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For a fixed size target, the maximum rotation angle for RD algorithm is: Θ R D = min 2 ρ r L X, λ L Y. (14).
Given the target size L X and L Y, the Keystone algorithm restricts the maximum rotation angle by: Θ Keystone = min 4 ρ r L Y, λ L Y. (15).
In order to avoid the MTRC, the maximum rotation angle for the RD algorithm in ISAR imaging should satisfy [2]: 1 ρ r ⋅ L X 2 Θ < 1 1 ρ a ⋅ L Y 2 Θ < 1, (13).
The range of external and internal rotation with the arm by the side of the body was measured beforehand so that the rotation cycle of the shoulder position for each subject could be computed in terms of shoulder rotation angle/ maximum rotation angle.
To avoid this phenomenon, the maximum rotation angle for PFA imaging is constrained as: Figure 3 Wavenumber spectrum for K R 2 cos Θ ≤ K R 1. Θ P F A = 2 cos - 1 K R 1 K R 2 = 2 cos - 1 1 - 0.5 μ 1 + 0.5 μ, (12).
The collision of the Izu-Bonin arc with the outer zone rocks of the Japanese arc has greatly deformed and rotated counterclockwise the Akaishi mountain range to the west of the ISTL, with a maximum rotation angle of 55° (Kano et al., 1990).
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Maximum rotation angles for all structure types with five axes are shown in Table 9.
For comparison, the maximum rotation angles for RD and Keystone are given below.
Maximum rotation angles for all structure types with those axes are shown in Tables 10 and 11, respectively.
In this subsection, the standard PFA algorithm will be introduced and the maximum rotation angles of PFA will be analyzed with comparison to RDA and Keystone algorithm.
For a LET joint design, we always expect k c to be small so as to lower the torsional stiffness in the desired direction for reducing actuation effort, and (tau_{c}) to be small to increase the maximum allowed rotation angle.
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