.: E-Polarized Wave Scattering from from Infinitely Thin and Finitely Width Strip Systems |
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.: Results-Graphs- Animations
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Pictures:
- Near Field Pictures
• For one linear one curvy Strips - Plane Wave
According to theory if the distance between to obstacle is proportional to the wave length lambda, the system will goes to resonance.
a) Near Picture for Linear-Curvy Strips - Scattered Field Picture k=1 Plane
Wave Angle=0, L1=4PI,RL2=2PI, Arc=120degs from Origin, Mash=40x40
![](result_pictures4/Scatteredfield_L1_4PI_R2_2PI_arc120_range40x40_BW.jpg)
b) Near Picture for Linear-Curvy Strips - Total Field Picture k=1 Plane Wave Angle=0, L1=4PI,RL2=2PI, Arc=120degs from Origin, Mash=40x40 ![](result_pictures4/totalfield_L1_4PI_R2_2PI_arc120_range40x40_BW.jpg)
You can the wave trap for Curvy Strip and Linear Strip. If the Linear Strip is inside the range of Curvy Strips Origin, (and ofcource the Lambda has to be proportional to the Length of obstacles) we can keep the wave mostly inside our trap and it can keep on resonating. If this case is not created (if the linear strip is outside the range of curvy strips origin) wave will escape from trap. This can be imagine as a basic type wave trapper and open rezonator (resonator). c) Near Picture for Linear-Curvy Strips - Total Field Picture k=1 Plane Wave Angle=0, L1=4PI,RL2=2PI, Arc=120degs from Origin, Mash=40x40
Inside Origin Case: ![](result_pictures4/Scatteredfield_L1_4PI_R2_2PI_arc120_range40x40_insideorigin_BW.jpg)
d) Near Picture for Linear-Curvy Strips - Total Field Picture k=1 Plane Wave Angle=0, L1=4PI,RL2=2PI, Arc=120degs from Origin, Mash=40x40
Outside Origin Case: ![](result_pictures4/Scatteredfield_L1_4PI_R2_2PI_arc120_range40x40_outsideorigin_BW.jpg)
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