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When performing a modeling task for any accelerator operation, the results of charged particle beam dynamics simulations must feed into the associated application. Thus, for a full simulation, one must include the codes in associated applications. For particle physics, the simulation may be continued in a detector with a code such as Geant4.
1986 – JMAG DYN was released including 3D transient magnetic field analysis. 1994 – JMAG-Works was released integrating electromagnetic and thermal analysis. 1998 – JMAG-Studio was released as an integrated electromagnetic analysis software native to Windows. 2000 – Coupled analyses were implemented for control simulation.
In February 2017, Algodoo for iPad was updated to version 2.1.2 to maintain functionality with iOS 10. Beginning in April 2024, Algoryx began releasing public betas for version 2.2.0, bringing 64-bit support to Windows, support for Apple Silicon, and fixes to several long-standing issues. [11]
Geant4 includes facilities for handling geometry, tracking, detector response, run management, visualization and user interface.For many physics simulations, this means less time needs to be spent on the low level details, and researchers can start immediately on the more important aspects of the simulation.
A neodymium magnet (also known as NdFeB, NIB or Neo magnet) is a permanent magnet made from an alloy of neodymium, iron, and boron to form the Nd 2 Fe 14 B tetragonal crystalline structure. [1] They are the most widely used type of rare-earth magnet .
2.4 GHz helical antenna radiation pattern (NEC simulation) The Numerical Electromagnetics Code, or NEC, is a popular antenna modeling computer program for wire and surface antennas. It was originally written in FORTRAN during the 1970s by Gerald Burke and Andrew Poggio of the Lawrence Livermore National Laboratory. The code was made publicly ...
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Magnetic induction B (also known as magnetic flux density) has the SI unit tesla [T or Wb/m 2]. [1] One tesla is equal to 10 4 gauss. Magnetic field drops off as the inverse cube of the distance ( 1 / distance 3 ) from a dipole source. Energy required to produce laboratory magnetic fields increases with the square of magnetic field. [2]