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explosive charge
The problem is considered concerning the breakdown of an arbitrary discontinuity, due to the emergence of a detonation wave at the boundary of a condensed explosive charge.
      
A comparison is carried out of the calculated values of the initial shock-wave velocities with the experimental data obtained at a certain distance from the explosive charge.
      
Gasdynamics of the scattering of the detonation products of a cylindrical explosive charge with inert metal particles
      
An Energy Source Based on a Spiral Magnetic-flux Compression Generator with Simultaneous Axial Initiation of an Explosive Charge
      
A spiral magnetic-flux compression generator with simultaneous axial initiation of an explosive charge is treated.
      
The effect of the thermophysical parameters of a cooling medium on the macrokinetics of secondary physicochemical processes that occur in a hermetic chamber after the explosion of a solid explosive charge is studied.
      
The electric field is assumed to be generated by charged dust grains produced during the explosion of a condensed chemical explosive charge.
      
The dependence of the detonation velocity on the detonation shock-front total curvature at the explosive charge axis is presented for steel and PVC detonation tubes of various inner diameters.
      
By means of pressure profiles of blast waves generated by the explosion, the limit between the two explosion phenomena (total and partial explosive charge) is defined.
      
We analyse the processes which occur when a planar detonation propagating from the fixed end of a donor explosive charge impacts on an acceptor homogeneous explosive.
      
These relationships allow determination of the parameters of a blast wave interacting with a structure as a function of the positions of the explosive charge and the structure.
      
CdS multiplings having more than three prisms were developed from the vapor generated from CdS powder by means of the conically converging shock-wave (CCSW) technique utilizing detonation of explosive charge.
      
Pressure-space-time history of shock waves due to the detonation of explosive charge in water is obtained by simulating the numerical integration of shock trajectory with the variation of fluid parameters behind the shock front.
      
The load was applied by detonating a small explosive charge inside a water filled, steel, cylindrical chamber enclosing the test specimen.
      
High-resolution simulations are then used to investigate thequalitative dependences of the detonation driving zone structure on the diameter and degree of confinement of the explosive charge.
      
From a purely mechanical viewpoint, each explosive charge should produce a peak blasthole pressure (Pb) that just fails to crush (i.e.
      
Blast vibration and its attenuation within the rock mass immediately adjacent to a blast hole (2-15 m) were monitored for a blast hole diameter of 100 mm and a 2.4 m column of an emulsion explosive charge.
      
The using of FEM and especially LS-DYNA3D code for the simulation of a heat transfer during the heating of the explosive charge is discussed in this paper.
      
Inside the sphere we place a small explosive charge (two detonators) to destabilize the glass wall.
      
Variation of the impulse transmitted to the surface of a barrier in the vicinity of an explosive charge
      
 

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