For more conventional structures, however, the roles of material, cross-section and boundary conditions are all comparatively small in allowing frequencies.
The matrix material, cross section of optical fiber, and the interface between fiber and matrix were analyzed by SEM.
The power per thermoelectric material cross section area ranged from 1 to 3 W cm−2.
By integrating the element areas of the bulk material cross section, a mathematical model to calculate the flow rate of bulk materials on moving belt is established.
A shear stress is defined as the component of stress coplanar with a material cross section; it arises from the force vector component parallel to the cross section.
Important parameters are nail diameter, nail material, cross-section (open vs. closed) and design of the screw/nail interface.
The measured mechanical properties, the morphology of the material cross-section, the fibre volume fractions, etc., were mutually correlated, and the results were used for determining the most appropriate forming condition.
Different ways of calculating the material cross-sections are compared as well.
The elastic wing is modelled by a generalized Timoshenko-type beam with six degrees of freedom for a material cross-section.
An efficient, finite elements (FE) based method of cross-sectional analysis of a longitudinally homogeneous beam, with an arbitrary cross section and material model assumed, submitted to tension/compression, bending, torsion, and shear is developed.
