Meshfree particle model for kinetic plasma simulations
POSTER
Abstract
We revisit a meshfree particle model for kinetics of a 1D electrostatic
plasma, using kernel density estimation and a similar method for the electric
field E. The kernel K(x − y) represents the macroparticle charge distribution.
Two length scales enter, the width w of K and the interparticle spacing λ. This
model conserves momentum and energy. Similarly, continuity is satisfied exactly,
and the Gauss’s law and Ampere’s law formulations are exactly equivalent. A
unified analysis is used for numerical stability and noise properties. The force
can be computed directly using the convolution K2 = K ∗ K, and K2 is positive
definite. We discuss the analogy in the presence of a grid. We can specify a
single kernel Kp , related to the `kernel trick’ of machine learning. Numerical
instability can occur unless Kp is positive definite, related to a breakdown in
energy conservation. For the noise analysis, the covariance matrix for the electric field shows a plasma dispersion function modified by w and λ. The number of particles per cell does not enter, and the noise is characterized by the number of particles per kernel width, i.e. w/λ. We present the bias-variance optimization (BVO) for the electric field, and compare it to the density BVO.
plasma, using kernel density estimation and a similar method for the electric
field E. The kernel K(x − y) represents the macroparticle charge distribution.
Two length scales enter, the width w of K and the interparticle spacing λ. This
model conserves momentum and energy. Similarly, continuity is satisfied exactly,
and the Gauss’s law and Ampere’s law formulations are exactly equivalent. A
unified analysis is used for numerical stability and noise properties. The force
can be computed directly using the convolution K2 = K ∗ K, and K2 is positive
definite. We discuss the analogy in the presence of a grid. We can specify a
single kernel Kp , related to the `kernel trick’ of machine learning. Numerical
instability can occur unless Kp is positive definite, related to a breakdown in
energy conservation. For the noise analysis, the covariance matrix for the electric field shows a plasma dispersion function modified by w and λ. The number of particles per cell does not enter, and the noise is characterized by the number of particles per kernel width, i.e. w/λ. We present the bias-variance optimization (BVO) for the electric field, and compare it to the density BVO.
Presenters
-
John M Finn
Los Alamos Natl Lab
Authors
-
John M Finn
Los Alamos Natl Lab
-
Evstati G Evstatiev
Sandia National Laboratories