2019
DOI: 10.1088/1361-6463/ab2ab5
|View full text |Cite
|
Sign up to set email alerts
|

Numerical investigation of shock wave characteristics at microsecond underwater electrical explosion of Cu wires

Abstract: Strong shock wave (SW) can be generated during underwater electrical wire explosion as the exploding wire rapidly expands and pushes the surrounding water. In this paper, a coupled model that describes the behaviours of the circuit, the exploding wire, and the evolution of SW was established. Wide range equation of state data and conductivity data were used, making the calculation from solid state possible. The calculated discharge current, voltage, and trajectories of the wire radius and SW front were general… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

2
20
0

Year Published

2020
2020
2023
2023

Publication Types

Select...
6
1

Relationship

1
6

Authors

Journals

citations
Cited by 13 publications
(22 citation statements)
references
References 38 publications
2
20
0
Order By: Relevance
“…Thus, the maximum velocity for a 40 µm thick copper wire (see figure 10(a)) is 7500 m s −1 , while it is only 650 m s −1 for a 100 µm wire (see figure 11 High-pressure generation further than a few centimeters from the wire requires decreasing the peak pressure attenuation rate by choosing the optimal discharge related to the wire size (0.1 GPa in 4.3 mm from wire at 450 ns in figure 10(c)) or increasing the initial stored energy, otherwise low pressure like what happened in 100 µm EEW will occur. Furthermore, it confirms other research [10].…”
Section: Effects Of Wire Diametersupporting
confidence: 92%
See 2 more Smart Citations
“…Thus, the maximum velocity for a 40 µm thick copper wire (see figure 10(a)) is 7500 m s −1 , while it is only 650 m s −1 for a 100 µm wire (see figure 11 High-pressure generation further than a few centimeters from the wire requires decreasing the peak pressure attenuation rate by choosing the optimal discharge related to the wire size (0.1 GPa in 4.3 mm from wire at 450 ns in figure 10(c)) or increasing the initial stored energy, otherwise low pressure like what happened in 100 µm EEW will occur. Furthermore, it confirms other research [10].…”
Section: Effects Of Wire Diametersupporting
confidence: 92%
“…A general method for investigating the metal vapor content in an electrically initiated plasma was presented and verified by experiments. Other numerical simulations of the initial plasma formation (PF) in vacuum [9] or underwater [10] are also available. Still, to the authors' knowledge, the method for the calculation of the mixture ratio in high-pressure gases and supercritical fluids (SCFs) presented in this paper has not been published by other researchers so far.…”
Section: Guide To the Studymentioning
confidence: 99%
See 1 more Smart Citation
“…where j(z, r) is current density, σ(z, r) is the electrical conductivity, Q R represents the average radiation loss per unit volume (W m −3 ) which is adopted from [24] as a simplification to avoid detailed radiation transport within the exploding wire.…”
Section: Numerical Modelmentioning
confidence: 99%
“…More accurate description of UEWE process can be realized by magnetohydrodynamic (MHD) models. Many research institutions including Israel Institute of Technology [18], Imperial College London [19], Institute of High Current Electronics [20], Seoul National University [21], Tsinghua University [22] and Xi'an Jiaotong University [23,24] have developed their own MHD codes; general-purpose MHD codes such as JULIA [25] and ALEGRA [26] were also used to study the UEWE process. Generally speaking, previous studies were usually focused on the exploding wire, for example, to test the accuracy of metal equation of states (EOSs) and conductivity data, to clarify the evolution of the wire state and instabilities, etc, and few on SW characteristics.…”
Section: Introductionmentioning
confidence: 99%