Dissertations / Theses on the topic 'Specific heat'
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McDonald, Frank Carl. "Specific heat measurements of copper benzoate." [Gainesville, Fla.] : University of Florida, 2003. http://purl.fcla.edu/fcla/etd/UFE0002844.
Full textNishizaki, Shuji. "Specific Heat of the Spin-Triplet Superconductor Sr2RuO4." 京都大学 (Kyoto University), 2000. http://hdl.handle.net/2433/181099.
Full text0048
新制・課程博士
博士(理学)
甲第8131号
理博第2153号
新制||理||1145(附属図書館)
UT51-2000-F35
京都大学大学院理学研究科物理学・宇宙物理学専攻
(主査)助教授 前野 悦輝, 教授 石黒 武彦, 教授 Sigrist Manfred(シーグリスト マンフレッド)
学位規則第4条第1項該当
Dahn, Douglas Charles. "Low temperature specific heat of LixNbS2 intercalation compounds." Thesis, University of British Columbia, 1985. http://hdl.handle.net/2429/25563.
Full textScience, Faculty of
Physics and Astronomy, Department of
Graduate
Varadarajan, Vijayalakshmi. "SPECIFIC HEAT MEASUREMENTS ON STRONGLY CORRELATED ELECTRON SYSTEMS." UKnowledge, 2009. http://uknowledge.uky.edu/gradschool_diss/805.
Full textGlockling, James L. D. "Heat and mass transfer in specific aerosol systems." Thesis, London South Bank University, 1991. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.303937.
Full textMoran, Joel Patrick. "Specific heats of aqueous lithium bromide solutions." Thesis, Georgia Institute of Technology, 1988. http://hdl.handle.net/1853/16363.
Full textPolcyn, Adam D. (Adam Daniel) 1970. "Specific heat of Sr₃CuPt₀₅Ir₀.₅O₆ below 1K." Thesis, Massachusetts Institute of Technology, 1999. http://hdl.handle.net/1721.1/85335.
Full textBalci, Hamza. "Specific heat and nernst effect of electron-doped cuprate superconductors." College Park, Md. : University of Maryland, 2004. http://hdl.handle.net/1903/217.
Full textThesis research directed by: Physics. Title from t.p. of PDF. Includes bibliographical references. Published by UMI Dissertation Services, Ann Arbor, Mich. Also available in paper.
Kirkham, Mark. "High temperature specific heat capacity measurement of Ni2+XMn1-XGa." Thesis, Loughborough University, 2014. https://dspace.lboro.ac.uk/2134/14416.
Full textZhu, Xiaoyi. "Prediction of Specific Heat Capacity of Food Lipids and Foods." The Ohio State University, 2015. http://rave.ohiolink.edu/etdc/view?acc_num=osu1437750532.
Full textMohammed, K. A. "Low temperature specific heat measurements of crystalline and amorphous magnetic materials." Thesis, University of Southampton, 1985. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.356096.
Full textLang, Brian E. "Specific Heat and Thermodynamic Properties of Metallic Systems: Instrumentation and Analysis." BYU ScholarsArchive, 2005. https://scholarsarchive.byu.edu/etd/785.
Full textZink, Barry Lee. "Specific heat and thermal conductivity of thin film amorphous magnetic semiconductors /." Diss., Connect to a 24 p. preview or request complete full text in PDF format. Access restricted to UC campuses, 2002. http://wwwlib.umi.com/cr/ucsd/fullcit?p3070996.
Full textChastin, S. "Low temperature specific heat and thermal conductivity of Kondo intermetallic compounds." Thesis, University of Sussex, 1998. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.244320.
Full textPoon, Wai-hei. "The induction of cellular stress responses by specific Kappa-opioid receptor agonist." Click to view the E-thesis via HKUTO, 2004. http://sunzi.lib.hku.hk/hkuto/record/B31473921.
Full textYOSHIKAI, YASUNOBU. "Regulatory Role of Heat Shock Protein-specific T Cells in Host Defense." Nagoya University School of Medicine, 1992. http://hdl.handle.net/2237/17519.
Full textNyeanchi, Emmanuel Bongkiyung. "Resistivity and specific heat capacity of high Tc superconductors and magnetic materials." Thesis, University of Sussex, 1994. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.239591.
Full textChen, Karen. "Studies on LiYRF." Thesis, Boston College, 2010. http://hdl.handle.net/2345/1561.
Full textSenior thesis on muon spin relaxation study of LiHoXY1-XF4 and semi-adiabatic specific heat experiment on LiTb0.40Y0.60F4
Thesis (BS) — Boston College, 2010
Submitted to: Boston College. College of Arts and Sciences
Discipline: Physics Honors Program
Discipline: Physics
Poon, Wai-hei, and 潘偉曦. "The induction of cellular stress responses by specific Kappa-opioid receptor agonist." Thesis, The University of Hong Kong (Pokfulam, Hong Kong), 2004. http://hub.hku.hk/bib/B31473921.
Full textMohamed, Mahmoud. "Physical Properties of Iron-based Superconductors Probed by Low-Temperature Specific-Heat Measurements." Doctoral thesis, Saechsische Landesbibliothek- Staats- und Universitaetsbibliothek Dresden, 2012. http://nbn-resolving.de/urn:nbn:de:bsz:14-qucosa-98736.
Full textRodan, Steven. "Nuclear magnetic resonance and specific heat studies of half-metallic ferromagnetic Heusler compounds." Doctoral thesis, Saechsische Landesbibliothek- Staats- und Universitaetsbibliothek Dresden, 2016. http://nbn-resolving.de/urn:nbn:de:bsz:14-qucosa-198412.
Full textLeigh, Nigel Royston. "Specific heat measurements on chevrel phase materials exhibiting coexistence of superconductivity and magnetism." Thesis, Durham University, 2001. http://etheses.dur.ac.uk/3849/.
Full textKmety-Stevenson, Carmen R. "Phase transitions in molecule-based magnets : neutron diffraction, magnetic and specific heat studies /." The Ohio State University, 2000. http://rave.ohiolink.edu/etdc/view?acc_num=osu1343146984.
Full textHunt, Andrew Philip. "Heat strain, hydration status, and symptoms of heat illness in surface mine workers." Thesis, Queensland University of Technology, 2011. https://eprints.qut.edu.au/44039/1/Andrew_Hunt_Thesis.pdf.
Full textWakelin, Jonathan Peter. "Low temperature specific heat and thermal conductivity of doped YBa2Cu3O7 and other ceramic superconductors." Thesis, University of Sussex, 1995. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.284082.
Full textKim, Dongkyun. "Specific heat and magnetization measurements on the ferromagnetic phase transition of manganites and ruthenates /." Diss., Connect to a 24 p. preview or request complete full text in PDF format. Access restricted to UC IP addresses, 2002. http://wwwlib.umi.com/cr/ucsd/fullcit?p3044768.
Full textParry, Thomas J. "I. Thermodynamics and Magnetism of Cu2OCl2 II. Repairs to Microcalorimeter the "2"s are subscripts, and the second 2 is preceded by a lower case L, not a one." Diss., CLICK HERE for online access, 2008. http://contentdm.lib.byu.edu/ETD/image/etd2609.pdf.
Full textKoppanooru, Sampat Kumar Reddy. "Estimating Thermal Conductivity and Volumetric Specific Heat of a Functionally Graded Material using Photothermal Radiometry." Thesis, University of North Texas, 2017. https://digital.library.unt.edu/ark:/67531/metadc1062896/.
Full textHollenhead, James B. "A calorimetric study of the immersion of bituminous coal in liquids." Thesis, Virginia Tech, 1988. http://hdl.handle.net/10919/45157.
Full textThe oxidation of both unextracted and extracted coal at
3200C was followed by immersional measurements in water.
The heat of immersion increased rapidly with oxidation time,
leveling off after 3 hours of oxidation. Extraction with
methanol or pyridine prior to oxidation and immersion
lowered the time of immersion in water compared to the
unextracted case. The oxidation of coal was also followed
by x-ray photoelectron spectroscopy (XPS). The XPS
oxygen/carbon ratios correlated linearly with the heats of
immersion for the extracted, oxidized coals. Thus, XPS was
shown to be a useful ancillary technique to heat of
immersion for the study of coal surfaces.
Master of Science
Babaee, Koochaksaraee Sima, and Sara Ghahremanpour. "Using Design of Experiments in Validation of a new calorimetric method for the specific heat capacity determination." Thesis, Högskolan i Borås, Institutionen Ingenjörshögskolan, 2009. http://urn.kb.se/resolve?urn=urn:nbn:se:hb:diva-19555.
Full textTovstyuk, C. C. "Thermodynamic Functions of Electron Gas in Strong anisotropic Materials. Quantum Gas." Thesis, Sumy State University, 2015. http://essuir.sumdu.edu.ua/handle/123456789/42583.
Full textMadden, Marie Catherine. "A non-clinical method to simultaneously estimate thermal conductivity, volumetric specific heat, and perfusion of in-vivo tissue." Thesis, Virginia Tech, 2004. http://hdl.handle.net/10919/34799.
Full textMaster of Science
Li, Gang. "Generation of Tumor-Specific Immunity Using HER2/NEU Positive Tumor Derived Chaperone-Rich Cell Lysate (CRCL)." Diss., The University of Arizona, 2007. http://hdl.handle.net/10150/193817.
Full textSchmidt, Joel Edward. "The Use of Ammonium Carbamate as a High Specific Thermal Energy Density Material for Thermal Management of Low Grade Heat." University of Dayton / OhioLINK, 2011. http://rave.ohiolink.edu/etdc/view?acc_num=dayton1310666985.
Full textLoula, George Dourado. "Estudo das propriedades físicas dos compostos UptSn e U(Cu, Au)Sn." [s.n.], 2005. http://repositorio.unicamp.br/jspui/handle/REPOSIP/277787.
Full textDissertação (mestrado) - Universidade Estadual de Campinas, Instituto de Fisica Gleb Wataghin
Made available in DSpace on 2018-08-10T12:45:58Z (GMT). No. of bitstreams: 1 Loula_GeorgeDourado_M.pdf: 2173914 bytes, checksum: ff1208aeb34d1619646a01ea6f3f1ec8 (MD5) Previous issue date: 2005
Resumo: Neste trabalho realizamos medidas de difração de raios-X, magnetização, calor específico e resistividade elétrica nos compostos da série U(Cu,Au)Sn, além do composto UPtSn, que pode cristalizar-se tanto na forma hexagonal (sem tratamento térmico) quanto cúbica, com tratamento térmico de 850ºC por uma semana. Na série UCu(1-x)A u(x)Sn verificamos que todos os compostos apresentam ordenamento antiferromagnético, sendo que a temperatura de ordenamento magnético ( TN) decresce com o aumento da concentração do substituinte. Além disso, percebe-se um pequeno aumento no calor especifico eletrônico ( d ) e no volume da célula unitária ao se inserir Au. O momento efetivo do urânio diminui de 3.44 m B para x=0 até 3 m B para x=1, devido a uma maior hibridização 5f-s,d decorrente da substituição do Cu por Au. Essa hibridização propicia diversas alterações nas propriedades físicas dos compostos. Quanto ao sistema UPtSn, verificamos que o tratamento térmico ao qual a amostra é submetida influencia na formação estrutural do composto e as propriedades físicas de cada estrutura são muito distintas. A fase cúbica ordena antiferromagneticamente em 35K e o urânio apresenta momento magnético efetivo igual a 3.24 m B, enquanto que a fase hexagonal ordena ferromagneticamente em 27K, e apresenta momento magnético efetivo de 2.82 m B. Esta redução no momento efetivo pode ser devida ao efeito Kondo, mas os resultados experimentais não são conclusivos quanto a isto
Abstract: In this work we report on measurements of x-ray diffraction, magnetization, specific heat and electrical resistivity for the series U(Cu,Au)Sn and for UPtSn, which crystallize either with hexagonal (as-cast) or with cubic simmetry (annealed). In the series UCu(1-x)Ausub(x)Sn we verify that all the compounds order antiferromagnetically and the magnetic ordering temperature (TN) decreases when the substitute's concentration is increased. We also noticed a small increase of the electronic specific heat coefficient and unit cell volume by replacing Au for Cu. The effective moment is reduced from 3.44 m B at x=0 to 3 m B at x=1 due to a more effective 5f-s,d hybridization. This hybridization is responsible for the phisical properties of these compounds. For UPtSn we found that the thermal treatment can define the structure of the compound. The phisical properties of both compound are quite different. The cubic phase is AF with TN = 35K and present m eff = 3.24 m B while the hexagonal phase orders at 27K with m eff = 3B. Such reduction of the effective moment may be due to the Kondo effect but the experiments where not conclusive about this
Mestrado
Física da Matéria Condensada
Mestre em Física
Klein, Markus. "Single-Zone Cylinder Pressure Modeling and Estimation for Heat Release Analysis of SI Engines." Doctoral thesis, Linköping : Department of Electrical Engineering, Linköping University, 2007. http://urn.kb.se/resolve?urn=urn:nbn:se:liu:diva-9863.
Full textMášová, Pavla. "Možnosti regulace vneseného tepla - experimentální ověření." Master's thesis, Vysoké učení technické v Brně. Fakulta strojního inženýrství, 2011. http://www.nusl.cz/ntk/nusl-229977.
Full textAli, Salamat. "Specific heat measurements using the A.C. technique on the chevrel phase superconductor Pb(_1-x)Gd(_x)Mo(_6)S(_8) in high magnetic fields." Thesis, Durham University, 1996. http://etheses.dur.ac.uk/5284/.
Full textLopes, Valerio Hayles Vivian. "The Treatment of Indians and Women as the Other in Ruth Prawer Jhabvala’s Heat and Dust: : Olivia’s and the Nawab’s Experiences of Discrimination as the Primary Reason for Their Mutual Attraction." Thesis, Högskolan Dalarna, Engelska, 2018. http://urn.kb.se/resolve?urn=urn:nbn:se:du-28117.
Full textDjurkovic, Borko. "Specific Heat of Unconventional Superconductors." Thesis, 2010. http://hdl.handle.net/10012/5687.
Full textLin, XI Chan Moses H. W. "Specific heat of solid ⁴He." 2008. http://etda.libraries.psu.edu/theses/approved/WorldWideIndex/ETD-2859/index.html.
Full textYi-ChenTseng and 曾意真. "Electronic specific heat of graphites." Thesis, 2012. http://ndltd.ncl.edu.tw/handle/24906962587030845769.
Full text國立成功大學
物理學系碩博士班
100
Abstract In this paper, we use the tight-binding model to study the density of states (DOS), the chemical potential, and the electronic specific heat of graphite. Different stacking sequences are taken into consideration, including monolayer, AA-, AB-, and ABC-stacked configurations. The different geometric structures result in the various energy bands. The band symmetry and degeneracy also reflect in the density of states and chemical potential, and thus affect the temperature-dependence of electronic specific heat. The energy bands of monolayer graphite (graphene) present a complete symmetry with respect to the Fermi level where two linear bands intersect. As a result, the DOS at the Fermi energy and the chemical potential are both zero, and the electronic specific heat is proportional to the square of the temperature. The energy bands of AA-stacked graphite are also symmetric about the Fermi level with more overlapping between linear bands. The DOS at the Fermi energy is therefore a considerable value, while the chemical potential hardly changes with the temperature. Its electronic specific heat is in direct proportion to the temperature. As for AB-stacked graphite, the energy bands are asymmetric, and the double degeneracy occurs on H-layer. Consequently, it reveals less symmetry in the DOS, and the chemical potential decreases with the increasing temperature. The electronic specific heat at low temperatures can be described by a linear relation, but such relationship no longer exists at high temperatures. The conduction and valence bands of ABC-stacked graphite show slight symmetry with two intersections of linear bands above and below the Fermi level on K- and H-layers respectively. The DOS is symmetric, the chemical potential rises with the temperature, and the specific heat is roughly proportional to the square of the temperature.
Ke, Cheng-Wen, and 柯誠文. "Specific heat and magnetism of MnxSi." Thesis, 2012. http://ndltd.ncl.edu.tw/handle/85962802517684867653.
Full text國立交通大學
物理研究所
101
We have measured the specific heat of MnxSi single crystals with the various manganese contents (x = 0.998, 0.981, 0.961, 0.945). We classified the magnetic transition features. The first kind has only one peak. The other kind have one sharp peak and a broad peak at higher temperature. The Debye temperatures and the γ have been calculated by fitting the specific heat from 100 K to 200 K. We subtract the electron and phonon contributions to obtain the purely magnetic contribution. Then, we calculated the magnetic entropy difference between these two types of compounds. We compared current results to the specific heat of the LiCu2O2 and the magnetic structure model provide by S.W. Huang et al. (Physical Review Letters 101, 077205(2008) ) and to the study of MnSi by S.V. Grigoriev et al.(Physical Review B 79, 144417(2009) ) and A. Bauer et al.(Physical Review B 85, 214418(2012) ). We discuss what physical mechanism is in the magnetic transitions.
Kang, Yu-Ching, and 康玉清. "Specific heat studies on NaxCoO2‧yH2O superconductor." Thesis, 2004. http://ndltd.ncl.edu.tw/handle/99475673063296322149.
Full text國立中山大學
物理學系研究所
92
Since the discovery of high superconducting transition temperature in layered copper oxides, many researchers have searched for similar behavior in other layered metal oxides, such as cobalt and nickel. The sodium cobalt oxyhydrate is the first cobalt-oxide layered superconductor. We present the studies of low-temperature specific heat C(T, H) in NaxCoO2‧yH2O (x ~ 0.35, y ~ 1.3). At H = 0, a very sharp anomaly was observed at T ~ 4.7 K indicating the existence of bulk superconductivity. There exists an αT2 term in C(T, H=0) in the superconducting state manifesting the line nodal superconducting order parameter. The feature at the superconducting transition is rather sharp, becoming broad and strongly suppressed in an applied magnetic field. The transition temperature also changed in an applied magnetic field. Thus an abrupt change of slope in H vs. Tc curve was observed. Possible scenarios such as the multiple phase transitions in the mixed state are discussed.
Chen, Kuen-He, and 陳昆河. "Specific heat of anharmonic oscillators in one dimension." Thesis, 2000. http://ndltd.ncl.edu.tw/handle/96425039922746733773.
Full text國立交通大學
物理研究所
88
The specific heats of one-dimension systems are obtained with two different methods, which are achieved in terms of the partition function and the probability density function, respectively. In this thesis, we consider three kinds of anharmonic potentials and calculate numerically the specific heat of a particle moving in a potential in one dimension and also at thermally equilibrium with a heat bath. From the views of classical statistical mechanics, the method from the partition function is standard, direct and simple. In addition, we construct the probability density function of a stochastic variable. Since we can calculate < V > / T and < V > / T , this method can gives us more information. Namely, we can realize the specific heat more deeply. For a symmetric double-well potential, V , we find that at very low temperature the curve of the specific heat has a peak. In addition, we also respectively calculate the specific heats of a symmetric single-well potential, V , and an asymmetric single-well one, V . After comparing the specific heats of these three potentials, we interpret the specific heats of them from the view of the geometry of these potentials. In V and V , we find that there is a region in the potential where the potential curvatures are negative. Finally we suggest that the peak of the specific heat of a one-dimension system, once it appears, is associated with the existence of negative curvature of the potential.
Huang, Chien-Hsun, and 黃建勳. "Specific Heat of Molten Salt Embedded with NanoParticles." Thesis, 2012. http://ndltd.ncl.edu.tw/handle/12481835014841901078.
Full text國立交通大學
機械工程學系
100
Molten salts are extensively used as a thermal energy storage material in solar-thermal power plants nowadays. The energy storage capacity of a solar-thermal power plant is restricted by the specific heat capacity of the molten salt. In this work, the effect of concentration and size of the nanoparticles on the specific heat capacity of the molten salt embedded with the nanoparticles (named as nano-salt) was studied. The nano-salts having alumina nanoparticles of two different sizes (13 nm and 90 nm) and three volume concentrations (1.1 %、3.3 % and 5.4 %) were synthesized. Experimental results show that the specific heat capacity of the nano-salt decreases as the volume concentration increases. Meanwhile, the nano-salts doped with 90 nm alumina nanopartilces have a larger specific heat capacity than that of nano-salts doped with 13 nm alumina nanoparticles. In addition, the predictions from the current existing models have a large difference from the experimental data. Thus, a modified model considering the nanolayer effect on the specific heat capacity of the nano-salt was proposed. The prediction based on this modified model agrees better with the experimental data as compared to the existing models.
Ho, Ming-Xi, and 何明析. "Enhancement of Specific Heat Capacity and Heat Transfer Performance of Nano-Nitrate Salt Eutectics." Thesis, 2018. http://ndltd.ncl.edu.tw/handle/65urb4.
Full text國立清華大學
工程與系統科學系
106
Both solar thermal and nuclear power systems are important energy options with low carbon emissions. Molten salt has been proposed as the working fluid in a concentrating solar power system, and it is also suggested to be employed in a molten salt reactor, which is one of six types of Generation-IV power systems. Molten salts present feature of high heat capacity and high thermal stability. Nevertheless, molten salts usually exhibit relatively poor heat transfer performance and non-uniform temperature distribution. Besides, the specific heat capacity of molten salts is not as high as water and there is a need for the enhancement. This study demonstrates the variation of specific heat capacity and heat transfer performance in the molten salt doped with nanoparticles. Innovative apparatus and procedures have been developed to prepare the specimen of molten salt with high quality. Moreover, a series of thermal-physical characteristics, including melting point, decomposition temperature, thermal diffusivity, thermal conductivity and specific heat capacity for a pure fluoride salt (FLINAK) and a nitrate salt (HITEC) are measured and compared with that reported in the literature to validate the specimen prepared. At first, this work studied the effect of alumina nanoparticles (mean diameter about 40 nm) concentration on the specific heat capacity of molten HITEC salt, which is called nano-HITEC. The nano-HITEC salt in this study is free of surfactant and an innovative preparation process and sampling apparatus for molten nano-HITEC have been established in the present study to avoid the possible precipitation of nanoparticles. The specific heat of molten HITEC and nano-HITEC are measured using a power compensated differential scanning calorimeter (DSC) at the Industrial Technology Research Institute (ITRI) of Taiwan. A power compensated DSC monitors the endothermic or exothermic reaction of specimen under a constant heating rate to determine the specific heat capacity of specimen. In this work, an optimal concentration of 0.063 wt.% is identified, demonstrating the highest enhancement on the specific heat capacity of 19.9%. Lower or higher concentration of nanoparticles tends to reduce the enhancement. For the concentration of 2 wt.%, the negative effect of doping the nanoparticles on the specific heat capacity appears for all temperatures in the present study. The SEM images after solidification of samples reveal that near uniform dispersion of nanoparticles with negligible agglomeration for the concentration smaller than 0.016 wt.%. The agglomeration becomes significant and the particle clusters seem to be inter-connected for higher concentrations. Moreover, this study conducts a statistical analysis on the number of isolated particles and number and size of clusters using SEM images to develop a simplified model, which describes the area of particle-liquid interface of nano-HITEC fluid with different concentration. The results indicate that the agglomeration of nanoparticles occurs as the concentration is over 0.023 wt.%; clusters with different sizes are formed and the total area of isolated particles is decreased and the clusters begin to contribute to the total interfacial areas with the overall area decreasing at the beginning. The minimum particle-liquid interface take place at concentration of 0.048 wt.%. Subsequently, the total interfacial area increases with increasing concentration. It is found that the optimal concentration is corresponding to approximately the concentration that the contribution of isolated nanoparticles and particle clusters, size ranging from 0.2 to 0.6 μm, to the interfacial area are approximately the same. The interfacial phenomena at the particle (isolated or cluster) fluid interface is proposed in the literature to be the primary reason for the enhancement of specific heat capacity in nano-salts. Subsequently, the effect of nanoparticle concentration on the laminar convective heat transfer performance for molten nano-HITEC fluid in a mini-circular tube is investigated. An innovative piston driven molten salt apparatus and preparation process of molten HITEC nanofluild are developed to prevent the precipitation of nanoparticles during the measuring process. The piston molten salt pump provides steady flow through the test section which the channel diameter and length are 2.1 mm and 120 mm, respectively. The mean heat transfer of molten salt flow can be evaluated by Newton’s cooling law based on the inlet/outlet temperature and three wall temperatures measured at three axial locations. The results demonstrate that the measurement of mean Nusselt number of the pure HITEC fluid in this study be in good agreement within ±10% with a well-known correlation. A concentration of nanoparticles of 0.25 wt.% in the nano-HITEC, which can be maintained uniform dispersion for about 30 minutes, results in the maximum enhancement of mean Nusselt number of 11.6%. On the other hand, a concentration of 0.063 wt.% provides 9.2% enhancement on the mean Nusselt number of HITEC nanofluid, and precipitation phenomenon is not observed within an hour. In addition, a new correlation with consideration of particle concentration for the laminar convective heat transfer performance of the nano-HITEC fluid in the present minichannel is developed, by which more than 93.9% of the experimental data can be predicted within ±10% of deviation. A nano-HITEC fluid with concentration of 0.063 wt.% of alumina particle of about 40 nm demonstrates best enhancements of its specific heat capacity of 19.9% as well as near best heat transfer performance in this study. This suggests that nano-HITEC of 0.063 wt.% of nano alumina particles of about 40 nm may serve as a working fluid for applications in a thermal storage system or a concentrating solar power system.
洪大軒. "Superconductivity, Specific heat and Magnetic Properties in CeRu2 Nanoparticles." Thesis, 2004. http://ndltd.ncl.edu.tw/handle/92756310186815189589.
Full text輔仁大學
物理學系
92
CeRu2 is a type Ⅱ superconductor with a superconduting transition temperature TC = 6 K. Its peak effect in magnetization was attributed to the pinning centers in the specimen. Applying the technique of Excimer laser ablation specimens of nanoparticle were fabricated. The X-ray diffraction patterns of nanoparticles not only showed the broadening of diffraction peaks, but also exhibited the increase of the lattice constant. From the measurements of magnetic susceptibility and heat capacity, the superconductivity in nanoparticles was observed with TC near that of the bulk. In nanoparticles a low-temperature anomaly was observed and was confirmed to be a Kondo effect through the measurements of heat capacity under magnetic field. The superconductivity in the bulk was suppressed from 6 K to 0.9 K as magnetic field up to 8 T. However the superconductivity (TC= 5.95 K) in nanoparticles hardly be influenced by the magnetic field even with the field up to 8 T. In magnetic susceptibility the occurrence of Meissner was observed at 4.5 K with a field as small as 100 G. The result of (T) which is different from that of C(T) may be the characteristic of magnetic properties of nanoparticles. A possible reason is that the contribution of paramagnetism in nanoparticles smears the diamagnetism of superconductivity. The existence of superconductivity in nanoparticles can be explained by the competition of Kondo interaction,electronic energy level splitting and the energy gap of superconductivity .
陳伯仲. "Superconductivity, specific heat and magnetic properties in CeCo2 nanoparticles." Thesis, 2004. http://ndltd.ncl.edu.tw/handle/96982280556011619242.
Full text輔仁大學
物理學系
92
In this thesis we studied the correlation of superconductivity, magnetism and heat capacity with the size in CeCo2. As the size decreases to nanoscale the fraction of surface atoms increases dramatically and the influence of the surface effect on physical properties becomes significant. In the meantime the electronic band structure become broaden and more discreteness. Bulk CeCo2 is a superconductor with Tc = 1.2 K. However the superconductivity disappears as the size of CeCo2 is reduced to 5.8nm - 14nm. The consequence is just as suggested by P. W. Anderson, the superconductivity will no longer exist when the electronic energy level splitting is larger than the energy gap of superconductivity. It is also observed that the lattice constant shrinks with the decrease of sample size. From the measurements of heat capacity, the electronic state of Ce was changed from intermediate valence into trivalence as particle size decreased. An occurrence of Kondo anomaly was also observed in nanoparticles. The Kondo anomaly was confirmed by the peak shifting to higher temperature with the increase of magnetic field. An important result was also found in heat capacity, that was the Kondo temperature and the volume fraction of Ce3+ declined as the particle size decreased. Based on the measurements of magnetic susceptibility it was kwon that the effective moment μB in nanoparticles was larger than that in the bulk.
Li, Hsiao-Hsun, and 黎孝勳. "Specific Heat Studies on the Electron-doped Superconductor Pr1.85Ce0.15CuO4." Thesis, 2001. http://ndltd.ncl.edu.tw/handle/31180598047408373255.
Full text國立中山大學
物理學系研究所
89
In this thesis we synthesize Pr1.85Ce0.15CuO4 system by mean of X-ray diffraction, electrical resistivity, magnetic susceptibility and low-temperature specific heat. From these data analysis, we hope to more clearly understand the transition of electron-doped superconductor Pr2-xCexCuO4 (0.14