## Abstract This study demonstrates that the pex portion of a typical 42Β° conically lined shaped charge is not being efficiently utilized. In fact, approximately 40% of the liner height at the apex end of the cone does not provide an efficient jet as far as penetration depth is concerned. In this p
The Natural Spread and Tumbling of the Shaped Charge Jet Segments
β Scribed by E. Hirsch
- Publisher
- John Wiley and Sons
- Year
- 1981
- Tongue
- English
- Weight
- 853 KB
- Volume
- 6
- Category
- Article
- ISSN
- 0721-3115
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β¦ Synopsis
Abstract
The collapse mechanism of the shaped charge jet prevents the formation of a jet, the segments of which move in a straight line with absolute accuracy, even under the assumption that the shaped charge is ideally symmetrical. This is a result of the fact that the jet breakβup mechanism already starts at the collapse stage, in which the liner material has a big transversal velocity component.
A model for calculating the distribution of the angle by which the jet segments' direction of movement deviates from the shaped charge axis of symmetry (the spread angle) is presented in detail. The tumbling frequency of the segments as a function of their velocity and final length is also predicted by the theory.
The predictions made by applying the model to the standard 83.8 mm 42 degrees opening angle B.R.L. precision shaped charge were found to be consistent with the data published in open literature. The comparison of these predictions with the data leads also to the conclusion that the cutoff in the copper jet penetration into steel targets occurs when the jet segments start to hit the walls of the already formed hole instead of reaching its bottom without being disturbed on their way.
π SIMILAR VOLUMES
## Abstract It was found that the breakupβtime of jets formed by shaped charges of cylindrical symmetry is given very accurately by the formula: This formula is obtained from a general principal applied here for the first time which says that the breakupβtime of homogeneous ductile metals under v
This paper proposes a numerical method to simulate not only the jet formation process of the conical shaped charge with the inhibitor: approximately 11 km/s aluminum jet, but also the succeeding flight and impact processes onto the target plates. The method is demonstrated by performing a series of