The flash technique for measuring thermal diffusivity is analyzed for the case of a cylindrical-shaped specimen of radius r0 and thickness a to determine the effects of radiation at high temperatures, finite duration of the heat pulse, and the feasibility of low temperature measurements. It is found that the flash diffusivity method is useful in two complementary limits: (1) pulse time τ short compared to the characteristic thermal response time tc, (2) τ/tc of the order 1 to 10. The former case corresponds to the original description of Parker, Jenkins, and Abbott, while the latter case is suitable at very low temperatures. Moreover, it is shown that there is an optimum specimen thickness a for a given material and pulse time τ, in the sense that a higher temperature can be reached before any corrections have to be made to the Parker et al. analysis.
We present a convenient formulation of the single-domain energy in the wall-energy model and minimize the total energy of a lattice of cylindrical domains and of a parallel-stripe array in an infinite plate. The latter structure is shown to have the lower energy for external transverse fields Hex<H1 while the lattice is favored for H1≤Hex<H2. The critical domain sizes and fields bounding these structures are calculated as functions of the plate thickness and the material parameters. The factors which affect the evolution of the domain structures in finite and nearly defect-free plates are discussed and the following conclusions drawn: Domain nucleation is favored by the presence of nonuniformities such as cracks or mounds. Stripes nucleated at cracks or boundaries expand and contract with one end tied to the nucleation point and there may be only as many stripes as nucleation centers. An energy barrier inhibits the separation of a domain from (or the joining to) a free edge boundary or another domain. Closed domains are repelled by boundaries and alternate between stripe- and bubble-domain configurations as the local field varies below and above the critical stripe-bubble instability value. The qualitative conclusions can be quantified to some extent in the wall-energy model and provide a satisfactory explanation of the domain structures observed in a high-mobility garnet film.
It is noted in this paper that the total energy of the electron-ion system in the metallic state arises from an electron self-energy term as well as volume-dependent pairwise interaction terms among the ions. The Slutsky-Garland model used by Schmunk et al. to analyze the experimental dispersion curves of Be does not give the proper elastic behavior. The experimental dispersion curves for beryllium and zinc measured by Schmunk et al. and Borgonovi et al., respectively, are analyzed using a model consistent with the elastic behavior. For beryllium, the calculated dispersion curves agree well with the neutron inelastic-scattering data and the elastic constants of Smith and Arbogast. For zinc, the calculated frequencies are within the experimental uncertainties with the exception of the transverse branches along the [OllO] direction which describes atomic motions perpendicular to the basal planes. The experimental data on Zn indicate high dispersion and fluctuations in frequency w versus wave number q. The calculated elastic constants agree within a few percent with the experimental data of Alers and Neighbours at 300°K, with the exception of C44 and C13, which are low by 19% and 27%, respectively. The Debye-Waller factor and the specific heat for both metals are compared with available experimental data. It is found that the calculated specific heat for zinc is in excellent agreement with experiment over the whole temperature range. However, for beryllium, the calculated values are low for small temperatures; the discrepancy could be attributed to heavy impurities in beryllium. The anisotropy in the Debye-Waller factor for zinc is in good agreement with x-ray and Mossbauer experiments.
Measurements have been made of relative marker movements in Au and Cu in the presence of temperature gradients of the order of 1200°K/cm. These experiments yielded results which indicate that a net vacancy current is established in these metals under appropriate experimental conditions. The magnitude and direction of the observed effects are consistent with kinetic theory predictions in conjunction with previously determined vacancy energies. A three-dimensional extension of existing kinetic theory is developed and important factors which do not appear in one-dimensional treatments are discussed. Porosity development in Cu was found under certain conditions and this may be a visual demonstration of the existence of a thermal diffusion effect in Cu.
A new analysis is presented of the shape of a liquid drop under the influence of gravity and surface tension. A variational method is used to minimize the total energy of the drop and the resulting expressions for the drop shape are evaluated numerically. The new treatment makes more direct use of the accurately measurable drop width than do the classical treatments based on the analysis of Bashforth and Adams.
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