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1 Ω⋅m for the Reference resistivity
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Dielectric losses: uses the constitutive relation D = ε0(ε' − jε")E. Specify that the Relative permittivity (real part) ε' (dimensionless) and the Relative permittivity (imaginary part) ε" (dimensionless) must be taken From material or be User defined. For User defined, select Isotropic, Diagonal, Symmetric, or Full and enter values or expressions in the field or matrix. The default is 1. Note that the material parameters Relative permittivity (real part) ε' and the Relative permittivity (imaginary part) ε" form the complex relative permittivity εr = ε' – jε''. The time-harmonic Sign Convention requires a lossy material to have a positive material parameter ε''.
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Loss tangent, loss angle: uses the constitutive relation D = ε0ε'(1 − jtanδ)E. Specify the Relative permittivity (real part) ε' (dimensionless) and Loss angle δ (SI unit: rad).
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Loss tangent, dissipation factor: uses the constitutive relation D = ε0ε'(1 − jtanδ)E. Specify the Relative permittivity (real part) ε' (dimensionless) and the Dissipation factor tanδ (dimensionless).
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Dispersion to use the constitutive relation D = ε0E + P(E, εrS), where the polarization vector is calculated from the electric field using the dielectric dispersion model. This option is available only when the Material type is set to Solid. You enter the Relative permittivity εrS (dimensionless) values From material. For User defined, select Isotropic, Diagonal, or Symmetric and enter values or expressions in the field or matrix. This value of electric permittivity will be used in stationary study, for which the polarization vector is calculated as P = ε0(εrS − Ι)E.
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Once this option is selected, a subnode Dispersion will become available under the Current Conservation node. At that subnode, you can select the dispersion model, enter the corresponding parameters, and choose how the relative permittivity input on the parent node will be interpreted in Eigenfrequency, Frequency Domain, and Time Dependent studies.
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