Dual-band blade antenna

Introduction

This article is under construction.

Monopole Antenna

A typical monopole antenna, pictured to the left, has an omni-directional pattern and is limited in its frequency range. Please keep in mind that an omni-directional (see omnidirectional antenna) radiation pattern applies to the azimuth patterns and does exhibit a null at zenith.

A monopole antenna can be thought of a dipole antenna where one end of the dipole antenna now becomes the ground plane for said monopole antenna. By this line of conceptual thinking, one can easily reach the conclusion that the radiation emanating from a monopole antenna exists in the half the space of similar dipole antenna. Therefore, the maximum gain is twice that or an addition 3dB of the maximum gain of typical dipole. Hence the nominal value of maximum for a monopole antenna is about 5.15dBi.

Stutzman, who has a way with words much better than this author, puts it as follows:

... A monopole is a dipole that has been divided in half at its center feed point and fed against a ground plane...

This article cover one type of dual band blade monopoles. This is the slot inside a monopole. Computational Electromagnetic Modeling (CEM) will be used to give some graphics of operations for a more conceptual understanding.

Theory

Monopoles

Monopole equations can be arrived by inspection of dipole antenna derivations with the knowledge that all radiation occurs in half the volume when compared to said dipole antenna. This leads to the following equations:

Directivity

$D_{mono}={\frac {4\pi }{\Omega _{A,mono}}}=2D_{dipole}$

The leads directly to the ealier stated maximum gain relation to a dipole buy the definition of gain a $G=\epsilon D$ where $\epsilon$ is the antenna radiation efficiency.

Impedance

$Z_{A,mono}={\frac {1}{2}}Z_{A,Dipole}$

Radiation Resistance

$R_{r,mono}={\frac {1}{2}}R_{r,mono}$

As can be seen in section 1 of the linked radiation resistance article.

Slot Antennas

A slot antenna can be viewed as a dipole with opposite polarization. This is due to the typical feed which sets the orientation of the E-field across the smallest linear dimension of the slot. The following equations can be used to 'translate' a vertical or horizontal slot antenna into its complement (dipole):

$E_{\theta s}=H_{\theta c}\quad E_{\phi s}=H_{\phi c}$

This is defined by Babinet's principle and Booker's Extension further expands this principle to include polarization. The simple equations from Babinet's principle are stated on the linked page for which the author has had input.

Computational Electromagnetic Modeling (CEM)

Insert modeling here etc.

References

--Wallace (talk) 22:13, 16 March 2008 (UTC)