- Page 1 and 2: Finite Element Method Magnetics Ver
- Page 3 and 4: 2.3.10 Line Integrals . . . . . . .
- Page 5 and 6: 3.7.8 View Commands . . . . . . . .
- Page 7 and 8: The purpose of this document is to
- Page 9 and 10: and the constitutive relationship,
- Page 11 and 12: − ∇ ·(k∇T) = q (1.24) FEMM s
- Page 13: 1.3.2 Heat Flow BCs There are six t
- Page 17 and 18: 2.2.2 Keyboard and Mouse Commands A
- Page 19 and 20: Point Mode Action Function Left But
- Page 21 and 22: 2.2.6 Problem Definition The defini
- Page 23 and 24: yet been defined. Pushing the Add P
- Page 25 and 26: Figure 2.8: Boundary Property dialo
- Page 27 and 28: Figure 2.9: Block Property dialog.
- Page 29 and 30: “B” (flux density) column as in
- Page 31 and 32: constrained to run along a particul
- Page 33 and 34: conductor of interest and achieve s
- Page 35 and 36: as compared to a magnetostatic prob
- Page 37 and 38: appears as a green line on the post
- Page 39 and 40: Figure 2.21: X-Y Plot dialog. data
- Page 41 and 42: • Force from stress tensor. This
- Page 43 and 44: • Block cross-section area • To
- Page 45 and 46: While an integration of (2.16) theo
- Page 47 and 48: 2.4.1 Problem Definition Figure 2.2
- Page 49 and 50: Figure 2.26: Property Definition di
- Page 51 and 52: an unbounded solution region. For m
- Page 53 and 54: For fixed voltages, one could alter
- Page 55 and 56: 2.5.3 Vector Plots A good way of ge
- Page 57 and 58: some types of integrals; however, s
- Page 59 and 60: dF = 1 (D(E · n)+E (D · n) −(D
- Page 61 and 62: The second edit box is the Solver P
- Page 63 and 64: Figure 2.41: Boundary Property dial
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Figure 2.43: Materials Library dial
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2.7 Heat Flow Postprocessor The the
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Figure 2.49: When in doubt plots an
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2.8.1 Problem Definition Figure 2.5
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Figure 2.52: Property Definition di
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Materials Properties The Block Prop
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never have to call the mesher from
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• J.t Tangential current density
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2.10 Exporting of Graphics Figure 2
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• open("filename") Opens a docume
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- meshsize: size constraint on the
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- editaction 0 -nodes, 1 - lines (s
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- NStrands Number of strands in the
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The next parameter is the number of
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Type Definition 0 A · J 1 A 2 Magn
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• mo_getcircuitproperties("circui
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• mo_hidecontourplot() Hides the
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3.5.3 Object Labeling Commands •
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• mi createradius(x,y,r)turnsacor
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For an “Anti-Perodic” boundary
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• ei attachouterspace() marks all
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• eo getconductorproperties("cond
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If eo numcontours is -1 all paramet
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• hi setblockprop("blockname", au
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• hi movetranslate(dx,dy,(editact
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• hi deleteboundprop("boundpropna
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• hi detachouterspace() undefines
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• ho groupselectblock(n) Selects
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• ho maximize() maximizes the act
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automesh: 0 = mesher defers to the
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• ci seteditmode(editmode) Sets t
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e applied to the specified property
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3.10.1 Data Extraction Commands •
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graph, the command would be: co mak
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• co showdensityplot(legend,gscal
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Chapter 4 Mathematica Interface FEM
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Chapter 5 ActiveX Interface FEMM al
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preconditioner must also be stored.
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Bibliography [1] M. Plonus, Applied
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Appendix A Appendix A.1 Modeling Pe
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Figure A.3: Shifting the B-H curve
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Figure A.5: Equivalent circuit for
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non-laminated materials as well, si
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Figure A.7: Air-cored coil with “
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The next step is to transform (A.19
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Figure A.9: Solved problem. ear tim