Patent Application
20200240752
The present invention described herein relates to an invisibility cloaking device and more particularly to an electromagnetic cloaking device. The present disclosure also relates to method of making of the said device.
Electromagnetic (EM) cloaking technology is a stealth or camouflage technology that renders an object to be invisible to the Electro Magnetic (EM) spectrum. Various theories that are adopted in this technology are transformation optics as described in US20080024792A1, microwave network, active camouflage and scattering cancellation as described in US2015051417.
Recent research on EM cloaking technology is to make a wide-band and multi-band EM cloaking device. In US20110050360A1, EM resonators were arranged in a number of layers in order to achieve a wide band EM cloaking. In US20160111782A1, EM cloak structure comprises of a patterned metallic sheet with slits both in azimuthal and vertical directions utilizes two layers of cloak structure in order to achieve cloaking at two frequency bands. In US2015051417, Single layer dual-band EM cloak was achieved by loading electrical components on to the patterned metallic sheets.
In all the above said prior art, in order to achieve a wide or multi-band, either number of layers of patterned cloak structure were increased or cloak structures were loaded with other electrical elements. These methods are complex and may not be reliable as different components needs to work coherently. Also because of many components, manufacturing cost may go high and in some case it may not be violable also. The present disclosures aims at achieving a wide or multi band cloaking through single layer with less components involved.
The present disclosure relates to an invisibility cloaking device, in particular, to an electromagnetic cloaking device. The cloaking structure of the device comprises of single layer of plurality of array of strips placed over a base wherein the strips have the characteristics of either aperiodically placed strips or different geometries of strips or a combination thereof. The electromagnetic cloaking device as disclosed in present disclosure is capable of achieving a wide and/or multi-band cloak using a single layered cloak structure.
The results and features of present invention are illustrated using graphs and drawings and are referred as “FIG.” followed by its numerical reference. Only figures that are most significant to illustrate the present invention are disclosed. However, the present disclosure is not limited to such figures alone. Following are the description or caption of those visual illustrations.
Hereinafter, the proposed electromagnetic (EM) cloaking will be explained in detail along with the method of making the same. The visual illustrations are referred wherever required while detailing the invention. It may be noted here that the invention thus disclosed is not limited either by following descriptions or embodiments.
The present disclosure is about an invisibility cloaking device, in particular, to an EM cloaking device. In an embodiment, the said cloaking device comprising a base and a plurality of arrays of one or more strips placed over said base wherein the strips are characterized by either different geometries or placing the strips aperiodically or a combination of both said characteristics.
In yet another embodiment, the device can be employed as a single layered multi-band cloaking device as the device can effectively cloak an object from radiation waves of sources operating at different frequencies. In yet another embodiment, the sources can be antennas of any type such as plane wave or directional antennas.
In yet another embodiment, the base and strips can be made out of either conductive or dielectric material but the materials used for both base and strips are not same.
Hereinafter, the proposed electromagnetic (EM) cloaking will be described with the best method of performing the said invention. It may be noted here that the description thus disclosed is not limited either by following descriptions or embodiments.
The object to be cloaked can be made of either a conducting or dielectric to material and is covered by a base made of dielectric or conducting material (first material) respectively. This cloaked object is illuminated by a TM/TE wave source.
In this example, the base was made of first (dielectric) material and strips were made of second (conducting) material and the object made of conducting material was illuminated by TM wave sources using dipole antenna of 4 GHz.
The length and radius of the object which is to be cloaked is said to have 65 mm and 3.23 mm respectively. The total electric and magnetic fields including the incident and scattered field of the cloaked object in all its corresponding coordinate components were calculated. Applying the boundary conditions (for calculating unknown parameters), the scattered field impedance as the ratio of scattered electric and magnetic fields along the direction of propagation of incident wave was obtained as 390 Ω.
To make the above said object to be invisible to TM source, the said scattered impedance was compensated by the impedances of the plurality of arrays of one or more strips placed over the said base. By introducing the variations in compensated impedances, cloaking at multi bands in a single layer of base can be achieved. The variations in impedances can be obtained by the series connection of possible combinations of parallel RLC values. These lumped RLC values were converted to its distributed form. Thus, the variable impedances can be pronounced by the plurality of arrays of one or more strips with variable geometry placed over the said base or by placing strips aperiodically or both. The geometry variation of one or more strips or in their spacing or both can create impedance difference that leads to changes in phase velocity which finally varies the propagation path of the incoming wave reaching this geometry surface.
In this example, the cloak was designed to cloak the object at two different frequencies 4 GHz and 5 GHz. The number of strips required to cover the cloak was 4 based on the scattered field impedance of 390Ω. The clock radius was designed at 3.86 mm. The strips were placed over the base which is made up of dielectric material of dielectric constant as 10.2. The width of the strips is described as D1, D2, D3, and D4 as shown in
The cloaking device as designed in example 1 was placed before the antenna source of 4 GHz. The results obtained are provided in
| Number | Date | Country | Kind |
|---|---|---|---|
| 201741028806 | Aug 2017 | IN | national |
| 201741028806 | Jul 2018 | IN | national |
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/IN2018/000044 | 8/9/2018 | WO | 00 |
