Broadband wave-absorbing metamaterial
A wave-absorbing material and broadband technology, which is applied in the field of broadband wave-absorbing superstructure materials, can solve the problems of narrow absorption frequency band, complex multi-layer structure design, and weak wave-absorbing ability, so as to reduce electromagnetic wave reflection and realize multifunctional structural integration , enhanced mechanical stability and environmental resistance
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Embodiment 1
[0046] The cell unit period of the metamaterial is 12mm, the thickness of the upper part of the gradient structure is 8mm, the outline can be conical, and the radius of the bottom of the surface gradient structure gradually increases along the direction of electromagnetic wave incident propagation, and the thickness of the lower part of the continuum is 8mm , the total thickness is 16mm. The metamaterial uses a single dielectric absorbing medium with a dielectric constant of 5.56 and a loss tangent of 0.4. The ratio of top diameter to cell period area of the upper gradient structure is 0.8, and the ratio of bottom diameter to cell period is 1.0. The reflectivity and effective absorptivity of periodic materials in the 4-18GHz wide frequency range are analyzed by finite element method, and the results are as follows figure 2 and image 3 shown. Depend on figure 2 It can be seen that the reflectivity of the periodic material is below -10dB in the wide frequency range of 4...
Embodiment 2
[0048] The dielectric constant of the metamaterial is 10, the loss tangent is 0.4, the thickness of the upper part of the gradient structure is 8mm, the shape is conical, and the radius of the bottom of the surface gradient structure increases gradually along the electromagnetic wave incident propagation direction, and the lower part is continuous The thickness of the medium is 8mm, and the total thickness is 16mm. The broadband reflection and absorbing properties of materials under two periodic structures were simulated and analyzed. One is that the cell period is 14mm, and the diameter of the gradient structure at the upper part of the electromagnetic wave incident end is 9.8mm, that is, the ratio of it to the period is 0.7; the other is that The cell period is 10mm, and the diameter of the gradient structure at the incident end of the upper part of the electromagnetic wave is 6.0mm, that is, the ratio of it to the period is 0.6. The result is as follows Figure 6 and Figu...
Embodiment 3
[0050] The dielectric constant of the metamaterial is 10, the loss tangent is 0.4, the thickness of the upper part of the gradient structure is 8 mm, and the outline is parabolic, and the radius of the bottom of the surface gradient structure increases gradually along the direction of electromagnetic wave incident propagation. Its shape is as follows: Figure 8 shown. The thickness of the lower part of the continuum is 10mm, and the total thickness is 18mm. The cell period is 14mm, and the diameter of the gradient structure at the incident end of the upper part of the electromagnetic wave is 5.6mm, that is, the ratio of it to the period is 0.4. The broadband reflection and absorbing performance of the metamaterial is simulated and analyzed, and the results are as follows Figure 9 and Figure 10 shown. It can be seen that the reflectivity of the periodic medium is below -10dB in the wide frequency range of 4-18 GHz, which can effectively reduce the reflection of the detectio...
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