(Ham Radio) Schantz - Uwb Magnetic Antennas (Ieee Aps 2003).pdf

(1656 KB) Pobierz
Understanding the “Self-Acceleration Paradox”
Copyright © 2003 IEEE. Reprinted from The Proceedings of the 2003 IEEE APS/URSI Conference
This material is posted here with permission of the IEEE. Internal or personal use of this material is permitted. However,
permission to reprint/republish this material for advertising or promotional purposes or for creating new collective works for resale or
redistribution must be obtained from the IEEE by writing to pubs-permissions@ieee.org . By choosing to view this document, you
agree to all provisions of the copyright laws protecting it.
http://www.uwbantenna.com
UWB Magnetic Antennas
Hans Gregory Schantz
Q-Track Corporation
315 North Main Street
Tennille, GA 31089
h.schantz@q-track.com
Introduction:
A wide variety of electric ultra-wideband (UWB) antennas have seen commercial
use. A few examples of these include diamond dipoles [1], and elliptical dipoles [2].
These electric antennas tend to have relatively large electric near-fields that are prone to
undesired coupling with near-by objects.
Many commercial applications, however, call for UWB antennas that are less
prone to near-field coupling. Magnetic antennas are well suited for these applications,
because the relatively large magnetic fields tend not to couple as strongly with near-by
objects. The purpose of this article is to provide a brief overview of some UWB
magnetic antennas. In particular, this paper will discuss large current radiators,
monoloop antennas, and magnetic slot antennas.
Large Current Radiators:
A “large current radiator” is ideally a current sheet whose return currents are
isolated by a ground plane (see Figure 1). Harmuth pioneered this basic design [3,4], and
variations of the large current radiator concept have been developed by various
investigators [5].
Ground
Plane
Farr et al proposed an
interesting variation on this basic
architecture [6]. The “balanced-
dipole” antenna (shown in Figure
2) has the interesting property
that it can be fed from either end,
while the opposite end is
terminated with an appropriate
impedance. Thus, the pattern of
this antenna may be dynamically
switched.
Differential Feed
Large
Current
Radiator
Figure 1: Harmuth’s large current radiator
The principal dis-
advantage of large current
radiators is that they tend to be
lossy antennas. A current sheet
will necessarily radiate from
both sides. This energy is
trapped between the large current
radiator and the ground plane
yielding undesirable resonances.
Ground
Plane
Feed
Resistive
Termination
Figure 2: Balanced-dipole antenna of Farr et al
647554413.011.png
 
647554413.012.png
 
647554413.001.png 647554413.002.png 647554413.003.png 647554413.004.png 647554413.005.png
Reprint: 2003 IEEE APS Conference
Accordingly, a ferrite or other absorptive coating is typically used to dissipate these
undesired emissions. Thus, large current radiators are generally not very efficient.
Monoloop Antennas:
The main disadvantage of
large current radiators follows
from the fact that these antennas
trap energy between their
radiating elements and their
ground planes. This suggests
that it might be fruitful to
consider radiating elements
oriented in a plane perpendicular
to the ground plane.
One early antenna with
this architecture was Turner et
al’s scimitar antenna shown in
Figure 4 [7]. This antenna is
characterized by an operating
bandwidth in excess of 1:10.
Although well matched, the
scimitar antenna exhibits some
variation in pattern as a function
of frequency. Ideally, a UWB antenna should have a stable and consistent pattern as a
function of frequency.
Feed
Figure 3: Scimitar antenna of Turner et al.
Ground
Plane
Feed
Figure 4: The author’s monoloop antenna.
The author devised a similar antenna, dubbed a “monoloop” [8]. The “monoloop”
name follows from the fact that antennas with this architecture are essentially half a loop
driven against a ground plane, just as a “monopole” is half a dipole antenna driven
against a ground plane.
The author’s monoloop antenna differs from the scimitar antenna in the feed
region. This antenna has a round, bulbous end that offers an excellent match to 50 ohms.
Like the scimitar antenna, the author’s monoloop antenna suffers from some variation in
pattern as a function of frequency. Also, the monoloop pattern is not uniform in the plane
of the monoloop element. The reason for this behavior may be understood by
considering the current flow in the monoloop element and the resulting radiation.
Assume each infinitesimal current element along the monoloop is the source of
radiation along the radius of curvature at that point. If the monoloop element is
considered in cross-section, this means that each infinitesimal current element generates a
direct ray of radiation radially outward, and a radially inward ray directed toward the
ground plane. This radially inward ray ends up reflected.
The radiation in any given direction is the sum of a direct ray from one part of the
monoloop and a reflected ray from a different part of the monoloop element. A quick
calculation of the path lengths involved demonstrates an asymmetry of the direct and
reflected paths: the relative path lengths varies as a function of angle. This variation is
the root cause of the non-uniform pattern as a “direct” impulse waveform combines with
a “reflected” impulse waveform with a relative delay that varies as a function of look
angle. This behavior is illustrated in Figure 5.
Ground
Plane
647554413.006.png 647554413.007.png
Reprint: 2003 IEEE APS Conference
Figure 5: Current and radiation from a
monoloop element.
One way to rectify this undesired
asymmetry is to feed the monoloop in a
symmetric manner. This was the
fundamental idea behind the author’s
center-fed monoloop (see Figure 6). By
moving the feed to the center top of the
monoloop antenna, symmetry is restored.
The direct and reflected paths are now the
same length as the look angle is varied.
Thus the pattern of a center-fed monoloop
is more uniform as a function of look
angle. Figure 7 shows characteristic
current and radiation rays for the center-
fed monoloop.
Direct Ray
Reflected
Ray
Ground
Plane
Feed
Current
Current
Feed Line
Ground Plane
Figure 6: A center-fed monoloop.
Figure 7: Current and radiation from a center fed monoloop.
Magnetic Slot Antennas:
Magnetic slot antennas are a final UWB magnetic antenna architecture. One
example is Barnes’s UWB magnetic slot antenna shown in Figure 8 [9,10]. If an
appropriate taper is chosen
for the slot line of this
antenna, excellent matching
can be obtained. A
magnetic slot antenna like
the one shown in Figure 8
exhibits a quadrupole type
radiation pattern with a
pattern lobe lying in the
normal direction on either
side of the plane. When
driven against a reflecting
back plane, this antenna
exhibited good perform-
ance in the Time Domain
Corporation’s RV1k
through-wall UWB radar.
Figure 8: Barnes’s UWB magnetic slot antenna.
647554413.008.png 647554413.009.png 647554413.010.png
Reprint: 2003 IEEE APS Conference
Conclusion:
In conclusion, there are a wide variety of magnetic type UWB antennas available
for commercial applications. This paper has surveyed three general kinds of magnetic
UWB antennas: large current radiators, monoloops, and slot antennas. Although far from
being exhaustive, this paper provided examples of each type to illustrate the variety of
antennas possible within each of these magnetic UWB antenna architectures.
Acknowledgement:
The author’s monoloop and center-fed monoloop antennas described in reference
8 were originally invented while the author was employed as an antenna engineer by the
Time Domain Corporation.
References:
[1] H. Schantz & L. Fullerton, “The Diamond Dipole: A Gaussian Impulse Antenna,”
IEEE APS2001 (July 2001).
[2] H. Schantz, “Planar Elliptical Element UWB Dipole Antennas,” IEEE APS 2002
(June 2002).
[3] H. Harmuth & S. Ding-rong, “Large-Current, Short-Length Radiator for
Nonsinusoidal Waves,” IEEE International Symposium on Electromagnetic
Compatibility, 1983 pp. 453-456.
[4] H. Harmuth, “Frequency Independent Shielded Loop Antenna,” U.S. Patent
4,506,267.
[5] G. Pochanin, “Large Current Radiator for the Short Electromagnetic Pulses
Radiation,” Ultra-Wideband, Short-Pulse Electromagnetics 4, New York: Kluwer
Academic/Plenum Publishers, 1999), pp. 149-155.
[6] E. Farr, C. Baum, W. Prather, and T. Tran “A Two-Channel Balanced-Dipole
Antenna With Reversible Antenna Pattern Operating at 50 Ohms,” Sensor and
Simulation Note #441 (December 1999).
[7] E. Turner, W. Turner, “Scimitar Antenna,” U.S. Patent 3,015,101.
[8] H. Schantz, “Single Element Antenna Apparatus,” U.S. Patent 6,437,756.
[9] M. Barnes, “Ultra-Wideband Magnetic Antenna,” U.S. Patent 6,091,374.
[10] H. Schantz, M. Barnes, “The COTAB UWB Magnetic Slot Antenna,” IEEE APS
2001 (July 2001).
Zgłoś jeśli naruszono regulamin