000 | 05375nam a2200649 i 4500 | ||
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001 | 6813178 | ||
003 | IEEE | ||
005 | 20200413152852.0 | ||
006 | m eo d | ||
007 | cr cn |||m|||a | ||
008 | 081203s2008 caua foab 000 0 eng d | ||
020 | _a9781598298147 (electronic bk.) | ||
020 | _a9781598298130 (pbk.) | ||
024 | 7 |
_a10.2200/S00156ED1V01Y200810ANT009 _2doi |
|
035 | _a(OCoLC)271225318 | ||
035 | _a(CaBNVSL)gtp00532197 | ||
040 |
_aCaBNVSL _cCaBNVSL _dCaBNVSL |
||
050 | 4 |
_aTK7871.6 _bW844 2008 |
|
082 | 0 | 4 |
_a621.3824 _222 |
100 | 1 | _aWu, Xuan Hui. | |
245 | 1 | 0 |
_aGeneralized transmission line method to study the far-zone radiation of antennas under a multilayer structure _h[electronic resource] / _cXuan Hui Wu, Ahmed A. Kishk, and Allen W. Glisson. |
260 |
_aSan Rafael, Calif. (1537 Fourth Street, San Rafael, CA 94901 USA) : _bMorgan & Claypool Publishers, _cc2008. |
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300 |
_a1 electronic text (ix, 86 p. : ill.) : _bdigital file. |
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490 | 1 |
_aSynthesis lectures on antennas, _x1932-6084 ; _v# 9 |
|
538 | _aMode of access: World Wide Web. | ||
538 | _aSystem requirements: Adobe Acrobat reader. | ||
500 | _aPart of: Synthesis digital library of engineering and computer science. | ||
500 | _aSeries from website. | ||
504 | _aIncludes bibliographical references (p. 83-84). | ||
505 | 0 | _aIntroduction -- Antennas under a multilayer dielectric slab -- Introduction -- Radiation due to an electric dipole -- Evaluation of the horizontal component using chainmatrix -- Evaluation of the vertical component -- Field projection -- Evaluation of the horizontal component using S chain matrix -- Radiation due to a magnetic dipole -- Evaluation of the horizontal component using chainmatrix -- Evaluation of the vertical component -- Field projection -- Evaluation of the horizontal component using S chain matrix -- Results verification -- Applications -- Thin wire monopole antenna in a two-layer structure -- DRA in a four-layer structure -- Conclusions -- Antennas under a polarized multilayer structure -- Introduction -- Radiation due to an electric dipole -- Radiation due to a magnetic dipole -- Asymptotic boundary conditions -- PEC-type asymptotic boundary conditions -- PMC-type asymptotic boundary conditions -- Applications -- Cross polarization reduction -- Polarizer -- Discussion -- Conclusions -- Hertzian dipole model for an antenna -- Introduction -- Narrowband Hertzian dipole model -- Particle swarm optimization method -- PSO model for getting a narrowband dipole model -- Limitations of the narrowband model -- Wideband Hertzian dipole model -- PSO model for getting a wideband dipole model -- Modeling of a wideband antenna -- Application -- Rejection of Gaussian noise -- Frequency scalability -- Conclusions -- A derivation of equations in chapter 2 -- Derivation of equation (2.24) -- Derivation of equation (2.29) -- Derivation of equation (2.30) -- Maxima source code -- Maxima source code for a PEC-SI -- Maxima source code for a PMC-SI. | |
506 | 1 | _aAbstract freely available; full-text restricted to subscribers or individual document purchasers. | |
510 | 0 | _aCompendex | |
510 | 0 | _aINSPEC | |
510 | 0 | _aGoogle scholar | |
510 | 0 | _aGoogle book search | |
520 | _aThis book gives a step-by-step presentation of a generalized transmission line method to study the far-zone radiation of antennas under a multilayer structure. Normally, a radiation problem requires a fullwave analysis which may be time consuming. The beauty of the generalized transmission line method is that it transforms the radiation problem for a specific type of structure, say the multilayer structure excited by an antenna, into a circuit problem that can be efficiently analyzed. Using the Reciprocity Theorem and far-field approximation, the method computes the far-zone radiation due to a Hertzian dipole within a multilayer structure by solving an equivalent transmission line circuit. Since an antenna can be modeled as a set of Hertzian dipoles, the method could be used to predict the far-zone radiation of an antenna under a multilayer structure. The analytical expression for the far-zone field is derived for a structure with or without a polarizer. The procedure of obtaining the Hertzian dipole model that is required by the generalized transmission line method is also described. Several examples are given to demonstrate the capabilities, accuracy, and efficiency of this method. | ||
530 | _aAlso available in print. | ||
588 | _aTitle from PDF t.p. (viewed on December 3, 2008). | ||
650 | 0 |
_aAntennas (Electronics) _xMathematical models. |
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650 | 0 | _aAntenna radiation patterns. | |
690 | _aTransmission line. | ||
690 | _aAntenna | ||
690 | _aHigh directivity. | ||
690 | _aMultilayer structure. | ||
690 | _aOptimization. | ||
690 | _aEBG. | ||
690 | _aHertzian dipole. | ||
690 | _aReciprocity. | ||
690 | _aAsymptotic boundary conditions. | ||
690 | _aFar-field radiation. | ||
690 | _aPolarizer. | ||
700 | 1 | _aKishk, Ahmed A. | |
700 | 1 |
_aGlisson, Allen W. _q(Allen Wilburn), _d1951- |
|
730 | 0 | _aSynthesis digital library of engineering and computer science. | |
830 | 0 |
_aSynthesis lectures on antennas ; _v# 9. |
|
856 | 4 | 2 |
_3Abstract with links to resource _uhttp://ieeexplore.ieee.org/servlet/opac?bknumber=6813178 |
999 |
_c561642 _d561642 |