Distribution over the radius of the plasma flow velocities v0 in the magnetosheath and magnetospheric convection velocity for different velocities of the solar wind.
We set such a plasma density distribution over the radius that its maximum is reached on the axis of the plasma cylinder, falling to a minimum toward its boundary.
Fig. 7. Distribution over the radius of the characteristic time τ needed for the asymptotic regime of the magnetospheric convection to set in for different solar wind velocities in the magnetosheath.
Figure 7 shows the distribution over the radius of the characteristic time τ needed for the asymptotic regime to set in in the geotail plasma flow, as calculated using formula (23), in which the diffusion coefficient is determined by (21), and the spectrum of FMS fluctuations in the magnetosheath (24) corresponds to the plasma flow profiles in Fig. 6(b).
This paper investigates the effects of draw die geometry on the sheet metal tool wear distribution over the draw die radius using numerical and experimental methods.
Rotation θ* is transmitted using a uniform distribution over a circle whose radius rθ* is the farthest distance of an interior point of the ideal model from the axis of rotation.
We tested this effect by providing various initial guesses to the algorithms, in the form of a homogeneous centered permittivity and conductivity distribution over a circular region of radius 6 cm.
In this paper we describe a 3D micro-CT and pore partitioning study to derive pore scale parameters including pore radius distribution, accessible radius, throat radius, and connectivity over the pore space of the tissue engineered constructs.
The reservoir characteristic curves include the pore radius distribution, throat radius distribution, pore throat radius ratio, and capillary pressure.
RP only uses data from the anterior surface whereas TCP uses data from the total cornea (anterior and posterior) over radius from 0.5 mm to 2.0 mm radius.
