128 lines
2.3 KiB
Plaintext
128 lines
2.3 KiB
Plaintext
[Format] = 4.0
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[Frequency] = 0
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[Precision] = 1e-008
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[MinAngle] = 25
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[Depth] = 5
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[LengthUnits] = millimeters
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[ProblemType] = planar
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[Coordinates] = cartesian
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[Comment] = "single low-E steel string (1.168 mm gauge, 25.5-inch scale). NdFeB bar magnets touch each end of the string with N faces facing inward. Flux is injected from both ends, the two flows cancel at the midpoint, producing a null point in the centre of the rod."
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[PointProps] = 0
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[BdryProps] = 1
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<BeginBdry>
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<BdryName> = "A=0"
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<BdryType> = 0
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<A_0> = 0
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<A_1> = 0
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<A_2> = 0
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<Phi> = 0
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<c0> = 0
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<c0i> = 0
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<c1> = 0
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<c1i> = 0
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<Mu_ssd> = 0
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<Sigma_ssd> = 0
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<EndBdry>
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[BlockProps] = 3
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<BeginBlock>
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<BlockName> = "Air"
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<Mu_x> = 1
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<Mu_y> = 1
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<H_c> = 0
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<H_cAngle> = 0
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<J_re> = 0
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<J_im> = 0
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<Sigma> = 0
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<d_lam> = 0
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<Phi_h> = 0
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<Phi_hx> = 0
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<Phi_hy> = 0
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<LamType> = 0
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<LamFill> = 1
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<NStrands> = 0
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<WireD> = 0
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<BHPoints> = 0
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<EndBlock>
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<BeginBlock>
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<BlockName> = "NdFeB"
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<Mu_x> = 1.05
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<Mu_y> = 1.05
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<H_c> = 915000
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<H_cAngle> = 0
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<J_re> = 0
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<J_im> = 0
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<Sigma> = 0.667
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<d_lam> = 0
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<Phi_h> = 0
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<Phi_hx> = 0
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<Phi_hy> = 0
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<LamType> = 0
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<LamFill> = 1
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<NStrands> = 0
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<WireD> = 0
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<BHPoints> = 0
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<EndBlock>
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<BeginBlock>
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<BlockName> = "Steel"
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<Mu_x> = 2500
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<Mu_y> = 2500
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<H_c> = 0
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<H_cAngle> = 0
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<J_re> = 0
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<J_im> = 0
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<Sigma> = 5.8
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<d_lam> = 0
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<Phi_h> = 0
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<Phi_hx> = 0
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<Phi_hy> = 0
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<LamType> = 0
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<LamFill> = 1
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<NStrands> = 0
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<WireD> = 0
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<BHPoints> = 0
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<EndBlock>
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[CircuitProps] = 0
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[NumPoints] = 16
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-100 -30 0 0
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750 -30 0 0
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750 30 0 0
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-100 30 0 0
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-30 -5 0 0
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-30 5 0 0
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0 -5 0 0
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0 -0.584 0 0
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0 0.584 0 0
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0 5 0 0
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647.7 -5 0 0
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647.7 -0.584 0 0
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647.7 0.584 0 0
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647.7 5 0 0
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677.7 5 0 0
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677.7 -5 0 0
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[NumSegments] = 18
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0 1 -1 1 0 0
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1 2 -1 1 0 0
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2 3 -1 1 0 0
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3 0 -1 1 0 0
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4 5 -1 0 0 0
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5 9 -1 0 0 0
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4 6 -1 0 0 0
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6 7 -1 0 0 0
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7 8 -1 0 0 0
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8 9 -1 0 0 0
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10 11 -1 0 0 0
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11 12 -1 0 0 0
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12 13 -1 0 0 0
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13 14 -1 0 0 0
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14 15 -1 0 0 0
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15 10 -1 0 0 0
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7 11 -1 0 0 0
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8 12 -1 0 0 0
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[NumArcSegments] = 0
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[NumHoles] = 0
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[NumBlockLabels] = 4
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325 20 1 -1 0 0 0 1 2
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-15 0 2 5 0 0 0 1 0
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662.7 0 2 5 0 180 0 1 0
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325 0 3 1 0 0 0 1 0
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