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The linearized impact models proposed can be used to well describe the small-deflection responses for the system, based on 1-D wave propagations or the dependence of quasi-static band deflection on time if the impact duration is much longer than the double wave transit time for the band.
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Band-eliminated noises with relatively narrow eliminated bands caused smaller N1m (the most prominent negative deflection of the slow auditory evoked field) responses as compared to band-eliminated noises with wider eliminated bands; the N1m response was interpreted as reflection of the ipsi-lateral masking effect.
In this study, through an in situ bending experiment under a scanning electron microscope, the shear banding behavior and the bending stress-deflection response were investigated.
By tailoring the morphology of the crystalline second phase, one observes deflection, bifurcation and suppression of local shear bands and succeeds in enhancing the global plasticity of the composite structure.
The predicted failure loads and deflection capacities were within 3.2 and 14%% error band, respectively.
As shear band propagating stably, the flexural stress increases with increasing the deflection, which is similar to but analytically found different with the traditional "work-hardening" behavior of metallic crystalline materials.
To determine the deflection or absorption properties under specific light wavelengths, band-pass filters (Nikon, Tokyo, Japan) transmitting 365 400 nm (UV), 410 492 nm (blue), 470 560 nm (green) were individually attached to the light port of the microscope, and the transmitted light through the cells was recorded using an ultra-sensitive CCD camera (Roper Scientific CoolSNAP ES, Tucson, AZ, USA).
To measure the sub-band-gap absorption of the ZnO and ZnO N, a custom-built photothermal deflection spectroscopy system was used.
Lightly damped structures that have one or more natural modes of oscillation within the frequency band of transport excitations can experience considerable amplification of both the forces and deflections.
The new BMG, while having an unimpressive Poisson's ratio of 0.367, derives its high toughness from its high propensity for crack deflection and local loading-mode change at the crack tip due to extensive shear band interactions.
In general, the level of the narrow-band peaks reduced and the high frequency content increased as the gap, overlap, angle of attack and slat deflection increased separately or in combination.
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