Plate bending wave absorber
US-2022051650-A1 · Feb 17, 2022 · US
US11448281B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11448281-B2 |
| Application number | US-202017067102-A |
| Country | US |
| Kind code | B2 |
| Filing date | Oct 9, 2020 |
| Priority date | Oct 9, 2020 |
| Publication date | Sep 20, 2022 |
| Grant date | Sep 20, 2022 |
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Devices for superscattering a plate bending wave include a solid plate, and a circular array of spring-mass resonators positioned on a surface of the plate. All resonators in the circular array have a resonance frequency that can be matched to a frequency of a target flexural wave. The circular array has a diameter that can further be matched to the wavelength of the target flexural wave. Scattering efficiencies can exceed several multiples of the theoretical limit.
Opening claim text (preview).
What is claimed is: 1. A device for superscattering a flexural wave, the device comprising: a plate; and a circular array of spring-mass resonators positioned on the plate, the array having N degrees of rotational symmetry about a center point, where N is the number of resonators in the array. 2. The device as recited in claim 1 , wherein N is six. 3. The device as recited in claim 1 , wherein the plate has a minimum lateral dimension that is equal to or greater than six-times a diameter defined by the circular array of spring-mass resonators. 4. The device as recited in claim 1 , wherein each spring-mass resonator comprises: a spring portion connected to the plate and formed of a resilient element having a spring constant, k; and a mass portion supported by the spring portion and having a mass, m, wherein each spring-mass resonator has a resonance frequency, f 0 , according to an equation: f 0 = 1 2 π k m , and each spring-mass resonator of the plurality has substantially the same resonance frequency. 5. The device as recited in claim 4 , wherein each resonator of the circular array has substantially the same spring constant, k, and mass, m. 6. The device as recited in claim 1 , wherein each resonator of the circular array is substantially identical. 7. The device as recited in claim 1 , comprising a flexural wave source positioned on the plate at a distance from the circular array, and operable to generate a target flexural wave having wavelength, A, such that the target flexural wave propagates from the flexural wave source to the circular array, defining a propagation direction. 8. The device as recited in claim 7 , wherein each resonator of the circular array has a resonance frequency, f 0 , that corresponds to the wavelength, λ, of the target flexural wave by an equation: λ = 2 π D ρ t ( 2 π f 0 ) 2 4 , wherein ρ is plate density, t is plate thickness, and D is plate bending stiffness. 9. The device as recited in claim 7 , wherein the circular array defines a diameter, d, that is substantially equal to λ/2. 10. The device as recited in claim 7 , wherein the plate has a width, w, perpendicular to the propagation direction, the width being greater than or equal to 3λ. 11. A vehicle having a device for superscattering a flexural wave, the vehicle comprising: a structural plate of the vehicle; and a circular array of spring-mass resonators positioned on the plate, the array having N degrees of rotational symmetry about a center point, where N is the number of resonators in the array. 12. The vehicle as recited in claim 11 , wherein the structural plate is a floorboard. 13. The vehicle as recited in claim 11 , wherein the structural plate is a floor of an engine compartment. 14. The vehicle as recited in claim 11 , wherein the structural plate is a truck bed. 15. The vehicle as recited in claim 11 , wherein N is six. 16. The vehicle as recited in claim 11 , wherein the plate has a minimum lateral dimension that is equal to or greater than six-times a diameter defined by the circular array of spring-mass resonators. 17. The vehicle as recited in claim 11 , wherein each spring-mass resonator comprises: a spring portion connected to the plate and formed of a resilient element having a spring constant, k; and a mass portion supported by the spring portion and having a mass, m, wherein each spring-mass resonator has a resonance frequency, f 0 , according to an equation: f 0 = 1 2 π k m , and each spring-mass resonator of the plurality has substantially the same resonance frequency. 18. The vehicle as recited in claim 17 , wherein each resonator of the circular array has substantially the same spring constant, k, and mass, m. 19. The vehicle as recited in claim 11 , wherein each resonator of the circular array is substantially identical. 20. The vehicle as recited in claim 11 , comprising a flexural wave source positioned on the plate at a distance from the circular array, and operable to generate a target flexural wave having wavelength, λ, such that the target flexural wave propagates from the flexural wave source to the circular array, defining a propagation direction.
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