2019
DOI: 10.1016/j.amc.2019.06.022
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Efficient energy-preserving methods for charged-particle dynamics

Abstract: In this paper, energy-preserving methods are formulated and studied for solving chargedparticle dynamics. We first formulate the scheme of energy-preserving methods and analyze its basic properties including algebraic order and symmetry. Then it is shown that these novel methods can exactly preserve the energy of charged-particle dynamics. Moreover, the long time momentum conservation is studied along such energy-preserving methods. A numerical experiment is carried out to illustrate the notable superiority of… Show more

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Cited by 12 publications
(14 citation statements)
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“…It is noted that Algorithm 2.1 is implicit, while the nonlinear equation (2.4) is independent of ε. Therefore, compared with other implicit energy-preserving schemes [4,20,33,34,36] for solving CPD (1.1), the computational cost of S1-AVF per time step is uniform in ε ∈ (0, 1]. To obtain an explicit scheme, we consider the following approximation.…”
Section: Methodsmentioning
confidence: 99%
See 2 more Smart Citations
“…It is noted that Algorithm 2.1 is implicit, while the nonlinear equation (2.4) is independent of ε. Therefore, compared with other implicit energy-preserving schemes [4,20,33,34,36] for solving CPD (1.1), the computational cost of S1-AVF per time step is uniform in ε ∈ (0, 1]. To obtain an explicit scheme, we consider the following approximation.…”
Section: Methodsmentioning
confidence: 99%
“…Among them, the Boris method [3] proposed in 1970 is still widely used by physicists, followed by some recent numerical analysis work [23,40] to address its mathematical property. Later on, many other structuralpreserving schemes have been designed, including the volume-preserving algorithm [28], the timesymmetric algorithm [24], the symplectic or K-symplectic algorithms [29,39,43,45,46], the Poisson integrators [30] and the energy-preserving algorithms [4,33,34].…”
Section: Introductionmentioning
confidence: 99%
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“…where the corresponding energy becomes H(x, v) = mv • v/2 + qϕ(x). Though several structure-preserving methods have been proposed for numerical solving (3.6), including symplectic methods [60,53], volumepreserving methods [46,34,26] and energy-conserving methods [41,9], with respect to the structures (…”
Section: Experiments Iii: 2d Charged Particle Dynamicsmentioning
confidence: 99%
“…In this paper, we are interested in investigating high-order numerical methods for solving the following charged particle dynamics [1][2][3][4]: q = p,ṗ = p × L(q) − ∇U(q), q(0) = q 0 , p(0) = p 0 , (q 0 , p 0 ) ∈ Ω ⊆ R 3 × R 3 , (1) where L(q) and −∇U(q) are, respectively, the magnetic and electric fields. In recent years, many energy-conserving numerical methods have been investigated within the framework of line integral methods [1,5] or Runge-Kutta methods [6][7][8][9].…”
Section: Introductionmentioning
confidence: 99%