.4, presumably due to increase in grain size and decrease in inhomogeneity.
Cheng, Yi-Hsiang, and 鄭憶湘. "Optimization Study of Thermoelectric Energy System through Genetic Algorithms." Thesis, 2007. http://ndltd.ncl.edu.tw/handle/53164723813308663757.
Full text國立清華大學
工程與系統科學系
95
This work presented a novel method based on genetic algorithms (GAs) to optimize thermoelectric energy systems. The objective of the optimization is on maximizing the cooling capacity or maximizing the coefficient of performance (COP) of thermoelectric cooling (TEC) systems. Two kinds of arrangements, including single- and two-stage TEC systems, have been studied. While optimizing a single-stage TEC system, structural parameters – including the thermocouple length, the thermocouple cross-section area and the number of thermocouple – were taken as the variables. While optimizing a two-stage TEC system, parameters – including the applied electrical current, the thermocouple length, the thermocouple cross-section area and the number of thermocouples – were considered. Two-stage TEC systems can be further categorized into three types, which are with two stages electrically connected in parallel, in series and in separate. A new mathematical modelling was also proposed to deal with the temperature-dependent material properties and to include the effects of contact and spreading thermal resistances between the two stages. For both single- and two-stage TEC systems, this study developed the design flowchart and programs that combine the mathematical modelling with GAs’ technique. All kinds of design constraints–space constraints and all others–can be considered and modeled during the optimization. The results indicate that the cooling capacity or COP can be increased by optimizing the parameters of TEC systems. This study also demonstrates that the new approach based on GAs can be used effectively to optimize the thermoelectric energy systems, and this method exhibits highly potential in handling complex design problems.
Lin, Ching-Po, and 林敬博. "Investigation of Biomass Multifuel Gasifier with a Thermoelectric System." Thesis, 2015. http://ndltd.ncl.edu.tw/handle/7cng6d.
Full text國立臺灣大學
機械工程學研究所
105
The aim of this study is to investigate the use of waste heat that is recovered from a multifuel biomass (Japanese cedar and rice husk) gasifier. In the gasification process, the low heating value of the biomass can be transferred to a high heating value for combustible gaseous fuel, which is a form that is widely used in industry and power plants. Conventionally, some cleaning processes must be conducted under higher operating temperatures than the low temperatures typically used to burn biomass. Thus, a catalytic reactor was designed before installing the scrubber in the downdraft gasifier system to effectively utilize the waste heat. The experimental results show that the temperature of the gasifier outlet is approximately 250-400℃; dolomite is used for tar removal in the catalytic reactor. To further improve the use of waste heat, a thermoelectric generator is added to recover waste heat. The thermoelectric generator system is manufactured using a Bi2Te3-based material and is composed of eight thermoelectric modules on the surface of the catalytic reactor. The measured surface temperature of the catalytic reactor is 100-250℃, which is the correct temperature for using Bi2Te3 as a thermoelectric generator. The results of this study show that the maximum hydrogen concentration is approximately 17.82vol% from pure Japanese cedar gasification and approximately 15.89vol% from pure rice husk gasification. The optimal operation of the gasification performance was found when the fuel is pure Japanese cedar at Φ = 0.4, and the obtained cold gas efficiency (CGE) at these conditions is approximately 63.59%. However, the optimal available biogas condition was found when 50% Japanese cedar and rice husk are mixed at Φ = 0.2, with a biogas high heating value (HHV) of approximately 5.75 MJ/m3. The performance of the thermoelectric generation system (TEG) that is used for waste heat recovery shows that the maximum power output of the thermoelectric generator system is 5.8 W and that the thermoelectric generator power density is approximately 180.6 W/m2. In this study, the total efficiency of a multifuel gasifier with a waste heat recovery system from thermoelectric generation modules was also investigated. The maximum exergetic efficiencies for 100% and 75% Japanese cedar are 55.46% and 54.49%, respectively. As the rice husk ratio increased, the maximum exergetic efficiency decreased to 44.2%~46.7%.