By milling away half of each particle a cross-section was obtained, revealing the particle substrate interface.
A ∼1-mm-long belt with a rectangular cross section was obtained after 8 h of growth.
A considerable increase in the value of 2PA cross section was obtained when triple bonds were introduced and the dimensionality and chromophore density increased.
The numbers of Sertoli cells and interstitial areas in a cross-section were obtained from these images as well.
Substituting Equation 15 in Equation 16, the G-S equation for an elongated cross section is obtained where L r, θ) = R = R0 + r cos(θ + δ sin θ): L r, θ K 1 r, θ K 1 r, θ L r, θ ψ + K 2 r, θ 2 ψ = − μ 0 L 2 r, θ d P d ψ − 1 2 d F 2 d ψ Open image in new window (19).
Also, accurate and direct equations to determine the uniform flow depth in an egg-shaped cross section were obtained by using an alternative regression based model developed according to the concept of the relative hydraulic sensitivity.
This window becomes progressively smaller and more like the desired shape, pass after pass, until at the end, in the final pass, the specified cross section is obtained.
Simple correlation equations for optimum design of annular fins with uniform cross section are obtained in the present work.
According to the property of transmission line, one reduced (normal and bi-normal) galloping model, with regard of bending, rotation and eccentricity of cross section, is obtained.
Furthermore, solving the G-S equation with this new formulation, the exact solution for the magnetic surfaces of the tokomak plasma with elongated cross section is obtained.
The sagittal and coronal widths which corresponded to the vertical height (H) and base length (B) of the triangular cross section were obtained using sliding callipers.
