This paper is concerned with the decay of Saint-Venant end effects for plane deformations of piezoelectric (PE)-piezomagnetic (PM) sandwich structures, where a PM layer is located between two PE layers with the same material properties or reversely. The end of the sandwich structure is subjected to a set of self-equilibrated magneto-electro-elastic loads. The upper and lower surfaces of the sandwich structure axe mechanically free, electrically open or shorted as well as magnetically open or shorted. Firstly the constitutive equations of PE mate- rials and PM materials for plane strain are given and normalized. Secondly, the simplified state space approach is employed to arrange the constitutive equations into differential equations in a matrix form. Finally, by using the transfer matrix method, the characteristic equations for eigen- values or decay rates axe derived. Based on the obtained characteristic equations, the decay rates for the PE-PM-PE and PM-PE-PM sandwich structures are calculated. The influences of the electromagnetic boundary conditions, material properties of PE layers and volume fraction on the decay rates are discussed in detail. 相似文献
Combination of thermochromism of perovskite-type materials and gratings can result in some interesting variations of the spectral properties of structured surfaces. This paper aims at investigating thermal absorptive/radiative characteristics of structured thermochromic material La0.825Sr0.175MnO3 (LSMO) with metallic and/or dielectric gratings. Numerical computation is conducted to obtain the distribution of the spectral absorptance of such structured surfaces with different structural parameters. The directional and temperature dependence of absorptance are also analyzed. The results reveal that compared with bulk LSMO material, the structured surface of LSMO achieves an improved thermochromic performance and much thinner layer of a structured LSMO film by combining the film with one-dimensional Al and SiO2 gratings. Therefore, the other advantage of such structured surface is that the reduction of material consumption and weight is achieved due to the smaller LSMO layer thickness, which may be vital for thermal management of space vehicles. 相似文献
Polyethylene terephthalate (PET) and polyethylene naphthalate (PEN) are both good candidates for use as scintillation base substrates. One advantage is their relatively high density of 1.33 g cm−3. To enhance their relative strengths and to mitigate their weaknesses, we blended PET and PEN 1:1 by weight and found that the overall characteristics are improved. The wavelength at maximum emission was 415 nm, the refractive index was 1.61, and the light yield was 0.85 times that of PEN. These results increase the available options for base materials to be used as scintillators. 相似文献
This paper reports on the use of Auger electron spectroscopy (AES)/ depth profile analysis for the investigation of plasma-sprayed coatings. Prior to spraying the St 37 substrates are heated to 300 °C or 500 °C for ceramic or metallic layers, respectively. Studies of the starting materials and of the interfaces are important if the adhesion mechanism is to be understood. Therefore the initial components—the unheated and heated substrates and the powder particles NiCrAl, Al2O3 and ZrO2-7.25Y2O3—are analyzed. Depth profiles obtained from two coatings St 37/NiCrAl and St 37/Al2O3 show the influence of plasmaspraying on substrate surfaces and sprayed particles. Plasma-spraying mainly causes a decrease of superficial carbon contamination for both coating layers. In the case of St 37/NiCrAl incorporation of carbon in the sprayed layer is observed. The whole layer is almost completely oxidized except for some areas where substrate and particle material are present. It is assumed that these areas are identical with so-called adherence zones.Dedicated to Professor Günther Tölg on the occasion of his 60th birthday 相似文献
Previous detailed studies of the interaction of a shock wave with a perforated sheet considered the impact of a shock wave
on a plate with regularly spaced slits giving area blockages of 60 and 67%, at various angles of incidence, and resulting
in both regular and Mach reflection. The current work extends this study to a much wider variety of plate geometries. Blockage
ratios of 20, 25, 33, 50, and 67 and inclinations of 45, 60, 75, and 90° to the shock wave were tested. Four different thicknesses
of plate were tested at the same frontal blockage in order to assess the effects of gap guidance. Tests were conducted at
two shock Mach numbers of 1.36 and 1.51 (inverse pressure ratios of 0.4 and 0.5). It is found that secondary reflected and
transmitted waves appear due to the complex interactions within the grid gaps, and that the vortex pattern which is generated
under the plate is also complex due to these interactions. The angle of the reflected shock, measured relative to the plate,
decreases with plate blockage and the angle of inflow to the plate reduces with increasing blockage. By analysing the flow
on the underside of the plate the pseudo-steady flow assumption is found to be a reasonable approximation. Both the pressure
difference and the stagnation pressure loss across the plate are evaluated. It is found that over the range tested the plate
thickness has a minimal effect. 相似文献
The ENEA fast neutron dosemeter is based on a planar poly allyl diglicol carbonate (PADC) placed in a polyethylene holder. The present paper reports the results of an experimental study of a CR-39® material with the addition of 0.1% of dioctylphthalate (DOP) produced by the Italian company Intercast Europe S.p.A.
The etching procedure is: pre-etching with 40% KOH water solution 6.25 N and 60% ethyl alcohol at 70°C followed by 12 h of etching in 6.25 N KOH water solution. For the energy dependence of response, dosemeters have been irradiated with neutron sources (241Am–Be, 252Cf, Pu–Li) and 14.9 MeV monoenergetic neutrons. The dosimetric performance of the material for fast neutrons is expressed in terms of sensitivity, background value, lowest detectable dose and energy dependence of response. Moreover, the results of a quality acceptance test of the material, performed on 11 sheets (980×980 mm2, 1.4 mm thick) of the same production batch, are given. Therefore, the homogeneity of the neutron sensitivity and of the background signal within a sheet and the whole batch is considered. The results are compared with the acceptance test outcome for a CR39 standard material batch. 相似文献