2015
DOI: 10.1063/1.4918537
|View full text |Cite
|
Sign up to set email alerts
|

Mass-velocity and size-velocity distributions of ejecta cloud from shock-loaded tin surface using atomistic simulations

Abstract: Abstract:The mass (volume and areal densities) versus velocity as well as the size versus velocity distributions of a shock-induced cloud of particles are investigated using large scale molecular dynamics (MD) simulations. A generic three-dimensional tin crystal with a sinusoidal free surface roughness (single wavelength) is set in contact with vacuum and shock-loaded so that it melts directly on shock. At the reflection of the shock wave onto the perturbations of the free surface, two-dimensional sheets/jets … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

1
21
0

Year Published

2016
2016
2022
2022

Publication Types

Select...
9
1

Relationship

1
9

Authors

Journals

citations
Cited by 64 publications
(22 citation statements)
references
References 41 publications
1
21
0
Order By: Relevance
“…Distinct defects may generate thin jets (which is sometimes referred to as microjetting) while a global roughness can lead to the expansion of a cloud of fine particles (sometimes called material ejection). Because this cloud may disrupt surface diagnostics used in shock physics (velocity interferometry, pyrometry, reflectivity) and because the impact of the ejecta can cause severe damage to nearby equipment in practical, engineering applications, this process has been widely studied both theoretically and experimentally under impact or explosive loading [1][2][3][4][5][6][7][8][9][10][11][12][13]. In a recent paper, we used laser driven shock loading to investigate microjetting from triangular, individual grooves of micrometric dimensions in several metals, both below and above shockinduced melting [14].…”
Section: Introductionmentioning
confidence: 99%
“…Distinct defects may generate thin jets (which is sometimes referred to as microjetting) while a global roughness can lead to the expansion of a cloud of fine particles (sometimes called material ejection). Because this cloud may disrupt surface diagnostics used in shock physics (velocity interferometry, pyrometry, reflectivity) and because the impact of the ejecta can cause severe damage to nearby equipment in practical, engineering applications, this process has been widely studied both theoretically and experimentally under impact or explosive loading [1][2][3][4][5][6][7][8][9][10][11][12][13]. In a recent paper, we used laser driven shock loading to investigate microjetting from triangular, individual grooves of micrometric dimensions in several metals, both below and above shockinduced melting [14].…”
Section: Introductionmentioning
confidence: 99%
“…For the first dynamic test of the auto-balancing algorithm, the ejection from a rough metal surface produced by shock wave arrival is chosen [25,26,27,28]. Surface grooves on metal may have small sizes of the order of 10-100 µm depending on experimental setup.…”
Section: Parallel Performance In Dynamic Tests With Materials In Extrmentioning
confidence: 99%
“…• Velocities and particle sizes are uncorrelated. This may only be true 23 for the high-velocity region of the spectrum (region visible to PDV). For the estimation of the optical extinction in each slab, a mean particle diameter d p and a mean extinction efficiency Q ext will be inferred from the size distribution.…”
Section: A a General Simulation Of Pdv Spectrogramsmentioning
confidence: 99%