TY - JOUR
T1 - Effect of defocus on the prompt response of a reflector IRA
AU - Tyo, J. Scott
AU - Farr, Everett G.
AU - Lawry, Dean I.
N1 - Funding Information:
Manuscript received June 1, 2004; revised February 28, 2005. This work was supported by the Directed Energy Directorate, Air Force Research Laboratory through a Small Business Innovative research Contract. J. S. Tyo is with the Electrical Engineering and Computer Engineering Department, University of New Mexico, Albuquerque, NM 87131 USA (e-mail: [email protected]). E. G. Farr is with Farr Research, Inc., Albuquerque, NM 87123 USA (e-mail: [email protected]). D. I. Lawry is with the Directed Energy Directorate, Air Force Research Laboratory, Kirtland AFB, NM 87117 USA (e-mail: [email protected]). Digital Object Identifier 10.1109/TAP.2005.856322 Fig. 1. Schematic of a generic four-arm IRA. The aperture plane is shown here. Various sizes and shapes of apertures can be considered in the physical optics theory.
PY - 2005/10
Y1 - 2005/10
N2 - Impulse radiating antennas (IRAs) are an emerging class of antenna that are designed to radiate extremely short electromagnetic pulses with multiple decades of instantaneous bandwidth. The most common IRAs are made with a transverse electromagnetic (TEM) transmission line feeding a paraboloidal reflector. The IRA is usually constructed so that the electrical feed point of the TEM transmission line coincides with the focal point of the paraboloid. The paraboloidal reflector converts the spherical wave emanating from the feed point into a plane wave (i.e., a spherical wave centered at -∞). In many practical cases, the feed point and focal points are not exactly aligned, producing some defocus of the reflector. In this paper, we model the case of hyperbolic defocus because of its analytic form and compare this model with experimental measurements. A hyperboloidal reflector fed from one focus converts the expanding spherical wave into a second expanding wave which appears to emanate from the second focal point of the hyperboloid (which is behind the reflector). Hyperboloidal defocus is roughly equivalent to moving the electrical feed closer to the reflector than the optical focal point. Previous theoretical results from in-focus IRAs predicted that the E- and H-plane temporal responses should be symmetric with respect to the temporal center of the response. The results shown here demonstrate that the defocusing causes these responses to become asymmetric. The new results are in better agreement with experimental measurements of IRAs and provide a physical explanation for experimental results that differ from the original theory.
AB - Impulse radiating antennas (IRAs) are an emerging class of antenna that are designed to radiate extremely short electromagnetic pulses with multiple decades of instantaneous bandwidth. The most common IRAs are made with a transverse electromagnetic (TEM) transmission line feeding a paraboloidal reflector. The IRA is usually constructed so that the electrical feed point of the TEM transmission line coincides with the focal point of the paraboloid. The paraboloidal reflector converts the spherical wave emanating from the feed point into a plane wave (i.e., a spherical wave centered at -∞). In many practical cases, the feed point and focal points are not exactly aligned, producing some defocus of the reflector. In this paper, we model the case of hyperbolic defocus because of its analytic form and compare this model with experimental measurements. A hyperboloidal reflector fed from one focus converts the expanding spherical wave into a second expanding wave which appears to emanate from the second focal point of the hyperboloid (which is behind the reflector). Hyperboloidal defocus is roughly equivalent to moving the electrical feed closer to the reflector than the optical focal point. Previous theoretical results from in-focus IRAs predicted that the E- and H-plane temporal responses should be symmetric with respect to the temporal center of the response. The results shown here demonstrate that the defocusing causes these responses to become asymmetric. The new results are in better agreement with experimental measurements of IRAs and provide a physical explanation for experimental results that differ from the original theory.
KW - Impulse radiating antennas (IRAs)
KW - Physical optics
KW - Time-domain electromagnetics
KW - UWB electromagnetics
KW - Ultrawide-band (UWB) antennas
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U2 - 10.1109/TAP.2005.856322
DO - 10.1109/TAP.2005.856322
M3 - Article
AN - SCOPUS:27644572981
SN - 0018-926X
VL - 53
SP - 3247
EP - 3254
JO - IEEE Transactions on Antennas and Propagation
JF - IEEE Transactions on Antennas and Propagation
IS - 10
ER -