The present invention relates to antennas and in particular to wide band antennas.
Modern communication system use multi-frequency devices. These multi-frequency devices need to use several antennas or wide band antennas. The known wide band antennas however have significant sizes. They are usually composed of a plurality of several narrow band radiators.
One of such knows antennas are a log periodic antenna shown in
Accordingly, it is an object of the present invention to provide a wide band antenna which avoids the disadvantages of the known wide band antennas.
In keeping with these objects and with others which will become apparent hereinafter, one features of the present invention resides, briefly stated, in a wide band antenna which has two radiators, including a first radiator formed as an electric field monopole radiator or a helix radiator, and a second radiator formed as an electric field folded dipole radiator or a magnetic field loop radiator.
When the broad band antenna is designed in accordance with the present invention is constitutes an improvement over the known wide band antennas because it has a significantly smaller size.
According to another feature of the present invention, in the wide band antenna the first radiator has a length of substantially one quarter of a wave of the lowest frequency (F), while the second radiator is a folded dipole radiator adjusted to a second harmonic of the lowest frequency (2F) and has a perimeter of substantially half wave length at the lowest frequency.
According to a further feature of the present invention, in the wide band antenna the first and second radiators are configured so that on odd frequencies F, 3F, 5F, etc. the first radiator radiates satisfactory and the second radiator operates as an inverter formed as a delay line substantially half wave length, while on even frequencies 2F, 4F, 6F, etc. the second radiator radiates satisfactory while the first radiator does not radiate. On even harmonics the first radiator operates, but not very efficiently.
According to a further feature of the present invention, in the wide band antenna the second radiator is formed as a loop radiator radiating a magnetic field signal with a wave length substantially equal to a perimeter of a loop radiator, and on even frequencies 2F, 4F, 6F, etc. the second radiator radiates while the first radiator does not radiate.
According to a further feature of the present invention, in the wide band antenna the radiators can be supplied with signals from a single source or from a plurality of sources.
The novel features of the present invention are set forth in particular in the appended claims.
The invention itself however both as to its construction and its manner of operation will be best understood from the following description of the preferred embodiment which is accompanied by the following drawings.
A wide band antenna according to the present invention can be used in communications system, including such communication system and devices as transducers, cellular telephones, feeds for satellite antennas, etc.
Abbreviations used in the description include WBMB which stands for a wide band Michael Bank antenna, and MB which stands for Michael Bank.
In the embodiment shown in
In the embodiment shown in
In accordance with still a further embodiment of wide band antenna of the present invention shown in
In the wide band antenna according to the present invention the first radiator is a monopole which can be in form of a wire, a rod, or a wide plate. This is a monopole radiator with a length of substantially one quarter of a wave of the lowest frequency (F), while the second radiator is adjusted to a second harmonic of the lowest frequency (2F) and has a perimeter of substantially half wave length at the lowest frequency.
The first and second radiators are configured so that on odd frequencies F, 3F, 5F, etc. only the first radiator radiates and the second radiator operates as an inverter formed as a delay line substantially over half wave length, while on even frequencies 2F, 4F, 6F, etc. the second radiator radiates while the first radiator does not radiate.
The second radiator formed as a folded dipole can radiate an electric field signal at a frequency which corresponds to a wave length equal to substantially a length of a folded dipole perimeter and at its harmonics, while the second radiator formed as a loop radiator can radiate a magnetic field signal at a frequency which corresponds to a wave length equal to substantially a length of a perimeter of the loop radiator and at its harmonics.
The present invention is not limited to the details shown since various modifications and structural changes are possible without departing from the spirit of the present invention.
What is desired to be protected by Letters Patent is set forth in particular in the appended claims.
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