The density of the magnetic vectors and the size of the magnetic vectors can be changed using the ‘Glyph Mode’ and ‘Scale Factor’ options respectively. The example magnetic state before and after adjustment is shown in Fig.20. Both can be adjusted in the Properties tab. The glyph object contains the magnetic vectors. The contour object is a surface which is taken at a specific level of helicity, and is used the show the core of magnetic vortices in the magnetic states. The two which can be used to control the visualisation are the ‘Contour1’ and ‘Glyph 1’ objects. This will load the magnetic states into the objects shown in Fig.19. The Properties tabs for both the Glyph1 (middle) and Contour1 (bottom) are also shown, with the editing options highlighted in red Using the arrows at the top of the window.įig.19 shows the Pipeline Browser with the two magnetic state objects, Contour1 and Glyph1, highlighted in red (top). tec files, for example in a hysteresis simulation, these mult_tec files will appear as a single option here, selecting this will open all of the magnetic states, which can then be cycled through. In the case that the simulation produces multiple.
Paraview point data contour windows#
tec file is selected, these windows are shown in Fig.18. Selecting the ‘…’ icon will open another prompt.
This loads the ‘Fix Paths in State File’ prompt. Here the ‘Takeshi X 0mT.pvsm’ should be chosen, not the. tec files are loaded using the ‘Load State…’ function. These can be visualised in Paraview, allowing the individual steps in any simulation to be analysed, whether these steps are steps in external field, temperature or different random states. tec files of each of the magnetic states at each simulation step. Micromagnetic simulations using MERRILL produces. Fig.17 shows the output of the Threshold function applied to the Mesh Quality output of the example mesh, low quality tetrahedra can be seen in dark red
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