The present invention relates to an electromagnetic wave propagation sheet, and more particularly, to an electromagnetic wave propagation sheet, a width of which is reduced, and a display shelf implementing the electromagnetic wave propagation sheet.
In addition to one-dimensional communication by a wire and three-dimensional communication by an electric wave, two-dimensional communication is proposed as a new communication type and partially used. A basic configuration of the two-dimensional communication system is constituted by an electromagnetic wave propagation sheet and a proximity coupler. The proximity coupler is an electromagnetic coupling element used to exchange electromagnetic waves between an electromagnetic wave propagation sheet and an external instrument. In the two-dimensional communication, since input and output of the electromagnetic wave are performed at an arbitrary place on the sheet, a clear cableless operation environment can be realized in comparison with the wired communication.
In addition, the two-dimensional communication has an advantage of electric power saving, in which loss due to diffusion is reduced, to confine the electromagnetic wave in the sheet, in comparison with the communication by the electric wave. In the electromagnetic wave propagation sheet, for example, as disclosed in Patent Document 1 or Non Patent Document 1, a dielectric layer is configured to be sandwiched between two conductor layers, one of the conductor layers is planar, and the other one of the conductor lavers has a mesh shape. The electromagnetic wave propagated in the sheet is leaked from an opening section of a mesh-shaped conductor as an evanescent wave. Exchange of the electromagnetic waves between the sheet and the coupler is performed using these.
The two-dimensional communication technique can be applied to power transmission as well as communication. By injecting high frequency power into the electromagnetic wave propagation sheet from the high frequency power source, supply of the power to an electronic instrument can be performed by performing power reception and rectification in the coupler.
Non Patent Document 1: Hiroyuki Shinoda, et al., “Simultaneous Transmission Method of Signal and Power using Surface Microwave (Theory Supporting Ubiquitous/Sensor Network, and General),” Electronics Information Communication Institute Corporation, Technical Research Report Vol. 107, No. 53 (20070517) pp.
115-118
In the electromagnetic wave propagation sheet of the related art, since occurrence of leakage of the electromagnetic wave from the end section of the electromagnetic wave propagation sheet is suppressed, the mesh-shaped conductor and the planar conductor may be electrically connected to each other in the sheet end section. Hereinafter, a structure in which the two conductors are connected in the sheet end section as described above will be referred to as a short end structure.
As shown in a side view of
In addition, while the electromagnetic wave propagation sheet is assumed to be used in a two-dimensional shape such as a mat, a merit obtained by a one-dimensional rail shape is also provided. The rail-shaped electromagnetic wave propagation sheet can improve transmission efficiency without reducing electricity diffusion in a widthwise direction, and can be implemented in a gap of a conventional layout because space can be saved.
When the short end structure is applied to the rail-shaped electromagnetic wave propagation sheet, a cutoff frequency is present like the rectangular waveguide, and thus a low frequency electromagnetic wave is not propagated. That is, a sheet width cannot be reduced to be smaller than a specific dimension determined by a frequency of the electromagnetic wave to be propagated, i.e., half of a wavelength of the electromagnetic wave in the sheet transmission path. In the rail-shaped electromagnetic wave propagation sheet elongated in one direction, when the sheet width can be reduced to be smaller than the limited dimension and the electromagnetic wave propagation sheet having a small implementation space can be realized, further expansion of an application field of the two-dimensional communication system can be expected.
In consideration of the above-mentioned circumstances, the present invention is directed to provide a two-dimensional communication system constituted by a mesh-shaped conductor layer, a planar conductor layer, and an inductor layer sandwiched therebetween and capable of expanding an application range thereof by reducing a sheet width of a rail-shaped electromagnetic wave propagation sheet elongated in one direction to provide an electromagnetic wave propagation sheet having a small implementation space.
In order to solve the aforementioned problems, an electromagnetic wave propagation sheet according to the present invention is constituted by a mesh-shaped conductor layer, a planar conductor layer, and an inductor layer sandwiched therebetween, wherein the mesh-shaped conductor layer and the planar conductor layer are electrically connected to each other in an end section of the electromagnetic wave propagation sheet by a short conductor, and a mesh-shaped conductor that constitutes the mesh-shaped conductor layer has a meander shape in the vicinity of the electromagnetic wave propagation sheet end section.
In addition, an electromagnetic wave propagation sheet according to the present invention is constituted by a mesh-shaped conductor layer, a planar conductor layer, and a dielectric layer sandwiched therebetween, wherein the mesh-shaped conductor layer and the planar conductor layer are electrically connected to each other in an end section of the electromagnetic wave propagation sheet by a short conductor, and a mesh-shaped conductor that constitutes the mesh-shaped conductor layer has a spiral shape in the vicinity of the electromagnetic wave propagation sheet end section.
Further, an electromagnetic wave propagation sheet according to the present invention is constituted by a mesh-shaped conductor layer, a planar conductor layer, and a dielectric layer sandwiched therebetween, wherein the mesh-shaped conductor layer and the planar conductor layer are electrically connected to each other in an end section of the electromagnetic wave propagation sheet by a short conductor, and a mesh-shaped conductor that constitutes the mesh-shaped conductor layer has a small line width in the vicinity of the electromagnetic wave propagation sheet end section.
Furthermore, an electromagnetic wave propagation sheet according to the present invention is constituted by a mesh-shaped conductor layer, a planar conductor layer, and a dielectric layer sandwiched therebetween, wherein the mesh-shaped conductor layer and the planar conductor layer are electrically connected to each other in an end section of the electromagnetic wave propagation sheet by a short conductor, and a magnetic body is applied in the vicinity of the electromagnetic wave propagation sheet end section.
According to the electromagnetic wave propagation sheet of the present invention, in the electromagnetic wave propagation sheet constituted by the mesh-shaped conductor layer, the planar conductor layer, and the inductor layer sandwiched therebetween, since inductance of the ferromagnetic field domain near the sheet end section is increased, a wavelength of the electromagnetic wave of the sheet transmission path can he reduced. Accordingly, in the electromagnetic wave propagation sheet, a sheet width can be reduced to be smaller than a specific dimension determined by a frequency of the electromagnetic wave to be propagated to the sheet.
Hereinafter, an embodiment of the present invention will be described in detail with reference to the accompanying drawings.
As shown in the side view of
While the mesh-shaped conductor 5 has a shape in which linear conductors 8 are arranged in a lattice shape, a meander-shaped conductor 9 having a zigzag meander shape is provided in the vicinity of the sheet end section of the linear conductor 8, and the meander-shaped conductor 9 is connected to the short conductor 7. In addition, the meander shape is a shape in which all or a portion thereof is formed in a zigzag to accommodate an antenna having a certain effective length in a limited space.
In the first embodiment, all distal ends of the mesh-shaped conductors 5 in the vicinity of the sheet have a meander shape, and a disposition interval of the meander-shaped conductor 9 is equal to a disposition interval of the linear conductor 8 that constitutes the mesh-shaped conductor 5. However, the disposition interval of the meander-shaped conductor 9 is not limited thereto but, as shown in
In this way, since inductance of a ferromagnetic field domain near the sheet end section is increased as the vicinity of the sheet end section of the mesh-shaped conductor 5 that forms the surface conductor layer 2 has a meander shape, a wavelength of an electromagnetic wave of a sheet transmission path can be reduced. According to the above-mentioned action, in the rail-shaped electromagnetic wave propagation sheet 1 elongated in one direction, a sheet width can be reduced to be smaller than a specific dimension determined by a frequency of the electromagnetic wave to be propagated in the sheet.
A distal end of the spiral-shaped conductor 12 is connected to a conductor pattern 13 of the intermediate conductor layer 11 through a conductor such as a via or the like, and further, the conductor pattern 13 of the intermediate conductor layer 11 is connected to the short conductor 7 of the sheet end section. In
In this way, since inductance of the ferromagnetic field domain near the sheet end section is increased as the vicinity of the sheet end section of the mesh-shaped conductor that forms the surface conductor layer 2C has a spiral shape, a wavelength of the electromagnetic wave of the sheet transmission path can be reduced. Accordingly, in the rail-shaped electromagnetic wave propagation sheet 1C elongated in one direction, a sheet width can be reduced to be smaller than a specific dimension determined by a frequency of the electromagnetic wave to be propagated in the sheet.
In a third embodiment, unlike the first embodiment in which the vicinity of the sheet end section of the mesh-shaped conductor has the meander shape, a conductor has a line width smaller than that of the linear conductor of the mesh-shaped conductor. That is, the linear conductor of the mesh-shaped conductor is reduced in a line width in the vicinity of the sheet end section.
Here, the thin line conductor requires that a length from the short conductor is smaller than λ/4. Provided that a characteristic impedance of a thin line conduction portion is set to Z0, a length of a thin line is set to 1, and a wavelength in a line is set to λ, an input impedance Zin of the thin line when a short end side is seen from the mesh conductor side is expressed as the following equation (1), and the thin line acts as an inductance within a range of mλ/2<1<(mλ/2+λ/4), where m is an integer.
As the thin line conductor is set as described above, inductance of the ferromagnetic field domain near the short end can be increased to reduce the wavelength, and the sheet width can be reduced.
In this way, since the inductance of the ferromagnetic field domain near the short end is further increased as the magnetic body 15 is applied in the vicinity of the sheet end section, the wavelength of the electromagnetic wave of the sheet transmission path can be further increased. For reference,
Transmission characteristics of three evaluation models of the sheet on which the magnetic body is applied in the vicinity of the sheet end section of the mesh-shaped conductor (“conventional mesh+magnetic body”), the sheet on which the magnetic body is not applied (
As a result, it can be confirmed that, as the magnetic body is applied, a cutoff frequency (a frequency at which an attenuation value is increased and an electromagnetic wave is not propagated) is shifted to a lower frequency side. It will be appreciated that, as the magnetic body is applied, the wavelength of the electromagnetic wave that propagates in the sheet is largely reduced. In addition, it can be confirmed that, as the sheet end section has a meander shape, the wavelength is largely reduced.
According to the above-mentioned action, in the rail-shaped electromagnetic wave propagation sheet elongated in one direction, the sheet width can be reduced to be smaller than a specific dimension determined by a frequency of the electromagnetic wave to be propagated in the sheet.
In a store such as a supermarket, a convenience store, or the like, goods are displayed using a display shelf 30 as shown in
As shown in
In addition, as shown in
A standard height of the shelf 33 and a standard height of the price rail 32 are about 30 mm. Showing an example of a result by simulation, in the case in which supply of power or communication is performed using an electromagnetic wave of a band of 2.4 GHz in the electromagnetic wave propagation sheet of a certain configuration (a specific material constant or dimension), when the electromagnetic wave propagation sheet 101 of the related art as shown in
On the other hand, as the electromagnetic wave propagation sheet 1 of the present invention is applied, the sheet width can be suppressed and reduced (the sheet height can be reduced) to about 30 mm. Relative permeability of the magnetic body in the calculation was about 50. In this way, as the present invention is applied, goods displayed on the shelf plate 31 can he easily found and it can arouse customer interests. In addition, in
Priority is claimed on Japanese Patent Application No. 2011-159565, filed Jul. 21, 2011, the content of which is incorporated herein by reference.
The electromagnetic wave propagation sheet according to the present invention can provide the electromagnetic wave propagation sheet having a reduced implementation space obtained by reducing a sheet width.
1 electromagnetic wave propagation sheet
2 surface conductor layer (mesh-shaped conductor layer)
3 rear surface conductor layer (planar conductor layer)
4 dielectric layer
7 short conductor
15 magnetic body
30 display shelf
31 shelf plate
Number | Date | Country | Kind |
---|---|---|---|
2011-159565 | Jul 2011 | JP | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
---|---|---|---|---|
PCT/JP2012/066088 | 6/22/2012 | WO | 00 | 1/17/2014 |