Abstract

In this paper, the design of a new flexible ultra-thin curvature metasurface energy harvester is presented. The use of cylindrical metasurface electromagnetic (EM) harvester would be desirable for the ambient EM energy harvesting since it can absorb the EM energy with maximum efficiency. The harvester is made by an 11×11 unit-cell metasurface with a flexible substrate to demonstrate the 2D-isotropic harvesting; as a small slice of the cylinder. We have proposed a sub-wavelength (∼0.13λ0) complementary quad split ring resonator (CQSRR) unit-cell which is loaded with a lump resistor mounted on the metal-backed substrate. The full-wave simulation shows that the efficiency of the flat metasurface energy harvester with thickness of 0.004λ0 at 5.33 GHz (WiFi) is up to 0.86 for normal radiation. It is 0.72 and 0.62 for 70° oblique angle of incidence from H- and E-plane. In addition to this, the experimental results show an agreement with the results of full-wave simulations. Due to the non-uniform mutual coupling between the cells in the finite array of the fabricated energy harvester and efficiency definition for the central cell as a metric of evaluating the device performance, an effective area for the central cell has been obtained experimentally which is 4.3 times greater than the physical area of a single unit-cell in an infinite array.

Highlights

  • Since 2012 various strategies have been utilized to improve the performance of the metasurface energy harvester (EH) structures2–7,16–25 including the wide angle reception and polarization free devices

  • The response showed an excellent incidence angle stability can enable us to measure the efficiency of the flexible EH with bending radius of 48 mm experimentally

  • We have introduced a figure-of-merit (FoM) for a fair comparison of our metasurface EH with the other reported works in Table I, as follows: FoM

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Summary

Introduction

Scitation.org/journal/adv polarizable arrays or metasurface can demonstrate the energy storage capability.16 EM harvesting can be applied as an effective energy source via transferring this stored energy to the loads.16 these loads are the input impedance of the rectifying circuits.2–4,6,7 Ramahi, et al exchanged the conventional antennas with split ring resonator in a rectenna system.17 The energy harvesting efficiency of the metasurface is often given in term of RF-to-AC efficiency.17 Since 2012 various strategies have been utilized to improve the performance of the metasurface energy harvester (EH) structures2–7,16–25 including the wide angle reception and polarization free devices.

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