Frequency independent shielded loop antenna

• US 4,506,267 A
• Filed: 01/26/1983
• Issued: 03/19/1985
• Est. Priority Date: 01/26/1983
• Status: Expired due to Term

• Current Assignee: Geophysical Survey Systems, Inc.
• Original Assignee: Geophysical Survey Systems, Inc.
• Inventors: Harmuth, Henning F.
• Primary Examiner(s): Lieberman, Eli
• Application Number:
  US06/461,153
• Time in Patent Office: 783 Days
• Field of Search: 343/708, 343/741, 343/748, 343/743, 343/744, 343/794, 343/807, 343/841, 343/842, 343/845, 343/846
• US Class Current: 343/744
• CPC Class Codes: H01Q 17/001 for modifying the directional characteristic of an aerial
• CPC Class Codes: H01Q 7/00 Loop antennas with a substantially uniform current distribution around the loop and having a directional radiation pattern in a plane perpendicular to the plane of the loop
• CPC Class Codes: H01Q 9/28 Conical, cylindrical, cage, strip, gauze, or like elements having an extended radiating surface; Elements comprising two conical surfaces having collinear axes and adjacent apices and fed by two-conductor transmission lines waveguide horns or mouths H01Q13/00; slot antennas H01Q13/00

Abstract

An antenna is disclosed that is especially useful for radiating and receiving non-sinusoidal electromagnetic waves. The antenna is an efficient and distortion-free radiator of electromagnetic pulses that do not use a sinusoidal carrier. The antenna'"'"'s size is independent of frequency and the antenna, therefore, can be of small size relative to the wavelength of the radiated electromagnetic waves. When used for reception of electromagnetic wave energy, the antenna performs with low distortion. The basic concept underlying the invention is the modification of the Hertzian electric dipole into an antenna structure that can carry large currents without requiring a large driving voltage. Antennas for the transmission or reception of sinusoidal waves achieve that goal by employing resonant structures. The invention achieves the same result by changing the Hertzian electric dipole into a loop that forms a Hertzian magnetic dipole and preventing the undesirable magnetic dipole radiation by shields of conducting and absorbing materials.

Claims

1. An antenna for producing electric dipole radiation, comprising

(a) electrically conductive means forming a loop, one portion of the loop being a radiator leg for radiating electromagnetic wave energy,

(b) a current source for driving a current around the conducting loop,

(c) shield means for confining radiation from the current source and that portion of the loop opposite the radiator leg, the shield means being disposed around the current source and that portion of the loop opposite the radiator, and

(d) adsorbing material on the shield means, the absorbing material absorbing energy from surface currents induced in the shield means by radiation from the radiator leg.

2. An antenna for producing electrical dipole radiation, comprising

(a) electrically conductive means forming a loop, one portion of the loop being a radiator leg for radiating electromagnetic wave energy,

(b) a current source for driving a current around the conducting loop, and

(c) shield means for confining radiation from the current source and that portion of the loop opposite the radiator leg, the shield means being disposed around the current source and that portion of the loop opposite the radiator leg, and the shield means being made of lossy material that attenuates surface currents induced in the shield means by radiation from the radiator leg.

3. A receiving antenna comprising

(a) electrically conductive means forming a loop, one leg of the loop being an elongate conductor for sensing electromagnetic wave energy and providing a current derived therefrom, the leg opposite the sensing leg having in it a lumped impedance,

(b) shield means shielding that opposite leg from electromagnetic wave energy to which the sensing leg is exposed, the shield means absorbing energy from surface currents induced in the shield means by the derived current flowing in the sensing leg, and

(c) means for detecting a signal developed across the lumped impedance by the current flow in the loop.