scholarly journals A complete equation of state for non-ideal condensed phase explosives

2017 ◽  
Vol 122 (22) ◽  
pp. 225112 ◽  
Author(s):  
S. D. Wilkinson ◽  
M. Braithwaite ◽  
N. Nikiforakis ◽  
L. Michael
2005 ◽  
Vol 98 (5) ◽  
pp. 053514 ◽  
Author(s):  
B. L. Wescott ◽  
D. Scott Stewart ◽  
W. C. Davis

2012 ◽  
Vol 710 ◽  
pp. 166-194 ◽  
Author(s):  
J. A. Saenz ◽  
B. D. Taylor ◽  
D. S. Stewart

AbstractWe use the weak-curvature, slow-time asymptotics of detonation shock dynamics (DSD) to calculate an intrinsic relation between the normal acceleration, the normal velocity and the curvature of a lead detonation shock for self-sustained detonation waves in condensed phase explosives. The formulation uses the compressible Euler equations for an explosive that is described by a general equation of state with multiple reaction progress variables. The results extend an earlier asymptotic theory for a polytropic equation of state and a single-step reaction rate model discussed by Kasimov (Theory of instability and nonlinear evolution of self-sustained detonation waves. PhD thesis, University of Illinois Urbana-Champaign, Urbana, Illinois) and by Kasimov & Stewart (Phys. Fluids, vol. 16, 2004, pp. 3566–3578). The asymptotic relation is used to study the dynamics of ignition events in solid explosive PBX-9501 and in porous PETN powders. In the case of porous or powdered explosives, two composition variables are used to represent the extent of exothermic chemical reaction and endothermic compaction. Predictions of the asymptotic formulation are compared against those of alternative DSD calculations and against shock-fitted direct numerical simulations of the reactive Euler equations.


2019 ◽  
Vol 45 (3) ◽  
pp. 374-386 ◽  
Author(s):  
Kibaek Lee ◽  
Alberto M. Hernández ◽  
D. Scott Stewart

Author(s):  
Prabal Adhikari ◽  
Jens O. Andersen ◽  
Patrick Kneschke

Abstract In this paper, we calculate the equation of state of two-flavor finite isospin chiral perturbation theory at next-to-leading order in the pion-condensed phase at zero temperature. We show that the transition from the vacuum phase to a Bose-condensed phase is of second order. While the tree-level result has been known for some time, surprisingly quantum effects have not yet been incorporated into the equation of state.  We find that the corrections to the quantities we compute, namely the isospin density, pressure, and equation of state, increase with increasing isospin chemical potential. We compare our results to recent lattice simulations of 2 + 1 flavor QCD with physical quark masses. The agreement with the lattice results is generally good and improves somewhat as we go from leading order to next-to-leading order in $$\chi $$χPT.


2013 ◽  
Vol 252 ◽  
pp. 163-194 ◽  
Author(s):  
Stefan Schoch ◽  
Kevin Nordin-Bates ◽  
Nikolaos Nikiforakis

2008 ◽  
Vol 47 (31) ◽  
pp. 5767 ◽  
Author(s):  
C. M. Wynn ◽  
S. Palmacci ◽  
R. R. Kunz ◽  
K. Clow ◽  
M. Rothschild

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