$MaterialParameter

Format

$MaterialParameter
 typedis       N         εr,∞        μr          σE          σH
 par1(1)    par1(2)    par1(3)    par1(4)
 par2(1)    par2(2)    par2(3)    par2(4)
   .          .          .          .
   .          .          .          .
   .          .          .          .
 parp(1)    parp(2)    parp(3)    parp(4)
   .          .          .          .
   .          .          .          .
   .          .          .          .
 parN(1)    parN(2)    parN(3)    parN(4)                // where typedis and N are integers, but the others are floating points.

Refer to Chap. 9 at p.353 - p.368.
type_dis means the type of dispersive model. N means the number of poles in this material. ε_r,∞ is the relative permittivity at infinite frequency, μ_r is relative permeability, σ_E is electric conductivity, and σ_H is equivalent magnetic loss, respectively.

Models	typedis	parp(1)	parp(2)	parp(3)	parp(4)
non-dispersive	0	0	0	0	0
Debye	1	εs,p	ε∞,p	τp	0
Lorentz	2	εs,p	ε∞,p	ωp	δp
Drude	3	ωi	γp	0	0

$\epsilon (\omega )={\epsilon }_{\mathrm{\infty }}+\sum _{p=1}^P{\chi }_p(\omega )$

Debye model: ${\chi }_p(\omega )=\frac{({\epsilon }_{s,p}-{\epsilon }_{\mathrm{\infty },p})}{1+j\omega {\tau }_p}$

Lorentz model: ${\chi }_p(\omega )=\frac{({\epsilon }_{s,p}-{\epsilon }_{\mathrm{\infty },p}){\omega }_p^2}{{\omega }_p^2+2j\omega {\delta }_p-{\omega }^2}$

Drude model: ${\chi }_p(\omega )=-\frac{{\omega }_p^2}{{\omega }^2-j\omega {\gamma }_p}$

Example

$NumberofObject
 2
$MaterialParameter
 2 3 10 1 0 0
 10 7 1.2566e15 1e14
 10 7 2.5133e15 2e14
 10 7 3.7699e15 3e14

Related commands

Input file 1: $NumberofObject, $MaterialStructure

Input file 2: $Backgroundparameter