Search engine for discovering works of Art, research articles, and books related to Art and Culture
ShareThis
Javascript must be enabled to continue!

Explosive-driven Shock Wave Demagnetization of Nd 2 Fe 14 B Hard Ferromagnets

View through CrossRef
Abstract Magnetic materials subjected to shock wave compression will undergo shock wave demagnetization. To further investigate the demagnetization performance of Nd 2 Fe 14 B ferromagnets, an open magnetic circuit cylinder was used as the energy-carrying body. The discharge process and circuit characteristics during shock wave demagnetization were analyzed. A series of the shock wave demagnetization tests were performed using the shock wave from the detonation of high explosives acting along the axial direction of the cylindrical magnets. The induced electromotive force and current were measured. The results indicate that Nd 2 Fe 14 B ferromagnet begins to demagnetize at approximately 0.28 μs after the shock wave enters its body. The induced electromotive force and current in coils are caused by the destruction of the magnetism in the smallest units of magnetic domains rather than the mechanical damage of the magnet structure. The influence of the shock wave pressure on the effect of demagnetization was investigated by altering the pressure of the shock wave acting the magnets. The results show that Nd 2 Fe 14 B ferromagnets can be absolutely demagnetized and destroyed by a high shock wave pressure, and that demagnetization is insufficient under a low 13 GPa shock wave pressure. In order to reduce eddy current losses during the process of the shock wave demagnetization, a new design of a split magnet with insulation layers was proposed. This process is very effective and beneficial to improve the energy conversion during the shock wave demagnetization.
Title: Explosive-driven Shock Wave Demagnetization of Nd 2 Fe 14 B Hard Ferromagnets
Description:
Abstract Magnetic materials subjected to shock wave compression will undergo shock wave demagnetization.
To further investigate the demagnetization performance of Nd 2 Fe 14 B ferromagnets, an open magnetic circuit cylinder was used as the energy-carrying body.
The discharge process and circuit characteristics during shock wave demagnetization were analyzed.
A series of the shock wave demagnetization tests were performed using the shock wave from the detonation of high explosives acting along the axial direction of the cylindrical magnets.
The induced electromotive force and current were measured.
The results indicate that Nd 2 Fe 14 B ferromagnet begins to demagnetize at approximately 0.
28 μs after the shock wave enters its body.
The induced electromotive force and current in coils are caused by the destruction of the magnetism in the smallest units of magnetic domains rather than the mechanical damage of the magnet structure.
The influence of the shock wave pressure on the effect of demagnetization was investigated by altering the pressure of the shock wave acting the magnets.
The results show that Nd 2 Fe 14 B ferromagnets can be absolutely demagnetized and destroyed by a high shock wave pressure, and that demagnetization is insufficient under a low 13 GPa shock wave pressure.
In order to reduce eddy current losses during the process of the shock wave demagnetization, a new design of a split magnet with insulation layers was proposed.
This process is very effective and beneficial to improve the energy conversion during the shock wave demagnetization.

Related Results

Explosive-driven Shock Wave Demagnetization of Nd 2 Fe 14 B Hard Ferromagnets
Explosive-driven Shock Wave Demagnetization of Nd 2 Fe 14 B Hard Ferromagnets
Abstract Magnetic materials subjected to shock wave compression will undergo shock wave demagnetization. To further investigate the demagnetization performance of Nd...
Dynamics modeling and analysis of the permanent-magnet synchronous motors bearing-rotor-magnetic field under rotor demagnetize
Dynamics modeling and analysis of the permanent-magnet synchronous motors bearing-rotor-magnetic field under rotor demagnetize
For the phenomenon of rotor demagnetization of Permanent Magnet Synchronous Motor(PMSM), studying the dynamic modeling and analysis of demagnetization rotor. Firstly, considering t...
Generation and modulation of shock waves in two-dimensional polariton condensates
Generation and modulation of shock waves in two-dimensional polariton condensates
Due to the ability of exciton-polariton condensates formed in semiconductor microcavities to be achieved at room temperature and their characteristics such as non-equilibrium and s...
A CLINICAL STUDY OF THE EXTRACORPOREAL CARDIAC SHOCK WAVE THERAPY FOR CORONARY ARTERY DISEASE
A CLINICAL STUDY OF THE EXTRACORPOREAL CARDIAC SHOCK WAVE THERAPY FOR CORONARY ARTERY DISEASE
Objectives To evaluate the security and efficiency of extracorporeal cardiac shock wave therapy (CSWT) for treatment of coronary artery disease. ...
Numerical Modelling of Shock Initiation of a HNIW‐Based Explosive
Numerical Modelling of Shock Initiation of a HNIW‐Based Explosive
AbstractTo investigate shock‐to‐detonation transition (SDT) characteristics of a HNIW‐based explosive, a rate law based on the Forest Fire model was calibrated by conducting five w...
Hurricane Eloise Directional Wave Energy Spectra
Hurricane Eloise Directional Wave Energy Spectra
ABSTRACT Directiona1 wave energy spectra, calculated from data recorded during Hurricane Eloise (Gulf of Mexico, 1975), are presented. The spectra, based on an en...
Wave Force Calculations for Stokes and Non-Stokes Waves
Wave Force Calculations for Stokes and Non-Stokes Waves
ABSTRACT A new wave particle velocity procedure permits calculation of forces from regular wave profiles of more or less arbitrary wave crest to height ratios, as...
Blast Wave Mitigation Through Confined Volume and Porous Material
Blast Wave Mitigation Through Confined Volume and Porous Material
Abstract Over a period of time, the impact of shock waves on human bodies and structures has been studied. To understand the shock wave mitigation over confined volume and ...

Back to Top