200 likes | 241 Views
Explore properties of metamaterials in waveguide experiments to analyze refraction and resonators for various applications in electrical engineering studies. Investigate the behavior of waveguides filled with 2D uniaxial MNG materials beyond cutoff frequencies, focusing on metasurfaces and subwavelength resonators. Examine the impact of metamaterial configurations on wave propagation and demonstrate negative refraction phenomena in waveguide environments.
E N D
WAVEGUIDE EXPERIMENTS TO CHARACTERIZE PROPERTIES OF SNG AND DNG METAMATERIALS 學生 電機三 許宗堯 指導教授 吳瑞北
OUTLINE • review—rods , rings, rectangular waveguide… • rectangular waveguide of 2D uniaxial MNG • Subwavelength resonator • Refraction experiment
REVIEW • Thin-wire epsilon-negative metamaterials
REVIEW • SRR Array MNG metamaterials
REVIEW • Rectangular waveguide analysis
INVESTIGATION OF RECTANGULAR WAVEGUIDE FILLED WITH 2D UNIAXIAL MNG • 2D uniaxial MNG • Structure : • Below cutoff frequency, backward-wave propagation occurs.
In backward-wave propagation • due to energy conservation • so one concludes that any passive metamaterial can exhibit negative permeability only within the limited frequency band
Nine double rings were placed along the line of symmetry of a 60-mm-long section of a standard J-band waveguide (d = 35 mm) • Solid line, resonance frequency located below cutoff (a = 12 mm) dash line, resonance frequency located above cutoff (a = 35 mm)
WAVEGUIDE MINIATURIZATION • The classical constraint on the minimum transverse dimension of a waveguide does not hold in this case, that is, the waveguide width can be arbitrarily smaller than half of the wavelength in the filling material • The transverse dimension of this waveguide was approximately only 3.7 percent of half of the wavelength
SUBWAVELENGTH RESONATOR • combination of a DPS slab and a DNG slab sandwiched between two infinite conducting planes • The phase delay of the forward-wave can be completely compensated by the phase advance of backward-wave.
The conventional case: overall phase shift = π d>=0.5λ • With metamaterial, overall phase shift = 0 • Zin1 = Zin2
If d1 and d2 are much shorter than a wavelength • d1 and d2 can arbitrarily be shorter than the wavelength, provided that their ratio satisfies the above equation • Modeled by equivalent circuit
Solid line: measured phase distribution of H field • Dashed line: phase of standing wave • The length of the structure: approximately 0.1λ
REFRACITON EXPERIMENTS IN WAVEGUIDE ENVIRONMENTS • negative refraction • left-handed media are also referred to as negative refractive index or negative refractive media
REFRACTION EXPERIMENTS IN WAVEGUIDE ENVIRONMENTS • In this chapter, we consider transverse electric (TE) incident waves polarized in the y direction, so that the relevant parameters are (εy , µx , µz) in the dispersion relation: • First consider normal incident (transmission) • n2 is real, wave number is also real • n2 is pure imaginary, wave number is also pure imaginary → the wave is strongly attenuated inside the slab
Example : …… hyperbola when ω ↑ k0 ↑ ,so the radius of blue circle ↑ (εyμz) ↓ (εyμx) ↑ εy μx μz