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A
microstrip periodic structure behaves like a magnetic screen near
resonance. Defined as a ratio of strength of a
reflected to strength of an incident electric field, a reflection coefficient
value equals +1 at a resonance. Far from resonance the reflection coefficient
is close to –1 and a microstrip structure behaves like a dielectric-coated
ideal metal screen. It is possible to design a microstrip periodic structure
formed of curved narrow particles which when stretched are much longer than
the structure periods. As a result resonance occurs on the wavelength that
is much longer than the array periods. |
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The frequency dependence of reflection coefficients
of a microstrip array formed by C-shaped metal particles near the lowest
resonance frequency is shown in the Figure below as an example. The
parameters of the strip are a=4 mm, f =15 degrees, 2w=0.5 mm. Array periods are
identical and are 10 mm long, substrate permittivity is 3 and substrate
thickness equals to 1.5 mm. The surface admittance
where |
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References Prosvirnin
S.L., Analysis of electromagnetic wave scattering by plane periodical array
of chiral strip elements, Proceedings of 7-th Intern. Conf. on Complex
Media “Bianisotropics-98”, Technische Universitat Braunschweig, Germany,
3-6 June 1998, p. 185-188. Prosvirnin S.L.,
Transformation of polarization when waves are reflected by a microstrip array
made of complex-shaped elements, Journal of Communications Technology and
Electronics, 1999, vol. 44, no. 6, p. 635-639. Russian version: Просвирнин С.Л., Преобразование поляризации при отражении волн микрополосковой решеткой из элементов сложной формы, Радиотехника и электроника, 1999, т.44, 6, 681-686. |
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