I. Field of the Invention
[0001] The present invention relates to an antenna and to a feed network for an antenna.
More specifically, the present invention relates to a dual band helical antenna with
first and second feed networks wherein a portion of each of the feed networks is provided
in an area coincident with radiators of the antenna.
II. Description of the Related Art
[0002] Contemporary personal communication devices are enjoying widespread use in numerous
mobile and portable applications. With traditional mobile applications, the desire
to minimize the size of the communication device, such as a mobile telephone for example,
has led to a moderate level of downsizing. However, as the portable, hand-held applications
increase in popularity, the demand for smaller and smaller devices has increased dramatically.
Recent developments in processor technology, battery technology and communications
technology, have enabled the size and weight of the portable device to be reduced
drastically over the past several years.
[0003] One area in which reductions in size are desired is the device's antenna. The size
and weight of the antenna play an important role in downsizing the communication device.
The overall size of the antenna can impact the size of the device's body. Smaller
diameter and shorter length antennas can allow smaller overall device sizes as well
as smaller body sizes.
[0004] Size of the device is not the only factor that needs to be considered in designing
antennas for portable applications. Another factor to be considered in designing antennas
is attenuation and/or blockage effects resulting from the proximity of the user's
head to the antenna during normal operations. Yet another factor is the characteristics
of the communication link, such as, for example, desired radiation patterns and operating
frequencies.
[0005] An antenna that finds widespread usage in satellite communication systems is the
helical antenna. One reason for the helical antenna's popularity in satellite communication
systems is its ability to produce and receive circularly-polarized radiation employed
in such systems. Additionally, because the helical antenna is capable of producing
a radiation pattern that is nearly hemispherical, the helical antenna is particularly
well suited to applications in mobile satellite communication systems and in satellite
navigational systems.
[0006] Conventional helical antennas are made by twisting the radiators of the antenna into
a helical structure. A common helical antenna is the quadrifilar helical antenna which
utilizes four radiators spaced equally around a core and excited in phase quadrature
(i.e., the radiators are excited by signals that differ in phase by one-quarter of
a period or 90°). The length of the radiators is typically an integer multiple of
the quarter wavelength of the operating frequency of the communication device. The
radiation patterns are typically adjusted by varying the pitch of the radiator, the
length of the radiator (in integer multiples of a quarter-wavelength), and the diameter
of the core.
[0007] Conventional helical antennas can be made using wire or strip technology. With strip
technology, the radiators of the antenna are etched or deposited onto a thin, flexible
substrate. The radiators are positioned such that they are parallel to each other,
but at an obtuse angle to the sides (or edges) of the substrate. The substrate is
then formed, or rolled, into a cylindrical, conical, or other appropriate shape causing
the strip radiators to form a helix.
[0008] This conventional helical antenna, however, also has the characteristic that the
radiator lengths are an integer multiple of one quarter wavelength of the desired
resonant frequency, resulting in an overall antenna length that is longer than desired
for some portable or mobile applications.
[0009] Additionally, in applications where transmit and receive communications occur at
different frequencies, dual-band antennas are desirable. However, dual-band antennas
are often available only in less than desirable configurations. For example, one way
in which a dual band antenna can be made is to stack two single-band quadrifilar helix
antennas end-to-end, so that they form a single cylinder. A disadvantage of this solution,
however, is that such an antenna is longer than would otherwise be desired for portable,
or hand-held applications.
[0010] Another technique for providing dual-band performance has been to utilize two separate
single band antennas. However, for hand-held units, the two antennas would have to
be located in close proximity to one another. Two single band antennas, placed in
close proximity on a portable, or hand-held unit would cause coupling between the
two antennas, leading to degraded performance as well as unwanted interference.
SUMMARY OF THE INVENTION
[0011] The invention provides a dual band helical antenna, comprising: a first antenna section
comprising a first feed network disposed on a first side of a substrate on a first
feed portion of the first antenna, a first ground plane disposed on a second side
of said substrate and opposite said feed network, and a first set of one or more radiators
disposed on said substrate and extending from said feed network; a second antenna
section comprising a second feed network disposed on said substrate on a second feed
portion, a second ground plane disposed on said substrate opposite said feed network;
a second set of one or more radiators disposed on said substrate and extending from
said feed network; and means for providing a path for current to flow from said radiators
of said second antenna along the axis of said second antenna to thereby increase the
energy radiated in the directions perpendicular to the axis; wherein said first feed
network comprises a first set of one or more traces disposed on said first feed portion
of the antenna and a second set of one or more traces disposed on a radiator portion
of said first antenna section, and said second feed network comprises a third set
of one or more traces disposed on said second feed portion and a fourth set of one
or more traces disposed on a radiator portion of said second antenna section.
[0012] The present invention is embodied in a novel and improved feed network for an antenna
which includes a radiator portion and a feed portion. The feed network is configured
such that a section of the feed network is disposed on the radiator portion of the
antenna and the remainder of the feed network is disposed on the feed portion. Because
part of the feed network is disposed on the radiator portion, the remainder of the
feed network requires less area on the feed portion. As a result, the feed portion
of the antenna can be smaller as compared to antennas having conventional feed networks.
Because this configuration requires less area on the feed portion, the feed network
is said to be area-efficient.
[0013] In a preferred embodiment, the traces of the feed network that are disposed on the
radiator portion are disposed opposite the ground portion of the radiators. As such,
the ground portion of the radiators serves as a ground plane for this part of the
feed network.
[0014] The feed network can be implemented with numerous different types of antennas of
varying configurations, including single-band and multi-band helical antennas.
[0015] One advantage of the invention is that the overall size of the antenna and the amount
of loss in the feed are reduced as compared to antennas having conventional feed networks.
[0016] In one embodiment, the feed network is implemented with a dual-band helical antenna
having two sets of one or more helically wound radiators. The radiators are wound,
or wrapped, such that the antenna is in a cylindrical, conical, or other appropriate
shape to optimize or otherwise obtain desired radiation patterns. According to this
implementation, one set of radiators is provided for operation at a first frequency
and the second set is provided for operation at a second frequency which preferably
is different from the first frequency. Each set of radiators has an associated feed
network to provide the signals to drive the radiators. Thus, the dual-band antenna
can be described as being comprised of two single-band antennas, each single-band
antenna having a radiator portion and a feed portion.
[0017] A tab can be provided to feed the signal to the first single-band antenna. The tab
extends from the feed portion of the first single-band antenna. When the antenna is
formed into a cylinder or other appropriate shape, the tab is aligned with the axis
of the antenna. More specifically, in a preferred embodiment, the tab extends radially
inward to provide a centrally located feed structure. Thus, the tab and the feed line
do not interfere with the signal patterns of the second single-band antenna.
BRIEF DESCRIPTION OF THE DRAWINGS
[0018] The features, objects, and advantages of the present invention will become more apparent
from the detailed description set forth below of an embodiment of the invention when
taken in conjunction with the drawings in which like reference characters identify
correspondingly throughout. Additionally, the left-most digit(s) of a reference number
identifies the drawing in which the reference first appears.
FIG. 1A is a diagram illustrating a conventional wire quadrifilar helical antenna.
FIG. 1B is a diagram illustrating a conventional strip quadrifilar helical antenna.
FIG. 2A is a diagram illustrating a planar representation of an open-circuited, or open
terminated, quadrifilar helical antenna.
FIG. 2B is a diagram illustrating a planar representation of a short-circuited quadrifilar
helical antenna.
FIG. 3 is a diagram illustrating current distribution on a radiator of a short-circuited
quadrifilar helical antenna.
FIG. 4 is a diagram illustrating a far surface of an etched substrate of a strip helical
antenna.
FIG. 5 is a diagram illustrating a near surface of an etched substrate of a strip helical
antenna.
FIG. 6 is a diagram illustrating a perspective view of an etched substrate of a strip helical
antenna.
FIG. 7A is a diagram illustrating an open-circuit coupled multi-segment radiator having
five coupled segments.
FIG. 7B is a diagram illustrating a pair of short-circuited coupled multi-segment radiators.
FIG. 8A is a diagram illustrating a planar representation of a short-circuited coupled multi-segment
quadrifilar helical antenna.
FIG 8B is a diagram illustrating a coupled multi-segment quadrifilar helical antenna formed
into a cylindrical shape.
FIG. 9A is a diagram illustrating overlap δ and spacing s of radiator segments.
FIG. 9B is a diagram illustrating example current distributions on radiator segments of
the coupled multi-segment helical antenna.
FIG. 10A is a diagram illustrating two point sources radiating signals differing in phase
by 90°.
FIG. 10B is a diagram illustrating field patterns for the point sources illustrated in FIG.
10A.
FIG. 10C is a diagram illustrating circular polarization field patterns for a conventional
helical antenna and circular polarization field patterns for a helical antenna having
a feed tab aligned with the axis of the antenna.
FIG. 11 is a diagram illustrating the embodiment in which each segment is placed equidistant
from the segments on either side.
FIG. 12 is a diagram illustrating an example implementation of a coupled multi-segment antenna
according to one embodiment of the invention.
FIG. 13 is a diagram illustrating planar representations of the surfaces of a stacked dual-band
helical antenna according to one embodiment of the invention.
FIG. 14 is a diagram illustrating planar representations of the surfaces of a stacked dual-band
helical antenna according to one embodiment of the invention in which the feed points
for the radiators are positioned at a distance from the feed network.
FIG. 15 is a diagram illustrating a planar representation of a tab used to feed one antenna
of the stacked dual-band helical antenna according to one embodiment of the invention.
FIG. 16 is a diagram illustrating example dimensions for a stacked dual-band helical antenna
according to one embodiment of the invention.
FIG. 17 is a diagram illustrating an example of a conventional quadrature phase feed network.
FIG. 18 is a diagram illustrating a feed network having portions that extend into the radiators
of the antenna according to one embodiment of the invention.
FIG. 19 is a diagram illustrating feed networks along with the signal traces, including the
feed paths, for antennas according to one embodiment of the invention.
FIG. 20 is a diagram illustrating an outline for the ground plane of antennas according to
one embodiment of the invention.
FIG. 21 is a diagram illustrating both the ground planes and the signal traces of a dual
band antenna superimposed according to one embodiment of the invention.
FIG. 22A is a diagram illustrating a structure for maintaining an antenna in a cylindrical
or other appropriate shape according to one embodiment.
FIGS. 22B-22E are diagrams illustrating the formation of an antenna in a cylindrical or other
appropriate shape according to the embodiment illustrated in FIG. 22A.
FIG. 23A is a diagram illustrating a form suitable for use in supporting an antenna in a
cylindrical or other appropriate shape according to one embodiment.
FIGS. 23B and 23C are diagrams illustrating the formation of an antenna in a cylindrical or other
appropriate shape according to the embodiment illustrated in FIG. 23A.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS
I. Overview and Discussion of the Invention
[0019] The present invention is directed toward an area-efficient feed network for an antenna.
A portion of the feed network is provided on a radiator portion of the antenna. This
decreases the area required for the feed portion of the antenna.
II. Example Environment
[0020] In a broad sense, the invention can be implemented in any system for which helical
antenna technology can be utilized. One example of such an environment is a communication
system in which users having fixed, mobile and/or portable telephones communicate
with other parties through a satellite communication link. In this example environment,
the telephone is required to have an antenna tuned to the frequency of the satellite
communication link.
[0021] The present invention is described in terms of this example environment Description
in these terms is provided for convenience only. It is not intended that the invention
be limited to application in this example environment. In fact, after reading the
following description, it will become apparent to a person skilled in the relevant
art how to implement the invention in alternative environments.
III. Conventional Helical Antennas
[0022] Before describing the embodiments of the invention in detail, it is useful to describe
the radiator portions of some conventional helical antennas. Specifically, this section
of the document describes radiator portions of some conventional quadrifilar helical
antennas. FIGS.
1A and
1B are diagrams illustrating a radiator portion
100 of a conventional quadrifilar helical antenna in wire form and in strip form, respectively.
The radiator portion
100 illustrated in FIGS.
1A and
1B is that of a quadrifilar helical antenna, meaning it has four radiators
104 operating in phase quadrature. As illustrated in FIGS.
1A and
1B, radiators
104 are wound to provide circular polarization.
[0023] FIGS.
2A and
2B are diagrams illustrating planar representations of a radiator portion of conventional
quadrifilar helical antennas. In other words, FIGS.
2A and
2B illustrate the radiators as they would appear if the antenna cylinder were "unrolled"
on a flat surface. FIG.
2A is a diagram illustrating a quadrifilar helical antenna which is open-circuited,
or open terminated, at the far end. For such a configuration, the resonant length
ℓ of the radiators
208 is an odd integer multiple of a quarter-wavelength of the desired resonarit frequency.
[0024] FIG.
2B is a diagram illustrating a quadrifilar helical antenna which is short-circuited,
or electrically connected, at the far end. In this case, the resonant length ℓ of
radiators
208 is an even integer multiple of a quarter wavelength of the desired resonant frequency.
Note that in both cases, the stated resonant length ℓ is approximate, because a small
adjustment is usually needed to compensate for non-ideal short and open terminations.
[0025] FIG.
3 is a diagram illustrating a planar representation of a radiator portion of a quadrinlar
helical antenna, which includes radiators
208 having a length ℓ = λ/2, where λ is the wavelength of the desired resonant frequency
of the antenna. Curve
304 represents the relative magnitude of current for a signal on a radiator
208 that resonates at a frequency of
f = ν/λ, where ν is the velocity of the signal in the medium.
[0026] Example implementations of a quadrifilar helical antenna implemented using printed
circuit board techniques (a strip antenna) are. described in more detail with reference
to FIGS.
4 - 6. The strip quadrifilar helical antenna is comprised of strip radiators
104A-
104D etched onto a dielectric substrate
406. The substrate is a thin flexible material that is rolled into a cylindrical, conical
or other appropriate shape such that radiators
104A-
104D are helically wound about a central axis of the cylinder.
[0027] FIGS.
4 - 6 illustrate the components used to fabricate a quadrifilar helical antenna
100. FIGS.
4 and
5 present a view of a far surface
400 and near surface
500 of substrate
406, respectively. The antenna
100 includes a radiator portion
404, and a feed portion
408.
[0028] In the embodiments described and illustrated herein, the antennas are described as
being made by forming the substrate into a cylindrical shape with the near surface
being on the outer surface of the formed cylinder. In alternative embodiments, the
substrate is formed into the cylindrical shape with the far surface being on the outer
surface of the cylinder.
[0029] In one embodiment, dielectric substrate
406 is a thin, flexible layer of polytetraflouroethylene (PTFE), a PTFE/glass composite,
or other dielectric material. In one embodiment, substrate
406 is on the order of 0.005 in., or 0.13 mm thick, although other thicknesses can be
chosen. Signal traces and ground traces are provided using copper. In alternative
embodiments, other conducting materials can be chosen in place of copper depending
on cost, environmental considerations and other factors.
[0030] In the embodiment illustrated in FIG. 5, feed network
508, 580 is etched onto feed portion
408 to provide the quadrature phase signals (i.e., the 0°, 90°, 180° and 270° signals)
that are provided to radiators
104A-
104D. Feed portion
408 of far surface
400 provides a ground plane
412 for feed circuit
508, 580. Signal traces for feed circuit
508, 580 are etched onto near surface
500 of feed portion
408.
[0031] For purposes of discussion, radiator portion
404 has a first end
432 adjacent to feed portion
408 and a second end
434 (on the opposite end of radiator portion
404). Depending on the antenna embodiment implemented, radiators
104A-
104D can be etched into far surface
400 of radiator portion
404. The length at which radiators
104A-
104D extend from first end
432 toward second end
434 is approximately an integer multiple of a quarter wavelength of the desired resonant
frequency.
[0032] In such an embodiment where radiators
104A-
104D are an integer multiple of λ/2. radiators
104A-
104D are electrically connected to each other (i.e., shorted, or short circuited) at
second end
434. This connection can be made by a conductor across second end
434 which forms a ring
604 around the circumference of the antenna when the substrate is formed into a cylinder.
FIG.
6 is a diagram illustrating a perspective view of an etched substrate of a strip helical
antenna having a shorting ring
604 at second end
434.
[0033] One conventional quadrifilar helical antenna is described in U.S. Patent No. 5,198,831
to Burrell
et.
al. (referred to as the '831 patent). The antenna described in the '831 patent is a
printed circuit-board antenna having the antenna radiators etched or otherwise deposited
on a dielectric substrate. The substrate is formed into a cylinder resulting in a
helical configuration of the radiators.
[0034] Another conventional quadrifilar helical antenna is disclosed in U.S. Patent No.
5,255,005 to Terret
et al (referred to as the '005 patent).
[0035] The antenna described in the '005 patent is a quadrifilar helical antenna formed
by two bifilar helices positioned orthogonally and excited in phase quadrature. The
disclosed antenna also has a second quadrifilar helix that is coaxial and electromagnetically
coupled with the first helix to improve the passband of the antenna.
[0036] Yet another conventional quadrifilar helical antenna is disclosed in U.S. Patent
No. 5,349,365, to Ow
et al (referred to as the '365 patent). The antenna described in the '365 patent is a quadrifilar
helical antenna designed in wireform as described above with reference to FIG.
1A.
IV. Coupled Multi-Segment Helical Antenna
[0037] In order to reduce the length of radiator portion
100 of the antenna, one form of helical antenna utilizes coupled multi-segment radiators
that allow for resonance at a given frequency at shorter lengths than would otherwise
be needed for a helical antenna with an equivalent resonant length.
[0038] FIGS.
7A and
7B are diagrams illustrating planar representations of example embodiments of coupled-segment
helical antennas. FIG.
7A illustrates a coupled multi-segment radiator
706 terminated in an open-circuit according to one single-filar embodiment. An antenna
terminated in an open-circuit such as this may be used in a single-filar, bifilar,
quadrifilar, or other x-filar implementation.
[0039] The embodiment illustrated in FIG.
7A is comprised of a single radiator
706. Radiator
706 is comprised of a set of radiator segments. This set is comprised of two end segments
708, 710 and
p intermediate segments
712, where
p = 0, 1, 2, 3 ... (the case where
p = 3 is illustrated). Intermediate segments are optional (i.e.,
p can equal zero). End segments
708, 710 are physically separate from but electromagnetically coupled to one another. Intermediate
segments
712 are positioned between end segments
708, 710 and provide electromagnetic coupling between end segments
708,
710.
[0040] In the open-terminated embodiment, the length
ℓs1 of segment
708 is an odd-integer multiple of one-quarter wavelength of the desired resonant frequency.
The length
ℓs2 of segment
710 is an integer multiple of one-half the wavelength of the desired resonant frequency.
The length ℓ
sp of each of the
p intermediate segments
712 is an integer multiple of one-half the wavelength of the desired resonant frequency.
In the illustrated embodiment, there are three intermediate segments
712 (i.e.,
p = 3).
[0041] FIG.
7B illustrates radiators
706 of the helical antenna when terminated in a short circuit
722. This short-circuited implementation is not suitable for a single-filar antenna,
but can be used for bifilar, quadrifilar or other x-filar antennas. As with the open-circuited
embodiment, radiators 706 are comprised of a set of radiator segments. This set is
comprised of two end segments
708, 710 and
p intermediate segments
712, where
p = 0, 1, 2, 3 ... (the case where
p = 3 is illustrated). Intermediate segments are optional (i.e.,
p can equal zero). End segments
708, 710 are physically separate from but electromagnetically coupled to one another. Intermediate
segments
712 are positioned between end segments
708, 710 and provide electromagnetic coupling between end segments
708,710.
[0042] In the short-circuited embodiment, the length ℓ
s1 of segment
708 is an odd-integer multiple of one-quarter wavelength of the desired resonant frequency.
The length
ℓs2 of segment
710 is an odd-integer multiple of one-quarter wavelength of the desired resonant frequency.
The length ℓ
sp of each of the
p intermediate segments
712 is an integer multiple of one-half the wavelength of the desired resonant frequency.
In the illustrated embodiment, there are three intermediate segments
712 (i.e.,
p = 3).
[0043] FIGS.
8A and
8B are diagrams illustrating a coupled multi-segment quadrifilar helical antenna radiator
portion
800 according to one embodiment of the invention. FIGS.
8A and
8B illustrate one example implementation of the antenna illustrated in FIG.
7B, where
p = zero (i.e., there are no intermediate segments
712) and the lengths of segments
708, 710 are one-quarter wavelength.
[0044] The radiator portion
800 illustrated in FIG.
8A is a planar representation of a quadrifilar helical antenna, having four coupled
radiators
804. Each coupled radiator
804 in the coupled antenna is actually comprised of two radiator segments
708, 710 positioned in close proximity with one another such that the energy in radiator segment
708 is coupled to the other radiator segment
710.
[0045] More specifically, according to one embodiment, radiator portion
800 can be described in terms of having two sections
820, 824. Section
820 is comprised of a plurality of radiator segments
708 extending from a first end
832 of the radiator portion
800 toward the second end
834 of radiator portion
800. Section
824 is comprised of a second plurality of radiator segments
710 extending from second end
834 of the radiator portion
800 toward first end
832. Toward the center area of radiator portion
800, a part of each segment
708 is in close proximity to an adjacent segment
710 such that energy from one segment is coupled into the adjacent segment in the area
of proximity. This is referred to in this document as overlap.
[0046] In a preferred embodiment, each segment
708, 710 is of a length of approximately ℓ
1 = ℓ
2 = λ/4. The overall length of a single radiator comprising two segments
708, 710 is defined as ℓ
tot. The amount one segment
708 overlaps another segment
710 is defined as δ = ℓ
1 + ℓ
2 - ℓ
tot.
[0047] For a resonant frequency
f = υ/λ the overall length of a radiator
ℓtot is less than the half-wavelength length of λ/2. In other words, as a result of coupling,
a radiator, comprising a pair of coupled segments
708, 710, resonates at frequency
f = υ/λ even though the overall length of that radiator is less than a length of λ/2.
Therefore, the radiator portion
800 of a ½ wavelength coupled multi-segment quadrifilar helical antenna is shorter than
the radiator portion of conventional half-wavelength quadrifilar helical antenna
800 for a given frequency
f.
[0048] For a clearer illustration of the reduction in size gained by using the coupled configuration,
compare the radiator portions
800 illustrated in FIG
8 with those illustrated in FIG.
3. For a given frequency
f = υ/λ, the length ℓ of radiator portion
300 of the conventional antenna is λ/2, while the length
ℓtot of radiator portion
800 of the coupled radiator segment antenna is less than λ/2.
[0049] As stated above, in one embodiment, segments
708, 710 are of a length ℓ
1 = ℓ
2 = λ/4. The length of each segment can be varied such that ℓ
1 is not necessarily equal to ℓ
2, and such that they are not equal to λ/4. The actual resonant frequency of each radiator
is a function of the length of radiator segments
708, 710 the separation distance s between radiator segments
708,
710 and the amount by which segments
708, 710 overlap each other.
[0050] Note that changing the length of one segment
708 with respect to the other segment
710 can be used to adjust the bandwidth of the antenna. For example, lengthening ℓ
1 such that it is slightly greater than λ/4 and shortening ℓ
2 such that it is slightly shorter than λ/4 can increase the bandwidth of the antenna.
[0051] FIG.
8B illustrates the actual helical configuration of a coupled multi-segment quadrifilar
helical antenna according to one embodiment of the invention. This illustrates how
each radiator is comprised of two segments
708, 710 in one embodiment. Segment
708 extends in a helical fashion from first end
832 of the radiator portion toward second end
834 of the radiator portion. Segment
710 extends in a helical fashion from second end
834 of the radiator portion toward first end
832 of the radiator portion. FIG.
8B further illustrates that a portion of segments
708, 710 overlap such that they are electromagnetically coupled to one another.
[0052] FIG.
9A is a diagram illustrating the separation s and overlap δ between radiator segments
708, 710. Separation s is chosen such that a sufficient amount of energy is coupled between
the radiator segments
708, 710 to allow them to function as a single radiator of an effective electrical length
of approximately λ/2 and integer multiples thereof.
[0053] Spacing of radiator segments
708, 710 closer than this optimum spacing results in greater coupling between segments
708,
710. As a result, for a given frequency
f the length of segments
708, 710 must increase to enable resonance at the same frequency
f. This can be illustrated by the extreme case of segments
708, 710 being physically connected (i.e.,
s = 0). In this extreme case, the total length of segments
708, 710 must equal λ/2 for the antenna to resonate. Note that in this extreme case, the antenna
is no longer really 'coupled' according to the usage of the term in this specification,
and the resulting configuration is actually that of a conventional helical antenna
such as that illustrated in FIG.
3.
[0054] Similarly, increasing the amount of overlap δ of segments
708, 710 increases the coupling. Thus as overlap δ increases, the length of segments
708, 710 increases as well.
[0055] To qualitatively understand the optimum overlap and spacing for segments
708, 710, refer to FIG.
9B. FIG.
9B represents a magnitude of the current on each segment
708, 710. Current strength indicators
911, 928 illustrate that each segment ideally resonates at λ/4, with the maximum signal strength
at the outer ends and the minimum at the inner ends.
[0056] To optimize antenna configurations for the coupled radiator segment antenna, the
inventors utilized modeling software to determine correct segment length ℓ
1, ℓ
2, overlap δ, and spacing s among other parameters. One such software package is the
Antenna Optimizer (AO) software package. AO is based on a method of moments electromagnetic
antenna-modeling algorithm. AO Antenna Optimizer version 6.35, copyright 1994, was
written by and is available from Brian Beezley, of San Diego, California.
[0057] Note that there are certain advantages obtained by using a coupled configuration
as described above with reference to FIGS.
8A and
8B. With both the conventional antenna and the coupled radiator segment antenna, current
is concentrated at the ends of the radiators. Pursuant to array factor theory, this
can be used to an advantage with the coupled radiator segment antenna in certain applications.
[0058] To explain, FIG.
10A is a diagram illustrating two point sources, A, B, where source A is radiating a
signal having a magnitude equal to that of the signal of source B but lagging in phase
by 90° (the
ejωt convention is assumed). Where sources A and B are separated by a distance of λ/4,
the signals add in phase in the direction traveling from A to B, and add out of phase
in the direction from B to A. As a result, very little radiation is emitted in the
direction from B to A. A typical representative field pattern shown in FIG.
10B illustrates this point.
[0059] Thus, when the sources A and B are oriented such that the direction from A to B points
upward, away from the ground, and the direction from B to A points toward the ground,
the antenna is optimized for most applications. This is because it is rare that a
user desires an antenna that directs signal strength toward the ground. This configuration
is especially useful for satellite communications where it is desired that the majority
of the signal strength be directed upward, away from the ground.
[0060] The point source antenna modeled in FIG.
10A is not readily achievable using conventional half wavelength helical antennas. Consider
the antenna radiator portion illustrated in FIG.
3. The concentration of current strength at the ends of radiators
208 roughly approximates a point source. When radiators are twisted into a helical configuration,
one end of the 90° radiator is positioned in line with the other end of the 0° radiator.
Thus, this approximates two point sources in a line. However, these approximate point
sources are separated by approximately λ/2 as opposed to the desired λ/4 configuration
illustrated in FIG.
10A.
[0061] Note, however that the coupled radiator segment antenna embodying the invention provides
an implementation where the approximated point sources are spaced at a distance closer
to λ/4. Therefore, the coupled radiator segment antenna allows users to capitalize
on the directional characteristics of the antenna illustrated in FIG.
10A.
[0062] The radiator segments
708, 710 illustrated in FIG.
8 show that segment
708 is very near its associated segment
710, yet each pair of segments
708, 710 are relatively far from the adjacent pair of segments. In one alternative embodiment,
each segment
710 is placed equidistant from the segments
708 on either side. This embodiment is illustrated in FIG.
11.
[0063] Referring now to FIG.
11, each segment is substantially equidistant from each pair of adjacent segments. For
example, segment
708B is equidistant from segments
710A,
710B. That is,
s1 =
s2. Similarly, segment
710A is equidistant from segments
708A,
708B.
[0064] This embodiment is counterintuitive in that it appears as if unwanted coupling would
exist. In other words, a segment corresponding to one phase would couple not only
to the appropriate segment of the same phase, but also to the adjacent segment of
the shifted phase. For example, segment
708B, the 90° segment would couple to segment
710A (the 0° segment) and to segment
710B (the 90° segment). Such coupling is not a problem because the radiation from the
top segments
710 can be thought of as two separate modes. One mode resulting from coupling to adjacent
segments to the left and the other mode from coupling to adjacent segments to the
right. However, both of these modes are phased to provide radiation in the same direction.
Therefore, this double-coupling is not detrimental to the operation of the coupled
multi-segment antenna.
[0065] FIG.
12 is a diagram illustrating an example implementation of a coupled radiator segment
antenna. Referring now to FIG.
12, the antenna comprises a radiator portion
1202 and a feed portion
1206. Radiator portion includes segments
708, 710. Dimensions provided in FIG.
12 illustrate the contribution of segments
708, 710 and the amount of overlap δ to the overall length of radiator portion
1202.
[0066] The length of segments in a direction parallel to the axis of the cylinder is illustrated
as ℓ
1sinα for segments
708 and ℓ
2sinα for segments
710, where α is the inside angle of segments
708, 710.
[0067] Segment overlap as illustrated above in FIGS.
8A and
9A, is illustrated by the reference character δ. The amount of overlap in a direction
parallel to the axis of the antenna is given by δsinα, as illustrated in FIG.
12.
[0068] Segments
708, 710 are separated by a spacing
s, which can vary as described above. The distance between the end of a segment
708, 710 and the end of radiator portion
1202 is defined as the gap and illustrated by the reference characters γ
1, γ
2, respectively. The gaps γ
1, γ
2 can, but do not have to be, equal to each other. Again, as described above, the length
of segments
708 can be varied with respect to that of segments
710.
[0069] The amount of offset of a segment
710 from one end to the next is illustrated by the reference character ω
0. The separation between adjacent segments
710 is illustrated by the reference character ω
s, and is determined by the helix diameter.
[0070] Feed portion
1206 includes an appropriate feed network to provide the quadrature phase signals to the
radiator segments
708. Feed networks are well known to those of ordinary skill in the art and are thus not
described in detail herein.
[0071] In the example illustrated in FIG.
12, segments
708 are fed at a feed point that is positioned along each segment
708 a distance from the feed network that is chosen to optimize impedance matching. In
the embodiment illustrated in FIG.
12, this distance is illustrated by the reference characters δ
feed.
[0072] Note that continuous line
1224 illustrates the border for a ground portion on the far surface of the substrate.
The ground portion opposite segments
708 on the far surface extends to the feed point. The thin portion of segments
708 is on the near surface. At the feed point, the thickness of segments
708 on the near surface increases.
[0073] Dimensions are now provided for an example coupled radiator segment quadrifilar helical
antenna suitable for operation in the L-Band at approximately 1.6 GHz. Note that this
is an example only and other dimensions are possible for operation in the L-Band.
Additionally, other dimensions are possible for operation in other frequency bands
as well.
[0074] The overall length of radiator portion
1202 in the example L-Band embodiment is 2.30 inches (58.4 mm). In this embodiment, the
pitch angle α is 73 degrees. With this angle α, the length of segments
708 ℓ
1sinα for this embodiment is 1.73 inches (43.9 mm). In the embodiment illustrated,
the length of segments
710 is equal to the length of segments
708.
[0075] In one example, segment
710 is positioned substantially equidistant from its adjacent pair of segments
708. In one implementation of the embodiment where segments
710 are equidistant from adjacent segments
708, the spacing
s1 =
s2 = 0.086 inches (2.2 mm). Other spacings are possible including, for example, the
spacing s of segments
710 at 0.070 inches (1.8 mm) from an adjacent segment
708.
[0076] The width τ of radiator segments
708,
710 is 0.11 inches (2.8 mm) in this embodiment. Other widths are possible.
[0077] The example L-Band embodiment features a symmetric gap γ
1 = γ
2 = 0.57 inches (14.5 mm). Where the gap γ is symmetric for both ends of the radiator
portion
1202 (i.e., where γ
1 = γ
2), the radiators
708, 710 have an overlap δsinα of 1.16 inches (29.5 mm) (1.73 inches - 0.57 inches).
[0078] The segment offset ω
0 is 0.53 inches and the segment separation ω
s is 0.393 inches (10.0 mm). The diameter of the antenna is 4ω
s/π.
[0079] In one embodiment, this is chosen such that the distance δ
feed from the feed point to the feed network is δ
feed = 1.57 inches (39.9 mm). Other feed points can be chosen to optimize impedance matching.
[0080] Note that the example embodiment described above is designed for use in conjunction
with a 0.032 inch thick polycarbonate radome enclosing the helical antenna and contacting
the radiator portion. It will become apparent to a person skilled in the art how a
radome or other structure affects the wavelength of a desired frequency.
[0081] Note that in the example embodiments just described, the overall length of the L-Band
antenna radiator portion is reduced from that of a conventional half-wavelength L-Band
antenna. For a conventional half-wavelength L-Band antenna, the length of the radiator
portion is approximately 3.2 inches (i.e., λ/2(sinα)), where α is the inside angle
of segments
708, 710 with respect to the horizontal), or (81.3 mm). For the example embodiments described
above, the overall length of the radiator portion
1202 is 2.3 inches (58.42 mm). This represents a substantial savings in size over the
conventional antenna.
V. Stacked Dual-Band Helical Antenna
[0082] Having thus described several embodiments of a single-band helical antenna, a dual-band
helical antenna embodying the present invention is now described. The present invention
is directed toward a dual-band helical antenna capable of resonating at two different
operating frequencies. Two helical antennas are stacked end to end, with one antenna
resonating at a first frequency and the other antenna resonating at a second frequency.
Each antenna has a radiator portion comprised of one or more helically-wound radiators.
Each antenna also has a feed portion comprised of a feed network and a ground plane.
The two antennas are stacked such that the ground plane of one antenna is used as
a shorting ring across the far end of the radiators of the other antenna.
[0083] FIG.
13 is a diagram illustrating planar representations of far surface
400 and near surface
500 of a dual-band helical antenna according to one embodiment of the invention. The
dual-band helical antenna is comprised of two single-band helical antennas: helical
antenna
1304 operating at a first resonant frequency and helical antenna
1308 operating at a second resonant frequency.
[0084] In the embodiment illustrated in FIG.
13, feed network
508, radiators
104A-
104D and first antenna
1304 are disposed on near surface
500 of first antenna
1304. Also disposed on near surface
500 is the ground plane
412 for the feed network
508 of second antenna
1308. On far surface
400 are feed network
508 and radiators
104A-
104D of second antenna
1308 as well as ground plane
412 for the feed portion of first antenna
1304.
[0085] As discussed above with reference to FIGS.
2A and
2B, where the resonant length ℓ of radiators
104A-
104D is an even integer multiple of a quarter-wavelength of the desired resonant frequency,
the far end of the radiators
104A-
104D is shorted. As illustrated in FIG.
13, this shorting is accomplished using ground plane
412 of first antenna
1304. As a result of this configuration, an additional shorting ring does not need to be
added to the end of radiators
104A-
104D.
[0086] Note that in the embodiment illustrated in FIG.
13, first antenna
1304 is illustrated as resonating at odd integer multiples of a quarter-wavelength of
the desired resonant frequency because the ends of radiators
104A-
104D are open circuited. In an alternative embodiment, a shorting ring (not illustrated)
could be added to the far end of radiators
104A-
104D of first antenna
1304, while changing the length of these radiators
104A-
104D such that they are an even-integer multiple of a quarter-wavelength of the desired
resonant frequency.
[0087] Radiators
104A-
104D of the dual-band antenna described with reference to FIG.
13 are illustrated as being fed at a first end near feed network
508. It is well known that a feed point of radiators
104A-
104D of the helical antenna can be positioned at any point along the length of radiators
104A-
104D where such positioning is primarily determined based on impedance matching considerations.
FIG.
14 is a diagram illustrating one embodiment of a dual-band helical antenna in which
the feed points of radiators
104A-
104D are positioned at a predetermined distance from feed network
508. Specifically, in the embodiment illustrated in FIG.
14, a feed point A of first antenna
1304 is positioned at a distance ℓ
FEED1 from feed network
508 and feed point B of second antenna
1308 is positioned at a distance ℓ
FEED2 from feed network
508.
[0088] This embodiment illustrates that radiators
104A-
104D are comprised of a ground trace
1436 on a first surface of the substrate
406, a feed trace
1438 on a second surface of substrate
406 and opposite said ground trace
1436, and a radiator trace
1440 on the second surface of substrate
406.
[0089] As with the embodiment illustrated in FIG.
13, in this embodiment, ground plane
412 of first antenna
1304 serves as a shorting ring for radiators
104A-
104D and second antenna
1308, such that the radiators of second antenna
1308 resonate at an even integer multiple of a quarter-wavelength of the desired resonant
frequency.
[0090] In order to decrease the overall length of the stacked antenna, the edge-coupled
technology discussed above can be utilized. In such embodiments, radiators
104A-
104D of first antenna
1304 and/or second antenna
1308 as illustrated in FIGS.
13 and
14 are replaced with edge-coupled radiators as illustrated, for example, in FIG.
12.
[0091] One challenge of providing a dual-band antenna such as that illustrated in FIGS.
13 and
14 is that of feeding first antenna
1304. To this end, first antenna
1304 is fed by means of a tab extending from the lower area of the feed portion of first
antenna
1304.
[0092] FIG.
15 is a diagram illustrating such a tab used to feed first antenna
1304. Referring now to FIG.
15, a tab
1504 extends from the side of the feed portion of first antenna
1304 on substrate
406. In the embodiment illustrated in FIG.
15, tab
1504 is approximately "L" shaped such that it extends horizontally from the feed portion
of first antenna
1304 at a given distance and is then angled axially through the center in the direction
of the feed portion of second antenna
1308. Although
1504 is illustrated as being shaped with a right angle, other angles could be used as
could curves of various radii.
[0093] Ideally, when substrate
406 is rolled into a cylinder or other appropriate shape to form the helical antenna,
axial component
1524 of tab
1504 is substantially along the axis of the dual-band helical antenna. Having axial component
1524 of tab
1504 coincident with the axis of the helical antenna minimizes the impact of this member
on the radiation patterns of the antenna. As illustrated in FIG.
15, in a preferred embodiment, tab
1504 extends from feed portion of first antenna
1304 at a vertical position that is as far as possible from first antenna
1304. This is done to minimize the effect of tab
1504 on the radiation patterns of first antenna
1304. Because second antenna
1308 is a coupled-segment one-half wavelength antenna and the ends of radiators
104A-
104D of second antenna
1308 are shorted by ground plane
412 of first antenna
1304, tab
1504 has a minimal effect on the radiation patterns of second antenna
1308.
[0094] Preferably, the length ℓ
gp of feed portion
1206 of first antenna
1304 can be determined by considering two factors at the appropriate operating frequency.
First, it is desirable to minimize the amount of current flowing from the radiators
of first antenna
1304 to second antenna
1308, and vice versa. In other words, it is desirable to achieve isolation between the
two antennas. This can be accomplished by ensuring that the length is great enough
such that the currents do not extend from one set of radiators to the other at the
frequency of interest.
[0095] Another challenge is the goal of not allowing current from radiators
104A-D of first antenna
1304 from reaching tab
1504. Currents from first antenna
1304 are attenuated as they travel across the feed portion of first antenna
1304 toward tab
1504. Tab
1504 creates an asymmetrical discontinuity in these currents. Therefore, it is desired
to minimize the magnitude of the currents reaching tab
1504 to the extent practical.
[0096] After reading this description, it will become apparent to a person skilled in the
art how to implement feed portion
1206 of appropriate length
ℓgp based on the materials used, the frequencies of interest, the expected power levels
in the antenna, and other known factors. This decision may also entail a tradeoff
between size and performance.
[0097] Note that the effects of tab
1504 are not non-existent in this embodiment. Because tab
1504 is close to the radiators of second antenna
1308, some current from second antenna
1308 is coupled into tab
1504, and, therefore, along the axis of the antenna. This current affects the radiation
of second antenna
1308, resulting in increased radiation to the sides of the antenna. For applications where
the antenna is mounted vertically, this results in increased radiation in the direction
of the horizon and decreased radiation in the vertical direction. As a result, this
application is well-suited for satellite communication systems where low-earth-orbiting
satellites are used to relay communications from or to the communication device.
[0098] This effect is illustrated in FIG.
10C, where circular polarization radiation pattern
1010 is a representation of a typical radiation pattern for a conventional helical antenna,
and radiation pattern
1020 is a representation of a radiation pattern for second antenna
1308. As FIG.
10C illustrates, pattern
1020 is "flatter" and "wider" than conventional pattern
1010.
[0099] To enable coupling of a signal to first antenna
1304, tab
1504 includes a connector such as a crimp or solder connector or other connector suitable
for making a connection between a feed cable and the signal trace on tab
1504. Various types of cable or wire can be used to connect transceiver RF circuitry to
the antenna at tab
1504. Preferably, a low loss flexible or semi-rigid cable is utilized. Of course, as is
well known in the antenna art, it is desired to match the impedance of the feed input
with that of the interface cable to maximize power transfer to the antenna. However,
if the input transition is poor, the radiation patterns will still be symmetric, only
their gains will be lowered by the corresponding amount of reflection loss. In addition
to a low insertion loss, it is also important that the connector provide a sturdy
mechanical connection between the cable and tab
1504.
[0100] Also illustrated in FIG.
15 is the outline for an example substrate shape. After reading this description, it
will become apparent to a person skilled in the art how to implement the antenna with
a tab
1504 utilizing substrates having other shapes.
[0101] FIG.
16 is a diagram illustrating one embodiment of a stacked antenna with example dimensions.
In this embodiment, first antenna
1304 is an L-band antenna and second antenna
1308 is an S-band antenna. In this embodiment, S-band antenna
1308 is an edge-coupled antenna wherein each radiator
104 is comprised of two segments. Note that this embodiment is provided for example only.
Alternative frequency bands can be chosen for operation. Also note that either first
antenna
1304 or second antenna
1308 or both could utilize the edge-coupled technology.
[0102] Example dimensions are now described for the L-band and S-band antenna illustrated
in FIG.
16. The radiating aperture of the L-band antenna is a total axial height of 1.253 inches,
while the S-band aperture is a total height of 1.400 inches. In this embodiment, the
height of feed portion
412 of first antenna
1304 is 0.400 inches. This yields a total radiating aperture of 3.093 inches. The inclination
angle of radiators
104A-
104D is 65°.
[0103] The above dimensions are provided by way of example only. As discussed above with
reference to conventional helical antennas, the overall length of radiators
104A-
104D determines the precise resonating frequency of the antenna. The resonating frequency
is important because the highest average gains and the most symmetric patterns occur
at the resonant frequency. If the antenna is made longer, the resonating frequency
shifts down. Conversely, if the antenna is made shorter, the resonating frequency
shifts up. The percentage of the frequency shift is approximately proportional to
the percentage that the radiators
104A-
104D are lengthened or shortened. At L-band operating frequencies, roughly 1 mm of length
in the direction of the antenna axis corresponds to 1 MHz.
[0104] In the illustrated embodiment, both first antenna
1304 and second antenna
1308 have four excited filar arms, or radiators
104A-
104D. Each of these radiators 104A-104D are fed in phase quadrature. The quadrature phase
excitation of four radiators
104A-
104D for each antenna
1304,
1308 is implemented using a feed network. While conventional feed networks capable of
providing quadrature phase excitation can be implemented, a preferred feed network
is discussed in detail below.
[0105] Another important dimension is the feedpoint axial length. The feedpoint axial length
defines the distance of the feedpoint from the feed network for embodiments where
the feedpoint is positioned along radiators
104A-
104D as illustrated in FIG.
13. The feedpoint axial length dimension indicates the position at which the microstrip
flares out to continue the radiator and is actually the feedpoint position for the
entire radiator
104. In the example illustrated in FIG.
16, the feedpoint length for first antenna
1304 is 1.133 inches (28.8 mm). The feedpoint length for second antenna
1308 is 0.638 inches (16.2 mm). These dimensions yield 50 ohm impedances at 1618 and 2492
MHz, respectively. If the feedpoint position is shifted lower, the impedance is lower.
Conversely, if the feedpoint position is shifted higher, the impedance is higher.
It is important to note that when the overall radiator length is being adjusted to
tune the frequency, the feedpoint position should also be shifted by a proportional
amount in the direction along the axis of the antenna to maintain the correct impedance
match.
[0106] Preferably, the antenna having dimensions as illustrated in FIG.
16 is rolled into a cylinder having a diameter of 0.500 inches (12.7 mm).
VI. Feed Network
[0107] The helical antennas described in this document can be implemented using a mono-filar,
quadrifilar, octafilar or other x-filar configuration. A feed network is utilized
to provide the signals to the filars at the necessary phase angle. The feed network
splits the signal and shifts the phase provided to each filar. The configuration of
the feed network is dependent on the number of filars. For example, for a quadrifilar
helical antenna, the feed network provides four equal-power signals in a quadrature
phase relationship (i.e., 0, 90, 180, and 270 degrees).
[0108] To conserve space on the feed portion of the antenna a unique feed network layout
may be utilized. The traces of the feed network extend into one or more radiators
104A-
104D of the antenna. For convenience, the feed network is described in terms of a feed
network designed to provide four equal-power signals in a quadrature phase relationship.
After reading this description, it will become apparent to a person skilled in the
relevant art how to implement the feed network for other x-filar configurations.
[0109] FIG.
17 illustrates the electrical equivalent of a conventional quadrature phase feed network.
For conventional quadrature phase feed networks, the network provides four equal-power
signals, each separated in phase by 90 degrees. The signal is provided to the feed
network via a first signal path
1704. At a first signal point A (referred to as a secondary feed point), the 0-degree phase
signal is provided to a first radiator
104. At signal point B, the 90-degree phase signal is provided to a second radiator
104. At signal points C and D, the 180- and 270-degree phase signals are provided to
third and fourth radiators
104.
[0110] Signals A and B are combined at a point P2 to yield a 25-ohm impedance. Likewise,
signals C and D are combined at a point P3 to yield a 25-ohm impedance. These signals
are combined at P1 to yield a 12.5-ohm impedance. Therefore, a 25-ohm, 90-degree transformer
is placed at the input to convert this impedance to 50-ohms. Note that in the network
illustrated in FIG.
17, part of the transformer is placed before the P1 split to shorten the feed and also
to decrease losses. However, because it is before the split, it must be twice the
impedance after the split.
[0111] The conventional feed network is modified such that the traces of the feed network
are disposed on portions of the substrate defined for radiators
104A-
104D. Specifically, in a preferred embodiment, these traces are disposed on the substrate
in an area which is opposite from the ground traces of the one or more of the radiators
104A-
104D.
[0112] FIG.
18 is a diagram illustrating an example embodiment of the feed network in a quadrifilar
helical antenna environment. Specifically, in the example illustrated in FIG.
18, two feed networks are illustrated: a first feed network
1804 for implementation with first antenna
1304; and a second feed network
1808 for implementation with second antenna
1308. Feed networks
1804,1808 have points A, B, C, and D, for providing the 0, 90,180, and 270-degree signals to
radiators
104A-
104D. The dashed lines provided on FIG.
18 approximately illustrate an outline for the ground plane of radiators
104A-
104D on a surface of the substrate opposite the surface on which feed networks
1804,1808 are disposed. Thus, FIG. 18 illustrates those portions of feed networks
1804, 1808 which are disposed on, or extend into, radiators
104A-
104D.
[0113] Note that according to conventional wisdom, the feed network is provided on an area
that is designated for the feed network and that is separate from the radiators. In
contrast, the feed network described herein is laid out such that a portion of the
feed network is deposited on the radiator portion of the antenna. As such, the feed
portion of the antenna can be reduced in size in comparison to the feed portion for
a conventional feed networks.
[0114] FIG.
19 is a diagram illustrating feed networks
1804, 1808 along with the signal traces, including the feed paths, for antennas
1304, 1308. FIG.
20 illustrates an outline for the ground plane of antennas
1304, 1308. FIG.
21 is a diagram illustrating both the ground planes and the signal traces superimposed.
[0115] An advantage of these feed networks is that the area required for the feed portion
of the antenna to implement a feed network is reduced over conventional feeding techniques.
This is because portions of the feed network which would otherwise be disposed on
the feed portion of the antenna are now disposed on the radiator portion of the antenna.
As a result of this, the overall length of the antenna can be reduced.
[0116] An additional advantage of such a feed network is that because the secondary feed
point is moved closer to the feed point of the antenna, transmission line loss is
decreased. Additionally, a transformer can be integrated into the routing line of
the feed network for impedance matching.
[0117] Thus, an area-efficient network is configured such that a section of the feed network
is disposed on a radiator portion of an antenna and the remainder of the feed network
is disposed on a feed portion. Because part of the feed network is disposed on the
radiator portion, the remainder of the feed network requires less area on the feed
portion. As a result, the feed portion of the antenna can be smaller as compared to
antennas having conventional feed networks. Preferably, the traces of the feed network
that are disposed on the radiator portion are disposed opposite the ground portion
of the radiators. As such, the ground portion of the radiators serves as a ground
plane for this part of the feed network. The area-efficient feed network can be implemented
with numerous different types of antennas of varying configurations, including single-band
and multi-band helical antennas. As a result of this configuration, the overall size
of the antenna and the amount of loss in the feed are reduced as compared to antennas
having conventional feed networks.
VII. Antenna Assembly
[0118] As described above, one technique for manufacturing helical antennas is to dispose
radiators, feed networks and ground traces on a substrate and to wrap the substrate
in an appropriate shape. Although the above-described antenna configurations can be
implemented using conventional techniques for wrapping the substrate in the appropriate
shape, an improved structure and technique for wrapping the substrate is now described.
[0119] FIG.
22A is a diagram illustrating one embodiment of a structure used to maintain the substrate
in an appropriate (e.g., cylindrical) shape. More specifically, FIG.
22A illustrates an example structure added to an antenna having an area efficient feed
network After reading this description, it will become apparent to a person skilled
in the relevant art how to implement the invention with helical antennas of other
configurations.
[0120] FIGS.
22B through
22F depict cross-sectional views of an example structure used to hold the antenna in
a cylindrical or other appropriate shape. Referring now to FIGS.
22A through
22F, the example includes a metallic strip
2218 on, or as an extension of, ground plane
412, solder material
2216 opposite metallic strip
2218, and one or more vias
2210.
[0121] Metallic strip
2218 can be comprised of a portion of ground plane
412, or a metallic strip added to ground plane
412. Preferably, in one embodiment, metallic strip
2218 is provided by merely extending the width of ground plane
412 by a predetermined amount. In the embodiment illustrated in FIG.
22A, this width is shown by ω
strip.
[0122] A series of vias
2210 are provided in ground plane
412 in the area of metallic strip
2218. Preferably, for a solid connection, the vias
2210 are added to radiator portions of both first antenna
1304 and second antenna
1308. The pattern chosen for vias
2210 is based on known mechanical and electrical properties of the materials used. While
the invention can be implemented with only one or two vias
2210 on each ground plane
412, to obtain a desired level of mechanical strength and electrical connection, several
vias
2210 may be employed. While not necessary, the portion of each ground plane
412 used can extend laterally, or circumferentially, beyond the antenna radiators.
[0123] As seen in FIG.
22B, vias
2210 extend completely through the material of ground plane
412 and through support substrate
406 (
100) from one surface to the next The vias are manufactured as metallized or metal coated
vias using well known techniques in the art. A relatively small portion or region
of an opposite edge
2214 of ground plane
412 is coated with solder material
2216.
[0124] The embodiments illustrated in FIGS.
22B and
22D, include a small metallic strip
2218 formed on substrate
406 on the opposite side from ground plane
412, but adjacent to first edge
2212. In this embodiment, the vias extend through the substrate to metallic strip
2218. While metallic strip
2218 is not necessary in all applications, it will be readily apparent to those skilled
in the art that metallic strip
2218 facilitates solder flow and improved mechanical bonding. A specific material for
manufacturing metallic strip
2218 is chosen according to known principles based on the ground plane material being
used, the solder chosen, and so forth.
[0125] When the antenna support substrate is rolled into the generally cylindrical shape
to form desired helical antenna structures, edges
2212 and
2214 are brought into close proximity with one another as illustrated in FIG.
22D. Vias
2210 and metallic strip
2218 (if provided) are positioned to overlap solder material
2216 on opposite ground plane edge
2214. Heat is applied using well known soldering techniques and equipment while strip
2218 is held in contact with solder material
2216.
[0126] As solder material
2216 is melted, it flows into vias
2210 and onto metallic strip
2218. The heat is then reduced or removed, and the solder forms a permanent, but removable
or serviceable, joint or bond between the two outer edges or ends of ground plane
412. In this manner, the antenna support substrate
406 and the antenna components deposited thereon are now mechanically held in the desired
cylindrical form without requiring other materials such as dielectric tape, adhesives,
or the like. This reduces the time, cost, and labor previously required to assemble
a helical antenna of this type. This may also allow increased automation of this operation
and provide more; readily reproducible antenna dimensions. In addition, one edge of
ground plane
412 is now electrically connected to the other edge, providing a continuous conductive
ring from the ground plane, as desired. This electrical connection is accomplished
without complicated soldering or connecting wires.
[0127] This technique can also be extended to provide support or engagement along other
portions of the antenna. For example, a series of one or more metallic pads or strips
2220 can be deposited at spaced apart locations along the length of one or both sets of
antenna radiators. As seen in FIG.
22E, the metallic pads or strips
2220 are positioned adjacent one or more radiators
104A-D but on the opposite side of support substrate
406 (
100). These pads or strips are positioned so that when the antenna substrate is rolled
or curved to produce the desired antenna, as seen in FIG.
22F, metallic pads or strips
2220 are positioned over a portion of radiators
104A-D on the opposite edge of the support substrate. Specifically, in one embodiment,
metallic pads or strips
220 are positioned over a ground trace 1436 of radiators
104A-D. Metallized vias may be formed in pads
2220 where desired for the application or to improve transfer of heat to melt the solder.
[0128] If a small amount of solder
2226 is previously applied to a mating portion on the surface of ground trace
1436, it can be used to join these radiators to the strips. This provides additional joints
or bonding points which efficiently hold the antenna structure together in the desired
form. Where electrical connection is desired, metallized vias can be formed in the
pads or strips which extend through to the opposite side. These pads can be used in
conjunction with or without the strips previously discussed for the ground planes.
Such a structure is especially useful where very long radiators, or multiple stacks
of antenna radiators are contemplated which result in tall antenna structures.
[0129] FIGS.
23A -
23C illustrate a series of views of an example embodiment of a form
2310 used for rolling substrate
406 into the desired shape. The example illustrated in FIG. 23 is a form
2310 of cylindrical shape used in rolling the antenna and to provide continued support
and rigidity for the antenna structure. In one embodiment, form
2310 can be provided with a series of prongs or teeth
2312 extending radially outward from an outer surface of form
2310. To interface with form
2310 and teeth
2312, a series of "tooling" or assembly guide" holes or passages
2230 are provided in substrate
406 for mating with teeth
2312.
[0130] In FIG.
22A, tooling holes
2230 are illustrated as being positioned within ground planes
412. The metallic material of ground plane
412 acts to reinforce the holes and prevent deformation and movement when a relatively
soft support substrate material is used. This assists with alignment accuracy for
the antenna structure. However, there is no requirement for holes
2230 to be placed within a metallic layer.
[0131] Referring again to FIGS.
23A -
23C, and commencing with the perspective view of FIG.
23A, substrate
406 is shown positioned to engage a support form 2310 by mating teeth
2312 with holes
2230. As seen in the side views of FIG.
23B and
23C, as support form
2310 is rotated about its axis, or substrate
406 is otherwise wrapped around support form
2310, holes
2230 engage teeth
2312 which help position substrate
406 in place against or on support from
2310. Eventually, the entire substrate
406 is engaged against support form
2310. In FIG.
23C, substrate
406 is illustrated as having been wrapped around support form
2310 until it overlaps itself so that strips
2218,
2220 engage solder
2216, 2226 as described above.
[0132] Of course, where strips
2218,
2220 and solder
2216, 2226 are not used to join the substrate sections, substrate
406 does not need to overlap on support form
2310. Additionally, there is no requirement that support form
2310 extend the entire length of the antenna(s), radiators
104A-D or substrate
406. In some applications, some or all of the portions of the antenna may be self supporting,
without the need for a form
2310. This feature can be advantageous, for example, to minimize the impact of the form
2310 on radiation patterns at certain frequencies.
[0133] For purposes of clarity and ease of illustration, in FIGS.
23A -
23C, only substrate
406 is shown, without material layers for ground planes, radiators, feeds, feed networks,
and so forth. It will also be readily apparent to those skilled in the relevant art
how to size holes
2230 to match the dimensions of teeth
2312.
[0134] Form
2310, as illustrated in FIG.
23, can be constructed using a solid or hollow structure formed in a cylindrical or
other desired shape, with teeth or prongs
2312 protruding therefrom. In this embodiment, form
2310 can be thought of, for example, as a variation of the toothed drum found in many
music boxes. As would be apparent to one of ordinary skill in the art after reading
this disclosure, alternative structures can be implemented to provide form
2310 including an axle/spoke arrangement, an axle/sprocket arrangement, or other appropriate
configuration.
[0135] Note that it is contemplated that the spacing of the prongs
2312 or spokes may not be symmetrical about the support element. That is, the spacing
may be larger in some portions in order to impart a greater amount of consistent tension
in rolling, and smaller in some areas to better control substrate positioning where
the substrate edges overlap. Preferably tooth spacing is chosen such that teeth
2312 apply a certain amount of tension to hold substrate
406 in place and to make the entire assembly a more rigid structure.
[0136] The use of holes
2230 and teeth
2312 provide improved manufacturing capabilities through position and assembly automation,
and in precision placement or positioning of the substrate on a form that can be mounted
within an antenna radome. This allows more precise structural definition and positioning
of the antenna assembly, resulting in more precise control and compensation for the
impact of the radome on radiation patterns.
[0137] The above description of the placement of metallic strips
2218, solder material
2216, and vias
2210 is provided by way of example. After reading this description, it would be apparent
to a person skilled in the art how these components could be placed in alternative
locations depending on the configuration desired. For example, these components can
be positioned such that the antenna can be rolled to have right-hand or left-hand
circular polarization and to have the radiators
104A-D on either the inside or the outside of the shape.
VIII. Conclusion
[0138] While various embodiments of the present invention have been described above, it
should be understood that they have been presented by way of example only, and not
limitation. Thus, the breadth and scope of the present invention should not be limited
by any of the above-described exemplary embodiments, but should be defined only in
accordance with the following claims.