A boundary condition for Guderley's converging shock problem
Creators
- 1. University of Rochester, NY (United States)
- 2. Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)
Description
The Guderley model of a self-similar imploding shock based on the group invariance of the flow equations is a powerful tool in understanding the behavior of converging shock waves. Two modifications described here improve the predictions of observable quantities in spherical-shock wave experiments. First, a non-infinite boundary condition is established by the isentropic release of the outer pressure. Second, a two-temperature system of ions and electrons allows description of higher temperatures while conserving energy and without perturbing the overall hydrodynamics of the solution. Furthermore, these modifications of the Guderley model improve the prediction of the observables in laser driven spherical shock experiments in reference to a one dimensional (1-D) hydrodynamics code.
Availability note (English)
Available from https://www.osti.gov/servlets/purl/1581638; https://www.osti.gov/biblio/1581638; DOE Accepted Manuscript full text, or the publishers Best Available Version will be available free of charge after the embargo periodAdditional details
Identifiers
Publishing Information
- Journal Title
- Physics of Fluids (1994)
- Journal Volume
- 31
- Journal Issue
- 12
- Journal Page Range
- vp.
- ISSN
- 1070-6631
INIS
- Country of Publication
- United States
- Country of Input or Organization
- United States
- INIS RN
- 54046728
- Subject category
- S71: CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS;
- Descriptors DEI
- BOUNDARY CONDITIONS; EQUATIONS OF STATE; IONS; ISENTROPIC PROCESSES; ONE-DIMENSIONAL CALCULATIONS; SHOCK WAVES; SPHERICAL CONFIGURATION
- Descriptors DEC
- CHARGED PARTICLES; CONFIGURATION; EQUATIONS
Optional Information
- Contract/Grant/Project number
- NA0003856; SC0019269; AC52-07NA27344
- Funding organization
- USDOE National Nuclear Security Administration (NNSA) (United States)
- Secondary number(s)
- LLNL-JRNL--812593; OSTIID--1581638