Table 7 Scaffold simulation steps (Luo et al. 2014) Step Detail Description 1 Crimp Rigid cylindrical tube to simulate a crimp tool (3.5 mm ➔ 1.5 mm) 2 Elastic recoil Removal of rigid cylindrical tube 3 Expansion Rigid cylindrical body denoting balloon catheter (➔ 3.2 mm inner radius) 4 Elastic recoil Removal of rigid cylindrical tube.
end{aligned} (29) Summarizing, the mixed initial boundary value problem for the three-phase-lag dipolar thermoelastic bodies, denoted by ({mathcal {P}}), is given by the geometric equations (1), the constitutive equations (14), (18) and (22), the equation of motion (25), the initial conditions (23) and the boundary conditions (24).
The polar body of a convex body K, denoted by (K^{ast}), is another convex body defined by (K^{ast}={y: xcdot yleq1mbox{ for all } xin K}).
(2.7) The body C, denoted by (Ksharp L ), is called the Blaschke sum of K and L. For Blaschke addition, a counterpart to the Brunn-Minkowski inequality, is the following: V(Ksharp L ^{frac{n-1}{n}}geq V(K)^{frac{n-1}{n}}+ V(L ^{frac{n-1}{n}}geq.8) with equality if and only if K and L are homothetic.
The spinel cobalt ferrite has a cubic symmetry, and it has six crystallographic easy axes (directions) along the cube edges of the crystal, represented as <100>, and four crystallographic hard axes (directions) across the body diagonals denoted as <111> [5, 6, 7].
The CoM position of the whole body is denoted by ({varvec{p}}_{mathrm {CoM}}) (see "Target CoM position generation" section), while ({varvec{p}}_{mathrm {swing}}) and ({varvec{R}}_{mathrm {swing}}) are the position and the orientation of the foot sole in the swing leg, ({varvec{R}}_{mathrm {torso}}) is the orientation of the torso link, and ({varvec{J}}) is the Jacobian matrix of the lower body.
The force applied to the body is denoted by F, and δ represents the displacement produced by the force.
Three sets of rigid body calculations, denoted as CORAL set 1, CORAL set 2, and CORAL decoy set, were performed as follows.
