The present disclosure relates to an antenna for wireless communication devices and systems and, more specifically, to printed dipole antennas for communication for wireless multi-band communication systems.
Wireless communication devices and systems are generally hand held or are part of portable laptop computers. Thus, the antenna must be of very small dimensions in order to fit the appropriate device. The system is used for general communication, as well as for wireless local area network (WLAN) systems. Dipole antennas have been used in these systems because they are small and can be tuned to the appropriate frequency. The shape of the printed dipole is generally a narrow, rectangular strip with a width less than 0.05 λ0 and a total length less than 0.5 λ0. The theoretical gain of the isotrope dipole is generally 2.5 dB and for a double dipole is less than or equal to 3 dB. One popular printed dipole antenna is the planar inverted-F antenna (PIFA).
The present disclosure is a dipole antenna for a wireless communication device. It includes a first conductive element superimposed on a portion of and separated from a second conductive element by a first dielectric layer. A first conductive via connects the first and second conductive elements through the first dielectric layer. The second conductive element is generally U-shaped. The second conductive element includes a plurality of spaced conductive strips extending transverse from adjacent ends of the legs of the U-shape. Each strip is dimensioned for a different center frequency λ0. The first conductive element may be L-shaped and one of the legs of the L-shape being superimposed on one of the legs of the U-shape. The first conductive via connects the other leg of the L-shape to the other leg of the U-shape.
The first and second conductive elements are each planar. The strips have a width of less than 0.05 λ0 and a length of less than 0.5 λ0.
The antenna may be omni-directional or uni-dimensional. If it is uni-dimensional, it includes a ground plane conductor superimposed and separated from the second conductive element by a second dielectric layer. A third conductive element is superimposed and separated from the strips of the second conductive element by the first dielectric layer. A second conductive via connects the third conductive element to the ground conductor through the dielectric layers. The first and third conductive elements may be co-planar. The third conductive element includes a plurality of fingers superimposed on a portion of lateral edges of each of the strips.
These and other aspects of the present disclosure will become apparent from the following detailed description of the disclosure, when considered in conjunction with accompanying drawings.
Although the present antenna of a system will be described with respect to WLAN dual frequency bands of, e.g., approximately 2.4 GHz and 5.2 GHz, the present antenna can be designed for operation in any of the frequency bands for portable, wireless communication devices. These could include GPS (1575 MHz), cellular telephones (824–970 MHz and 860–890 MHz), some PCS devices (1710–1810 MHz, 1750–1870 MHz and 1850–1990 MHz), cordless telephones (902–928 MHz) or Blue Tooth Specification 2.4–2.5 GHS frequency ranges.
The antenna system 10 of
The four strips 34, 36, 35 and 37 are each uniquely dimensioned so as to be tuned to or receive different frequency signals. They are each dimensioned such that the strip has a width less than 0.05 λ0 and a total length of less than 0.5 λ0.
The dielectric substrate 12 may be a printed circuit board, a fiberglass or a flexible film substrate made of polyimide. Covers 14, 16 may be additional, applied dielectric layers or may be hollow casing structures. Preferably, the conductive layers 20, 30 are printed on the dielectric substrate 12.
As an example of the quad-band dipole antenna of
The height h of the dielectric substrate 12 will vary depending upon the permeability or dielectric constant of the layer.
The narrow, rectangular strips 34, 36, 35, 37 of the appropriate dimension increases the total gain by reducing the surface waves and loss in the conductive layer. The number of conductive strips also effects the frequency sub-band.
The position of the via 40 and the slot S between the legs 33 of the U-shaped sub-conductor 32 effect the antenna performance related to the gain “distributions” in the frequency bands. A width of slot dimensions S and the location of the via 40 are selected so as to have approximately the same gain in all of the frequency bands of the strips 34, 36, 35, 37. The maximum theoretical gain obtained are above 4 dB and are 5.7 dB at 2.4 GHz and 7.5 dB at 5.4 GHz.
It should be noted that changing the length of legs 34, 35, 36, 37 between 5 mm, 10 nm and 15 mm has very little effect on VSWR and the gain at S11.
A directional or unidirectional dipole antenna incorporating the principles of the present invention is illustrated in
The antenna 11 of
The directive dipole 50 includes a plurality of fingers superimposed on a portion of the edges of each of the strips 34, 36, 35, 37. As illustrated, the end strips 52, 58 are superimposed and extend laterally beyond the lateral edges of strips 34, 36, 35, 37. The inner fingers 54, 56 are adjacent to the inner edge of strips 34, 36, 35, 37 and do not extend laterally therebeyond.
Preferably, the permeability or dielectric constant of the dielectric substrate 12 is greater than the permeability or dielectric constant of the dielectric layer 16. Also, the thickness h1 of the dielectric substrate 12 is substantially less than the thickness h2 of the dielectric layer 16. Preferably, the dielectric substrate 12 is at least half of the thickness of the dielectric layer 16.
The polygonal perimeter of the end portion 53 of the dipole directive 50 has a similar shape of the PEAN03 fractal shape directive dipole. It should also be noted that the profile of the antenna 12 gives the appearance of a double planar inverted-F antenna (PIFA).
Although not shown, a number of via holes around the dipole through the insulated layer 12 may be provided. These via holes would provide pseudo-photonic crystals. This would increase the total gain by reducing the surface waves and the radiation in the dielectric material. This is true of both antennas.
Although the present disclosure has been described and illustrated in detail, it is to be clearly understood that this is done by way of illustration and example only and is not to be taken by way of limitation. The scope of the present disclosure is to be limited only by the terms of the appended claims.
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