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The incidence beam cone angle is of 17°, the incidence beam size depends on the incidence angle, and it is however smaller than 10 mm, being the sample cup/reference diameter size for reflectance measurements.
Some particularities of the estimation of residual macrostresses in textured materials via the sin2ψ X-ray diffraction method realised in grazing incidence beam geometry are discussed.
Some important parameters of the grown oxide film namely: phase composition; lattice imperfections; and residual macro-stresses have been estimated via X-ray asymmetric grazing incidence beam methods.
The data consist of hourly global and diffuse solar radiation on a horizontal surface, normal incidence beam and global radiation on a south-oriented surface tilted at 40°.
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Focusing optics based on Wolter optical geometries developed for X-ray grazing incidence beams can be designed for neutron beams.
As plotted in Fig. 3(c), for normal incidence as the incident beam direction is perpendicular to the collagen fiber optic axis direction in the superficial zone but parallel in the deeper radial zone, the cumulative retardance tends to display a strong band near the surface and remain constant in the deeper region, an observation which is supported by EJMC simulation.
Angle of incidence of beam radiation.
The angle of incidence of beam radiation is 0° ≤ θ < 90°.
Below are the limitations of using Equation 3: (a) The angle of incidence of beam radiation is 0° ≤ θ < 90°.
Grazing incidence parallel beam optics was combined with side-inclination geometry using in-house designed sample stage to ensure results accuracy.
This figure also shows angles of incidence of beam (direct) solar radiation relative to the surface normal of horizontal and inclined planes on the Earth's surface, θz and θ, respectively.
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