Influence of shaped charge jet state on its interaction with ERA flying plate

The Explosive Reactive Armors (ERA) are really efficient at reducing Shaped Charge Jet (SCJ) performance. The main destabilizing mechanism is the transverse movement of the front and rear moving plates (MP) on the SCJ. Therefore, a good understanding of the interaction SCJ/MP is essential for improv...

Full description

Saved in:
Bibliographic Details
Main Authors: Nicolas Reboul, Ashwin Chinnayya, Frédéric Paintendre, Simon Dalle Piagge, Vincent Jaulin, Jérôme Limido, Anthony Collé, Fabien Rondot
Format: Article
Language:English
Published: KeAi Communications Co., Ltd. 2025-07-01
Series:Defence Technology
Subjects:
Online Access:http://www.sciencedirect.com/science/article/pii/S2214914725000819
Tags: Add Tag
No Tags, Be the first to tag this record!
_version_ 1839648345310625792
author Nicolas Reboul
Ashwin Chinnayya
Frédéric Paintendre
Simon Dalle Piagge
Vincent Jaulin
Jérôme Limido
Anthony Collé
Fabien Rondot
author_facet Nicolas Reboul
Ashwin Chinnayya
Frédéric Paintendre
Simon Dalle Piagge
Vincent Jaulin
Jérôme Limido
Anthony Collé
Fabien Rondot
author_sort Nicolas Reboul
collection DOAJ
description The Explosive Reactive Armors (ERA) are really efficient at reducing Shaped Charge Jet (SCJ) performance. The main destabilizing mechanism is the transverse movement of the front and rear moving plates (MP) on the SCJ. Therefore, a good understanding of the interaction SCJ/MP is essential for improving both weapon and armor systems. In a previous article, we have shown that interaction regimes are mainly influenced by the local collision geometry. Thus, in the collision point frame, the angle of collision between the continuous SCJ and the MP is a key parameter. This flow angle is acute for the Backward Moving plate (BMP) moving against the SCJ and obtuse for the Forward Moving Plate (FMP) moving alongside it. In the former, the jet is simply deflected, which is the regime 1 of deflection. In the latter, the interaction turns on an alternative creation of fragment and ligament, which is the regime 2. Fragments are parts of the jet that are only slightly deflected while ligaments are the curved material bridges that connect two consecutive fragments.When stretching, the jet is systematically subject to instabilities that disturb its surface, creating necks along it. Their growth finally leads to the jet fragmentation. In this article, we focus on this jet disturbance and its consequences on the SCJ/MP interaction.An experimental set-up was built to implement the interaction between a SCJ and a moving plate for different collision points, at different stand-off distances. The plate can interact with a smooth SCJ or a disturbed SCJ at a close and a far stand-off distance, respectively.One of the main results is the visualization of a regime change in SCJ/BMP interaction. A regime 1 (deflection) interaction changes into a ligament regime interaction (similar to a FMP regime 2) when the collision point stand-off is increased. It is proposed that this change can be attributed as the increase of the amplitude of the jet surface disturbances. This phenomenon is well captured by the γSPH simulations. Finally, using both experimental and numerical approaches, we propose a new detailed analysis of the different phenomena occurring during the interaction between a disturbed-surface jet and a moving plate. Interaction regime changes are linked to jet local geometry changes. The interactions of a BMP with a smooth SCJ or with a disturbed surface SCJ are geometrically not the same and, thus, generate different local flows and interaction mechanisms.However, some other simulations have been carried out with constant velocity jet whose surface has been previously disturbed. These simulations underline the influence of both disturbance wavelength λ and amplitude A on the interaction regimes.Surface disturbances of the SCJ, linked to its stretching, have a major influence on its interaction with a moving plate.
format Article
id doaj-art-080191401da547d3884fbd3d1ffb57a4
institution Matheson Library
issn 2214-9147
language English
publishDate 2025-07-01
publisher KeAi Communications Co., Ltd.
record_format Article
series Defence Technology
spelling doaj-art-080191401da547d3884fbd3d1ffb57a42025-06-29T04:52:04ZengKeAi Communications Co., Ltd.Defence Technology2214-91472025-07-0149355370Influence of shaped charge jet state on its interaction with ERA flying plateNicolas Reboul0Ashwin Chinnayya1Frédéric Paintendre2Simon Dalle Piagge3Vincent Jaulin4Jérôme Limido5Anthony Collé6Fabien Rondot7MBDA France, Le Plessis-Robinson, 92350, France; Institut Pprime, UPR 3346, CNRS, ISAE-ENSMA, Université de Poitiers, Poitiers, 6961, France; Corresponding author.Institut Pprime, UPR 3346, CNRS, ISAE-ENSMA, Université de Poitiers, Poitiers, 6961, FranceMBDA France, Le Plessis-Robinson, 92350, FranceMBDA France, Le Plessis-Robinson, 92350, FranceMBDA France, Le Plessis-Robinson, 92350, FranceABSTRAO, Plaisance-du-Touch, 31830, FranceABSTRAO, Plaisance-du-Touch, 31830, FranceISL, French-German Research Institute of Saint-Louis, Saint Louis, 68300, FranceThe Explosive Reactive Armors (ERA) are really efficient at reducing Shaped Charge Jet (SCJ) performance. The main destabilizing mechanism is the transverse movement of the front and rear moving plates (MP) on the SCJ. Therefore, a good understanding of the interaction SCJ/MP is essential for improving both weapon and armor systems. In a previous article, we have shown that interaction regimes are mainly influenced by the local collision geometry. Thus, in the collision point frame, the angle of collision between the continuous SCJ and the MP is a key parameter. This flow angle is acute for the Backward Moving plate (BMP) moving against the SCJ and obtuse for the Forward Moving Plate (FMP) moving alongside it. In the former, the jet is simply deflected, which is the regime 1 of deflection. In the latter, the interaction turns on an alternative creation of fragment and ligament, which is the regime 2. Fragments are parts of the jet that are only slightly deflected while ligaments are the curved material bridges that connect two consecutive fragments.When stretching, the jet is systematically subject to instabilities that disturb its surface, creating necks along it. Their growth finally leads to the jet fragmentation. In this article, we focus on this jet disturbance and its consequences on the SCJ/MP interaction.An experimental set-up was built to implement the interaction between a SCJ and a moving plate for different collision points, at different stand-off distances. The plate can interact with a smooth SCJ or a disturbed SCJ at a close and a far stand-off distance, respectively.One of the main results is the visualization of a regime change in SCJ/BMP interaction. A regime 1 (deflection) interaction changes into a ligament regime interaction (similar to a FMP regime 2) when the collision point stand-off is increased. It is proposed that this change can be attributed as the increase of the amplitude of the jet surface disturbances. This phenomenon is well captured by the γSPH simulations. Finally, using both experimental and numerical approaches, we propose a new detailed analysis of the different phenomena occurring during the interaction between a disturbed-surface jet and a moving plate. Interaction regime changes are linked to jet local geometry changes. The interactions of a BMP with a smooth SCJ or with a disturbed surface SCJ are geometrically not the same and, thus, generate different local flows and interaction mechanisms.However, some other simulations have been carried out with constant velocity jet whose surface has been previously disturbed. These simulations underline the influence of both disturbance wavelength λ and amplitude A on the interaction regimes.Surface disturbances of the SCJ, linked to its stretching, have a major influence on its interaction with a moving plate.http://www.sciencedirect.com/science/article/pii/S2214914725000819Shaped charge jet disturbancesSingle moving plateNecks and bumps and fragmentationγSPH simulations
spellingShingle Nicolas Reboul
Ashwin Chinnayya
Frédéric Paintendre
Simon Dalle Piagge
Vincent Jaulin
Jérôme Limido
Anthony Collé
Fabien Rondot
Influence of shaped charge jet state on its interaction with ERA flying plate
Defence Technology
Shaped charge jet disturbances
Single moving plate
Necks and bumps and fragmentation
γSPH simulations
title Influence of shaped charge jet state on its interaction with ERA flying plate
title_full Influence of shaped charge jet state on its interaction with ERA flying plate
title_fullStr Influence of shaped charge jet state on its interaction with ERA flying plate
title_full_unstemmed Influence of shaped charge jet state on its interaction with ERA flying plate
title_short Influence of shaped charge jet state on its interaction with ERA flying plate
title_sort influence of shaped charge jet state on its interaction with era flying plate
topic Shaped charge jet disturbances
Single moving plate
Necks and bumps and fragmentation
γSPH simulations
url http://www.sciencedirect.com/science/article/pii/S2214914725000819
work_keys_str_mv AT nicolasreboul influenceofshapedchargejetstateonitsinteractionwitheraflyingplate
AT ashwinchinnayya influenceofshapedchargejetstateonitsinteractionwitheraflyingplate
AT fredericpaintendre influenceofshapedchargejetstateonitsinteractionwitheraflyingplate
AT simondallepiagge influenceofshapedchargejetstateonitsinteractionwitheraflyingplate
AT vincentjaulin influenceofshapedchargejetstateonitsinteractionwitheraflyingplate
AT jeromelimido influenceofshapedchargejetstateonitsinteractionwitheraflyingplate
AT anthonycolle influenceofshapedchargejetstateonitsinteractionwitheraflyingplate
AT fabienrondot influenceofshapedchargejetstateonitsinteractionwitheraflyingplate