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Transport thermal

As described above, quantum restrictions limit tire contribution of tire free electrons in metals to the heat capacity to a vety small effect. These same electrons dominate the thermal conduction of metals acting as efficient energy transfer media in metallic materials. The contribution of free electrons to thermal transport is very closely related to their role in the transport of electric current tlrrough a metal, and this major effect is described through the Wiedemann-Franz ratio which, in the Lorenz modification, states that... [Pg.167]

Since air has relatively poor thermal transport properties when compared to water, the air cooled heat exchanger could have considerably more heat transfer surface area. A large space requirement may result. [Pg.13]

In contrast to the strong effect of gas properties, it has been found that the thermal properties of the solid particles have relatively small effect on the heat transfer coefficient in bubbling fluidized beds. This appears to be counter-intuitive since much of the thermal transport process at the submerged heat transfer surface is presumed to be associated with contact between solid particles and the heat transfer surface. Nevertheless, experimental measurements such as those of Ziegler et al. (1964) indicate that the heat transfer coefficient was essentially independent of particle thermal conductivity and varied only mildly with particle heat capacity. These investigators measured heat transfer coefficients in bubbling fluidized beds of different metallic particles which had essentially the same solid density but varied in thermal conductivity by a factor of nine and in heat capacity by a factor of two. [Pg.162]

This packet renewal model has been widely accepted and in the years since 1955 many researchers have proposed various modifications in attempts to improve the Mickley-Fairbanks representation. Several of these modifications dealt with the details of the thermal transport process between the heat transfer surface and the particle packet. The original Mickley-Fairbanks model treated the packet as a pseudo-homogeneous medium with a constant effective thermal conductivity, suggesting that... [Pg.164]

At milli-kelvin temperatures, the problem of contact resistance between helium and solids becomes more complex. Thermal transfer phenomena take place involving spins and thermal resistance of sintered materials. The understanding of the thermal transport at very low temperature is of the utmost importance, also from a technical point of view, since helium is the working substance in dilution refrigerators (see Chapter 6). [Pg.110]

Recent developments of materials and devices with structures in nanometer length scales have created new opportunities and challenges in the science of thermal transport. Interfaces play a particularly important role in the properties of nanoscale structures and nanostructured materials [97-98], This is why a renewed interest for contact resistance arose in recent years with studies of nanocomposite, semicrystalline and polycrystalline materials where contact resistances has a controlling role to determine the bulk thermal conductivity of the material [99-100],... [Pg.115]

Weber WJ, Griffin CW, and Bates JL. Effects of cation substitution on electrical and thermal transport properties of Y0rO3 and LaCr03. J. Am. Ceram. Soc. 1987 70 265-270. [Pg.205]

Eq. (437) may be transformed into a true transport equation for f this transport equation is the generalized linearized Boltzmann equation for f, as it also appears in the theory of thermal transport coefficients. More precisely, we get ... [Pg.261]

Aliev AE, Guthy C, Zhang M, Fang S, Zakhidov AA, Fischer E, et al. Thermal transport in MWCNT sheets and yarns. Carbon. 2007 Dec 45(15) 2880-8. [Pg.253]

Mass and energy transport occur throughout all of the various sandwich layers. These processes, along with electrochemical kinetics, are key in describing how fuel cells function. In this section, thermal transport is not considered, and all of the models discussed are isothermal and at steady state. Some other assumptions include local equilibrium, well-mixed gas channels, and ideal-gas behavior. The section is outlined as follows. First, the general fundamental equations are presented. This is followed by an examination of the various models for the fuel-cell sandwich in terms of the layers shown in Figure 5. Finally, the interplay between the various layers and the results of sandwich models are discussed. [Pg.450]

An important issue requiring future work is the consideration of anisotropic thermal transport since the thermal conductivity has an order of magnitude difference between the in-plane and through-phase directions as mentioned earlier. [Pg.501]

Yamashita M, Nakata N, Kasahara Y, Sasaki T, Yoneyama N, Kobayashi N, Fujimoto S, Shibauchi T, Matsuda Y (2009) Thermal-transport measurements in a quantum spin-liquid state of the frustrated triangular magnet k-(BEDT-TTF)2Cu2(CN)3. Nat Phys 5 44-47... [Pg.126]

In Eqs. (3.58) and (3.59), the kt are the reaction rate constants. We will see in Chapter 4 that many solid-state ceramic processes involve simultaneous mass transport (diffusion), thermal transport, and reaction. [Pg.246]

All trap-spectroscopic techniques that are based on thermal transport properties have in common that the interpretation of empirical data is often ambiguous because it requires knowledge of the underlying reaction kinetic model. Consequently, a large number of published trapping parameters—with the possible exception of thermal ionization energies in semiconductors—are uncertain. Data obtained with TSC and TSL techniques, particularly when applied to photoconductors and insulators, are no exceptions. [Pg.9]

The temperature dependence of various thermal transport phenomena can be measured isothermally at a number of different temperatures where the sample is in thermal equilibrium, in steady-state equilibrium, or decays after pulsed excitation in a transient fashion. In contrast, TSL and TSC experiments are nonisothermal and observed only during a programmed change in a sample temperature. [Pg.9]

If one were to judge the importance of TSL and TSC relative to other thermal transport methods for trap characterization by number of recently published papers, these techniques appear to far outweigh all others combined, even though about one-third of the publications are concerned with applications in dosimetry and related TSL (TSC) instrumentation. However, the large number of articles on TSL and TSC does not necessarily indicate any advantage in their usefulness as trap-spectroscopy tools over the other methods. What can safely be concluded is that nonisothermal TSR is still, at the present time, a very active field of research. [Pg.9]

K rm n (K3) and Prandtl (P7) indicated analogies between momentum and thermal transport and placed the matter before the engineering profession. Using Karm n s original analysis (Kl) Deissler (D2) indicated that on the basis of the similarity hypothesis the eddy viscosity may be evaluated for steady, uniform flow in the following way ... [Pg.251]

The foregoing discussion relates to the transport of momentum under steady, uniform conditions in turbulently flowing streams. Such matters are of direct interest to the chemical engineer but usually only as they influence the power requirements for the movement of fluids. A deeper interest exists in prediction of the thermal transport and temperature... [Pg.253]

The present approach to the prediction of thermal transport in turbulent flow neglects the effect of thermal flux and temperature distribution upon the relationship of thermal to momentum transport. The influence of the temperature variation upon the important molecular properties of the fluid in both momentum and thermal transport may be taken into account without difficulty if such refinement is necessary. [Pg.255]

In a description of thermal transport in steady, uniform flow it is necessary to consider the conservation of internal and kinetic energy (K7) under conditions involving gross motion of the fluid. For laminar flow... [Pg.255]

Reynolds (Rl) suggested that the natures of turbulent momentum and thermal transport were similar. K rm n (K2) extended this analysis and defined eddy conductivity in the following way for steady, uniform, two-dimensional flow ... [Pg.256]


See other pages where Transport thermal is mentioned: [Pg.255]    [Pg.163]    [Pg.19]    [Pg.21]    [Pg.182]    [Pg.398]    [Pg.127]    [Pg.90]    [Pg.196]    [Pg.371]    [Pg.163]    [Pg.201]    [Pg.72]    [Pg.426]    [Pg.136]    [Pg.136]    [Pg.290]    [Pg.241]    [Pg.241]    [Pg.254]    [Pg.254]    [Pg.255]   
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