2012
DOI: 10.1016/j.newast.2011.07.011
|View full text |Cite
|
Sign up to set email alerts
|

A natural symmetrization for the plummer potential

Abstract: We propose a symmetrized form of the softened gravitational potential which is a natural extension of the Plummer potential. The gravitational potential at the position of particle i (x i

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
4
0

Year Published

2012
2012
2021
2021

Publication Types

Select...
5
1

Relationship

2
4

Authors

Journals

citations
Cited by 10 publications
(4 citation statements)
references
References 32 publications
0
4
0
Order By: Relevance
“…I use a simulation code ASURA (Saitoh et al 2008, 2013, 8 in which a symmetric form of a Plummer softening kernel (Saitoh & Makino 2012), a parallel tree method with an computational accelerator GRAPE (GRAvity PipE, Makino 2004;Tanikawa et al 2013) and the second-order leap-frog integrator with individual timesteps are used. The number of stellar particles, 3 but for halo models different in rs and σ h .…”
Section: Settingsmentioning
confidence: 99%
“…I use a simulation code ASURA (Saitoh et al 2008, 2013, 8 in which a symmetric form of a Plummer softening kernel (Saitoh & Makino 2012), a parallel tree method with an computational accelerator GRAPE (GRAvity PipE, Makino 2004;Tanikawa et al 2013) and the second-order leap-frog integrator with individual timesteps are used. The number of stellar particles, 3 but for halo models different in rs and σ h .…”
Section: Settingsmentioning
confidence: 99%
“…It is fairly easy to incorporate higher-order multipole expansion terms into our method, and it would be a natural extension to the present work. Another good application of the tree method on a GPU would be to simulations that adopt a symmetrized Plummer potential (Saitoh & Makino, 2010). We believe that our method is the best for implementing that proposal, and hence that we shall certainly obtain better accuracy and good performance in simulating galaxy evolution and formation with different mass resolutions.…”
Section: Discussionmentioning
confidence: 99%
“…The CO is modeled as a point mass which interacts only gravitationally with other particles. We set gravitational softening lengths to prevent numerical divergences during close approaches to √ 2ǫ, ǫ, and 0 for gas-gas particles, gas-CO, and CO-CO interactions, respectively [36].…”
mentioning
confidence: 99%