2016
DOI: 10.1016/j.pss.2016.04.007
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Surface motion relative to the irregular celestial bodies

Abstract: Abstract. We study the motion and equilibria of the grains on the surface of the irregular celestial body (hereafter called irregular bodies). Motions for the grains on the smooth and unsmooth surfaces are discussed, respectively. The linearized equations of motion relative to a surface equilibrium point and its characteristic equations are presented. Considering the stick-slip effect, the damping forces and the spring forces for the grain are calculated, then the linearized equations of motion and the charact… Show more

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Cited by 25 publications
(9 citation statements)
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“…In this study, an effective, parallel, three-dimensional N-body numerical code, Discrete Element Method (DEM) 10 , 20 , 39 , in which elastic spherical particles (i.e., soft-sphere) are described by linear-spring dashpot in conjunction with slider model, is carried out to simulate the impact process of various projectiles into granular regolith based on our previous work 40 . The motion of each particles is simultaneously calculated by taking into account whole mechanical interactions that occur when particles make contact, such as various kinds of friction, including rolling friction, which corresponds to the transformation of rotation energy into friction energy, and the normal and tangential deformation of colliding particles.…”
Section: Methodsmentioning
confidence: 99%
“…In this study, an effective, parallel, three-dimensional N-body numerical code, Discrete Element Method (DEM) 10 , 20 , 39 , in which elastic spherical particles (i.e., soft-sphere) are described by linear-spring dashpot in conjunction with slider model, is carried out to simulate the impact process of various projectiles into granular regolith based on our previous work 40 . The motion of each particles is simultaneously calculated by taking into account whole mechanical interactions that occur when particles make contact, such as various kinds of friction, including rolling friction, which corresponds to the transformation of rotation energy into friction energy, and the normal and tangential deformation of colliding particles.…”
Section: Methodsmentioning
confidence: 99%
“…Here λ represents the eigenvalues of the equilibrium point. There are several topological cases for the equilibrium point (Jiang et al 2016c). The most common cases are ordinary case O1, O2, O3 and O4.…”
Section: Gravitational Potential and Effective Potentialmentioning
confidence: 99%
“…The shape and gravitational model of minor celestial bodies can be modeled by the polyhedral model [3,[25][26][27] or the hard/soft-sphere discrete element method [10,[28][29][30]. Asteroid 433 Eros is elongated, and has both concave and convex areas on surface.…”
Section: Gravitational Potentialmentioning
confidence: 99%