The present invention relates to a radiator for an RF (radio frequency) communication device. In particular, the invention relates to a radiator for use in a portable or handheld communication device.
Portable handheld RF communication devices such as cellular telephones, portable radios, data communication devices, and the like employ a radiator or antenna to radiate and receive RF signals. Monopole antennas are widely used as RF radiators in such devices. As such communication devices become more complex, e.g. by the incorporation of additional functional components such as cameras, advanced loudspeakers, and the like, extra functional requirements are imposed on the radiator system. There is also an ongoing search for ways to reduce the overall size and weight of such devices, including the radiator system.
Thus, it is expected in the future that the space available in a portable communication device for the radiator will decrease, since the overall size of the device will continue to decrease and/or the device will have to accommodate other functional components at the expense of the radiator. However, reducing the radiator size may negatively impact radiator gain and bandwidth. This follows from the fact that a radiator is used to transform a bounded wave into a radiating wave. However, when the dimensions of the radiator are much smaller than the wavelength of the RF radiation to be transmitted, the radiator performs this transformation with only a poor efficiency. The loss in radiator gain can to some extent be compensated for by amplification. However, this causes a greater energy consumption, e.g. from a battery of the device.
Another challenging task is that the distance available between the radiator and other components of the communication device, such as a camera unit or an advanced loudspeaker, is likely to be reduced as well. This requires careful selection of where components are placed in the communication device to give suitable operation of the radiator.
Thus there is a need for a new radiator (antenna) which addresses the above problems.
According to the present invention in a first aspect there is provided a radiator as defined in claim 1 of the accompanying claims.
Further features of the present invention are as defined in the accompanying dependent claims and are disclosed in the embodiments of the invention to be described.
Embodiments of the present invention will now be described by way of example with reference to the accompanying drawings, in which:
In embodiments of the invention to be described a radiator for an RF communication device includes a first member including a first conducting surface operable to provide a radiating surface, a second member including a second conducting surface operable to provide a near field reflector or ground plane, the first conducting surface and the second conducting surface being galvanically connected, wherein the first conducting surface is sloping relative to the second conducting surface and the first conducting surface includes a first conducting region and a second conducting region having between them a gap including at least a portion which is tapered.
The radiator may include at least one contact area on the first conducting surface to receive a feed conductor to feed RF electrical signals to and from the first and second conducting regions.
The first and second conducting regions of the radiator may be separate regions and the gap may extend between the first and second conducting regions to separate them.
The first member may comprise a first insulating substrate having thereon a first conducting layer providing the first conducting surface; and the second member may comprise a second insulating substrate having thereon a second conducting layer providing the second conducting surface. The first and second insulating substrates may conveniently be made of printed circuit board material and the first and second conducting layers may be metallic layers, e.g. of copper, each formed on a surface of each substrate in a known manner. The first insulating substrate and the first conducting layer thereon may be shaped to facilitate suitable operation of the radiator as will be illustrated in the embodiments of the invention to be described.
A first insulating body 307 and a second insulating body 315 are mounted on an insulating pedestal 309 on the insulating board 301 near an upper end of the front portion 103. The insulating body 307 may comprise a case housing a component device of the device 100 such as an image processing unit. The insulating body 315 may comprise a case housing a further component device of the device 100, e.g. an imaging camera. The insulating body 307 carries on a rear face (a face which is shown uppermost in
In operation, to be described in more detail later, the conducting layer 303, galvanically connected to the first antenna portion 311 by the stub connector 401, forms the first conducting surface, referred to earlier, of a radiator embodying the invention. That is, the conducting layer 303 provides a near field reflector known in the art as a ground plane (or alternatively as a counterpoise) for the first antenna portion 311 which provides the second conducting surface, referred to earlier, of the radiator embodying the invention. The conducting layer 303 may also form a ground plane for the second antenna portion 313. As known by those skilled in the art, a ground plane of a radiator is a conducting surface which serves as a near field reflector to allow normal operation of the radiator.
As shown in
As noted earlier, a gap 621 is formed between the conducting regions 601 and 603, thereby exposing insulating material of the board on which the regions 601 and 603 are formed. The gap 621 includes a first portion 623 extending from a region mid-way along the upper edge 507 in a direction perpendicular to the upper edge 507. The first portion 623 of the gap 621 has parallel sides 625 and 627 formed by edges of the regions 601 and 603. The gap 621 has a second portion 629 extending from the first portion 623 to the side edge 615. The second portion 629 of the gap 621 has sides 631 and 633 formed by edges of the regions 601 and 603. The side 631 is perpendicular to the sides 627 and 629. The side 633 is not parallel to the side 631 but instead is disposed at a small acute angle relative to the side 631. The small acute angle may be between one degree and twelve degrees, particularly between three degrees and nine degrees, e.g. six degrees. The gap 621 thereby has a shape in the second portion 629 which is tapered such that the gap is wider at the edge 615 than where it joins the first portion 623.
A small area 633 of the region 601 adjacent to the gap 621 near the upper edge 507 and a similar small area 635 of the region 603 adjacent to the gap 621 near the upper edge 507 form contact areas for a feed conductor (not shown), e.g. an inner conductor of a coaxial cable, for delivery of RF electrical signals between the first antenna portion 311 and an RF transceiver (not shown) housed inside the device 100. The stub connector 401 shown in
The first antenna portion 311, e.g. the antenna portion 600, operating in conjunction with its associated ground plane provided by the metallic conducting layer 303 on the insulating board 301, provides a novel radiator embodying the invention which beneficially can provide very attractive properties, particularly a very wide operational resonance band with a controlled impedance as illustrated later. The disposition of the conducting regions 601 and 603 relative to the ground plane provided by the conducting layer 303 and the shape of the conducting regions 601 and 603 and the gap 621 between them allow good radiator efficiency to be obtained by providing reduced reactive impedance. In other words, substantially all of the RF energy transformed by the antenna portion 600 from conducted energy to energy radiated in free space (or vice versa) will essentially be transformed without reactive impedance losses. In addition, the recess in the conducting layer 303 at the recess 503 of the insulating board 301 plays a useful role in encouraging diffraction effects from electrical currents in the adjacent metallic conducting layer 303 (i.e. in the adjacent part of the ground plane) which in turn allows a wide angle radiation beam to be obtained from the first antenna portion 311, e.g. the antenna portion 600.
In a particular example, the insulating board 301 and the antenna portion 600 have the following properties which are exemplary only to illustrate results which may be obtained:
1) The insulating board 301 has a length (longest dimension) of 181 (one hundred and eighty one) millimeters and a width at the upper edge (including the recess 503) of 67.5 (sixty seven point five) millimeters.
2) The insulating board 301 and the insulating board of the antenna portion 600 are made of the industry standard material FR4 (commonly used in printed circuit board manufacture) having a thickness of 1.6 millimeters, and dielectric properties of εr=4.5 (where εr is relative permittivity) and tan δ=0.019 (where tan δ is loss factor or tangent of loss angle).
3) The metallic conducting layer 303 on the insulating board 101, and the metallic conducting material on the antenna portion 600 to form the conducting regions 601 and 603, is copper having a thickness of 0.018 millimeters deposited and shaped in a known manner.
4) The antenna portion 600 including the conducting regions 601 and 603 is disposed at an angle of 15 (fifteen) degrees relative to the conducting layer 303 on the insulating board 301.
5) The antenna portion 600 has the following dimensions: length of the edge 507: 32.5 (thirty two point five) millimeters; distance between the edge 507 and the side 611: 25.2 (twenty five point two) millimeters; length of the first portion 623 of the gap 621 (from the side 507 to the side 633): 18 (eighteen) millimeters; width of the first portion 623 of the gap 621: 1.2 (one point two) millimeters; length of the second portion 629 of the gap 621 (to the side 625): 11 (eleven) millimeters; width of the second portion 629 of the gap 621: 4 (four) millimeters; angle of slope of the side 633 relative to the side 631: 6 (six) degrees.
6) The electrical length of the antenna portion 600 was increased by a factor of about 1.3 by the presence of parasitic capacitance from metallic parts (not shown) of the body 315 acting as a case housing the parts.
Using the particular example described above for the antenna portion 600 (as the first antenna portion 311) and the insulating board 301, the following measurement results were obtained:
(i) The VSWR (voltage standing wave ratio) as a function of operational frequency in GigaHertz (GHz) was measured and the results obtained are plotted as a curve 700 as shown in
(ii) The radiation pattern (gain) performance was measured at various frequencies of interest in the frequency range illustrated by the curve 700 and the measurement results which were obtained are as summarised in Table 1 as follows:
The results shown in Table 1 indicate good performance at all of the measured frequencies, with substantially omnidirectional radiation patterns. Similar results were obtained when the dimensions of the metallic conducting layer 303 on the insulating board 301 were reduced to a length of 85 mm and a width of 42 mm (with the recess 503 in the same position as shown in
The second column in Table 1 indicates well known systems operating at the frequencies indicated in the first column thereby providing applications in which the device 100 embodying the invention may operate using the radiator provided by the first antenna portion 311 and the insulating board 301 including the conducting layer 303.
The antenna portion 800 provides a quasi quarter wave radiator in which the radiating metallic conducting material resembles a known ‘inverted L’ antenna shape. The strip 803 is employed to provide a galvanic connection (not shown) to the ground plane provided by the conducting layer 303.
In operation, the first antenna portion 311 and the second antenna portion 313, e.g. the antenna portion 800, operate to transform RF signals between electrical signals carried by a feed conductor (not shown) and radiated electromagnetic waves sent over the air, and vice versa. The first antenna portion 311 and the second antenna portion 313 may provide polarisation diversity for a given signal at 2.44 and 4.9 GHz. In other words, the polarisation components of the signal at each of the selected frequencies differ in the two antenna portions giving a better overall polarisation coverage. This may be important in some applications such as wireless local area networks used in indoors or in urban outdoor environments in which an RF radiated signal may undergo several reflections and scatterings which may change its polarisation significantly. The mutual disposition of the first antenna portion 311 and the second antenna portion 313, with the second antenna portion 313 mounted in a plane perpendicular to that of the first antenna portion 311, e.g. at an end of the gap 621 distant from the contact areas 633 and 635 at which RF current is delivered into and out of the antenna portion 600, allows operation of the antenna portions 311 and 313 without substantial coupling or mutual interference. In other words, there is a substantial electrical isolation between the first antenna portion 311, e.g. the antenna portion 600, and the second antenna portion 313, e.g. the antenna portion 800, of about 15 dB (decibels).
The antenna portion 900 is aimed principally at operation in a frequency band that includes 806 (eight hundred and six) MegaHertz and 960 (nine hundred and sixty) MegaHertz. The antenna portion 900 is suitable to give similar gain results as for the antenna portion 600 at these frequencies but may be formed using less conducting material to form the conducting regions 901 and 903.
A particular example of the antenna portion 900, made from the same materials and having the same outer dimensions and the same ground plane as for the particular example of the antenna portion 600 specified above, gave the following measurement results:
(i) VSWR at 806 MHz: 1.692;
(ii) VSWR at 960 MHz: 1.964;
(iii) directivity at 900 MHz: 2.45 dBi
(iv) gain at 900 MHz: 2.40 dBi
These results obtained indicate good performance at the measured frequencies, with omnidirectional radiation patterns.
Similar results were obtained when the dimensions of the conducting layer 303 on the insulating board 301 providing a ground plane were reduced to a length of 85 mm and a width of 42 mm (with the recess 503 in the same position as shown in
Although the present invention has been described in terms of the above embodiments, especially with reference to the accompanying drawings, it is not intended to be limited to the specific form described in such embodiments. Rather, the scope of the present invention is limited only by the accompanying claims. In the claims, the terms ‘comprising’ or ‘including’ do not exclude the presence of other integers or steps. Furthermore, although individually listed, a plurality of means, elements or method steps may be implemented by, for example, a single unit or processor. Additionally, although individual features may be included in different claims, these may possibly be advantageously combined, and the inclusion in different claims does not imply that a combination of features is not feasible and/or advantageous. In addition, singular references do not exclude a plurality. Thus references to “a”, “an”, “first”, “second” etc do not preclude a plurality.
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