## Abstract This paper presents numerical analyses of a plasma‐column antenna using the finite‐difference time‐domain (FDTD) technique. We have simulated simple plasma‐antenna configurations (monopoles) to demonstrate some of their properties. We have evaluated the field distribution around the pla
FDTD analysis of a plasma whip antenna
✍ Scribed by Z. H. Qian; R. S. Chen; H. W. Yang; K. W. Leung; Edward K. N. Yung
- Publisher
- John Wiley and Sons
- Year
- 2005
- Tongue
- English
- Weight
- 132 KB
- Volume
- 47
- Category
- Article
- ISSN
- 0895-2477
No coin nor oath required. For personal study only.
✦ Synopsis
order of increasing losses. Figure 1 shows that it is possible that the correlation decreases with increasing losses, but it also shows the general tendency of pattern correlation to increase. If the antenna pair is physically symmetric and the added losses are asymmetric (that is, the dissipating material is not very close to the array), then Figures 1 and 2 are realistic. However, if the pair and the added losses are symmetric, then only the phase differences of 0°or 180°a re possible, with the lowest or highest level of pattern correlation and with maximum or minimum difference between the reflectedpower eigenvalues.
4. CONCLUSION
An exact matrix expression has been presented for the dependency of the pattern correlation for the reflected-power and dissipatedpower rates. In the lossless case, the scattering matrix defines the pattern-correlation matrix exactly. However, in the more realistic case of lossy arrays, that is, for handheld devices, the losses need to be taken into account. Since the losses cannot be determined exactly in the general case, the pattern correlation can only be estimated.
REFERENCES
📜 SIMILAR VOLUMES
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