Changes

EM.Tempo

12 bytes removed, 02:48, 1 June 2015
/* Building the Physical Structure */
PEC and PMC materials do not have any constitutive material properties that you can modify except for their color or texture.
 
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[[Image:FDTD2.png|thumb|250px|EM.Tempo's PEC Dialog]]
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[[Image:FDTD3.png|thumb|250px|EM.Tempo's PMC Dialog]]
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[[Image:FDTD4.png|thumb|250px|Dielectric Material dialog]]
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[[Image:FDTD6.png|thumb|250px|[[FDTD Module]]'s Anisotropic Material dialog]]
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[[Image:FDTD8.png|thumb|250px|Debye Material Dialog]]
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===Dielectric Materials===
[[EM.Tempo]] allows you to define a general anisotropic material, whose constitutive [[parameters]], i.e. permittivity ('''&epsilon;'''), permeability ('''&mu;'''), electrical conductivity ('''&sigma;''') and magnetic conductivity ('''&sigma;<sub>m</sub>'''), are all tensorial in nature. Each constitutive parameter in this case is represented by a 3×3 matrix:
 |[[ImageFile:FDTD16.png|thumb|500px|]] 
A "'''Uniaxial'''" material is a special case of an anisotropic material whose constitutive [[parameters]] are all diagonal matrices. Specifying an anisotropic material as <u>'''Uniaxial'''</u> in the [[FDTD Module]] has a very important computational implication. There are six field update equations for uniaxial materials at each time steps: three for the electric field and three for the magnetic field. In this respect, a uniaxial material is similar to an isotropic dielectric material. On the other hand, a fully anisotropic material with non-zero off-diagonal constitutive matrix elements requires twelve update equations at each time step: three equations for the three components of each of the four vector fields '''E''', '''D''', '''H''' and '''B'''. As a result, the time loop for fully anisotropic materials takes much longer time than uniaxial materials.
===Dispersive Materials===
[[File:FDTD7.png|thumb|250px|Debye Add Pole Dialog]]
[[#Perfect Conductors|PEC]], [[#Perfect Conductors|PMC]], [[#Dielectric Materials|dielectric]] and [[#Anisotropic Materials|anisotropic]] materials are non-dispersive. In other words, their constitutive [[parameters]] do not vary with frequency. Most of the materials used in the design of RF and microwave circuits, antennas and systems fall into this frequency-independent category. However, there are other types of materials whose constitutive [[parameters]] exhibit frequency-dependent behaviors. [[EM.Cube]]'s [[FDTD Module]] currently offers four types of dispersive material:
where <math>\omega _p</math> and <math>\delta_p</math> are the angular resonant frequency and angular damping frequency corresponding to the p''th'' pole, respectively, and both are expressed in rad/s. Similar to a Debye material, <math>\Delta \varepsilon_p = \varepsilon_{sp} - \varepsilon_{\infty}</math> represents the change in permittivity due to the p''th'' pole.
{| border="0"|-| valign="top"|[[FileImage:FDTD7FDTD2.png|thumb|250px|EM.Tempo's PEC Dialog]]| valign="top"|[[Image:FDTD3.png|thumb|250px|EM.Tempo's PMC Dialog]]| valign="top"|[[Image:FDTD4.png|thumb|250px|Dielectric Material dialog]]| valign="top"|[[Image:FDTD6.png|thumb|250px|[[FDTD Module]]'s Anisotropic Material dialog]]| valign="top"|[[Image:FDTD8.png|thumb|250px|Debye Add Pole Material Dialog]]|-|}
===Geometrical Rules & Material Hierarchy===
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