Hello John Bordelon
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Posted:
1 decade ago
26.04.2012, 09:43 GMT-4
Cole-Cole permittivity models can be done in the following way on 4.2a
Under
Electromagnetic Waves -> Wave Equation -> Electric Displacement Field -> Electric Displacement Field Model
choose the "Dielectric Losses" option. This will activate the real and imaginary part of relative permittivity
requirement for material properties. You can then enter your cole-cole equations in the material parameters
epsilonBis and epsilonPrim. For example, muscle tissue can be modeled over the microwave band by these equations:
Real part
(55.32+1.0131763650973007E-8*freq^0.875+2.3290263939139233E-18*freq^1.75)/(1.+3.47871713338129E-10*freq^0.875+7.948895542368339E-19*freq^1.75)
Imaginary part
-(-1.3966655477570145E10-4.858604370585691*freq^0.875-1.1101948546745167E-8*freq^1.75-4.581162876363306E-8*freq^1.875)/(freq*(1.+3.47871713338129E-10*freq^0.875+7.948895542368339E-19*freq^1.75))
Be careful that you don't have a "conductivity" defined for the material that is redundant with the Cole Cole model.
I set conductivity to zero and put everything in epsilon. Also, the imaginary part of epsilon is actually the negative of the imaginary part. For most materials, epsilonBis should be a *positive* number in Comsol. Note the extra minus
sign in the formula above for the Imaginary part. Power dissipation should be positive in material. If you see negative power dissipation, you probably have the sign of the imaginary part of permittivity wrong.
As far as Gaussean pulse goes, it sounds to me like you should be using CST rather than COMSOL. Also, if
you use CST the Cole-Cole equations are built in for first and second order models. You just need to enter the parameters. And plane wave illuminations with absorbing boundaries are easier in CST.
But COMSOL makes nicer plots.
Cole-Cole permittivity models can be done in the following way on 4.2a
Under
Electromagnetic Waves -> Wave Equation -> Electric Displacement Field -> Electric Displacement Field Model
choose the "Dielectric Losses" option. This will activate the real and imaginary part of relative permittivity
requirement for material properties. You can then enter your cole-cole equations in the material parameters
epsilonBis and epsilonPrim. For example, muscle tissue can be modeled over the microwave band by these equations:
Real part
(55.32+1.0131763650973007E-8*freq^0.875+2.3290263939139233E-18*freq^1.75)/(1.+3.47871713338129E-10*freq^0.875+7.948895542368339E-19*freq^1.75)
Imaginary part
-(-1.3966655477570145E10-4.858604370585691*freq^0.875-1.1101948546745167E-8*freq^1.75-4.581162876363306E-8*freq^1.875)/(freq*(1.+3.47871713338129E-10*freq^0.875+7.948895542368339E-19*freq^1.75))
Be careful that you don't have a "conductivity" defined for the material that is redundant with the Cole Cole model.
I set conductivity to zero and put everything in epsilon. Also, the imaginary part of epsilon is actually the negative of the imaginary part. For most materials, epsilonBis should be a *positive* number in Comsol. Note the extra minus
sign in the formula above for the Imaginary part. Power dissipation should be positive in material. If you see negative power dissipation, you probably have the sign of the imaginary part of permittivity wrong.
As far as Gaussean pulse goes, it sounds to me like you should be using CST rather than COMSOL. Also, if
you use CST the Cole-Cole equations are built in for first and second order models. You just need to enter the parameters. And plane wave illuminations with absorbing boundaries are easier in CST.
But COMSOL makes nicer plots.