Measurement and Simulation of Vector Hysteresis Characteristics
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1 Measurement and Smulaton of Vector Hsteress Characterstcs Mklós Kuczmann Laborator of Electromagnetc Felds Department of Telecommuncaton Széchen István Unverst Gır, Hungar Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds
2 Outlne Rotatonal Sngle Sheet Tester Arrangement Sensors Results Vector Presach model Model descrpton Identfcaton Comparsons Applcaton n Fnte Element Method Fxed pont method Results Conclusons Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds
3 Block Dagram of the RRSST Sstem RRSST Round shaped Rotatonal Sngle Sheet Tester Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds
4 Constructon of H-sensors 4 bakelte flans z N H = 810 H (t ) = H µ0 S H N H x t u(τ ) dτ 0 Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds Lnear extrapolaton d 2 H1 d1 H 2 H ( z = 0) = d 2 d1 1
5 The RRSST Sstem Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds
6 Measured Results F 1 ( α, β ) = ( H H ) 2 α αβ Everett functon from concentrc mnor loops 2D splne approxmaton Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds
7 Measured Results Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds
8 Measured Results Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds
9 Inverse Vector Presach Model π 2 n H ( t) = eϕ B{ Bϕ } dϕ H ( t) e B ϕ { B } ϕ π 2 B = B e + B e x Bϕ x = B x cos ϕ + B = 1 snϕ ( cosϕ ) cosϕ sgn( snϕ ) ϕ 1/ w Bϕ = B x sgn + B snϕ H H x = = n = 1 n = 1 H H ϕ ϕ cosϕ snϕ B H = H e + H x ( cos[ ϕ + ψ ]) cos[ ϕ + ψ ] + sgn( sn[ ϕ + ψ ]) sn[ ϕ ψ ] ϕ = B x sgn B + Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds x e
10 F Inverse Vector Presach Model π 2 n ( α β ) = cosϕ E( α cos ϕ, β cos ϕ) dϕ cosϕ E( α cos ϕ, β cos ϕ ) -π 2 = 1, ϕ measured unknown Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds
11 Inverse Vector Presach Model Intalzaton n=14, w=1, ψ=0 o Result: n=14, w=1.0894, ψ=1.3 o F Vector Everett functon π 2 ( α, β ) = cosϕ E( α cos ϕ, β cos ϕ) -π 2 dϕ ψ n Error Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds
12 Inverse Vector Presach Model Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds
13 Applcaton n FEM Reduced magnetc scalar potental, Φ Polarzaton technque Fxed pont method Inverse vector Presach model 3D Fnte Element Method prsm elements nodes unknown for T unknown for Φ Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds
14 Applcaton n FEM The average B s equal to B n the center. Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds
15 Applcaton n FEM The lnear extrapolaton can be used to calculate H at the surface. Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds
16 Conclusons, Future Works RRSST Sstem Sensor sstem, calbraton Controllng of flux Input data for the dentfcaton of vector Presach model Inverse vector Presach model Identfcaton technque Frequenc dependence Mnor loops Inserton nto 3D FEM Statc magnetc feld Edd current feld Other nonlnear problems and applcatons Mklós Kuczmann, Ph.D. Széchen István Unverst, Laborator of Electromagnetc Felds
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