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href=\"https://books.google.com.sg/url?id=CoihHs1Ctp4C\u0026pg=PA149\u0026q=http://www.springer.com/shop\u0026clientid=ca-print-springer-kluwer_academic\u0026linkid=1\u0026usg=AOvVaw0ChdAamR-CfhNpEpnEAehg\u0026source=gbs_pub_info_r\"\u003eSpringer Science \u0026amp; Business Media\u003c/a\u003e","is_ebook":false,"volumeresult":{"has_flowing_text":false,"has_scanned_text":true,"can_download_pdf":false,"can_download_epub":false,"is_pdf_drm_enabled":false,"is_epub_drm_enabled":false},"publisher":"Springer Science \u0026 Business Media","publication_date":"2003.07.31","subject":"Computers","num_pages":191,"sample_url":"https://play.google.com/books/reader?id=CoihHs1Ctp4C\u0026source=gbs_vpt_hover","synposis":"Millimeter-Wave Waveguides is a monograph devoted to open waveguides for millimeter wave applications. In the first chapters, general waveguide theory is presented (with the emphasis on millimeter wave applications). Next, the book systematically describes the results of both theoretical and experimental studies of rectangular dielectric rod waveguides with high dielectric permittivities. Simple and accurate methods for propagation constant calculations for isotropic as well as anisotropic dielectric waveguides are described. Both analytical and numerical approaches are covered. Different types of transitions have been simulated in order to find optimal configurations as well as optimal dimensions of dielectric waveguides for the frequency band of 75-110 GHz. Simple and effective design is presented. The experimental studies of dielectric waveguides show that Sapphire waveguide can be utilized for this frequency band as a very low-loss waveguide. Design of antennas with low return loss based on dielectric waveguides is also described.","my_library_url":"https://www.google.com/accounts/Login?service=print\u0026continue=https://books.google.com.sg/books%3Fop%3Dlibrary\u0026hl=en","is_magazine":false,"is_public_domain":false,"last_page":{"pid":"PA190","order":190,"title":"190"}},{"enableUserFeedbackUI":true,"pseudocontinuous":true,"is_cobrand":false,"sign_in_url":"https://www.google.com/accounts/Login?service=print\u0026continue=https://books.google.com.sg/books%3Fid%3DCoihHs1Ctp4C%26q%3D%2522dielectric%2Bwaveguide%26pg%3DPA149%26redir_esc%3Dy%26hl%3Den\u0026hl=en","isEntityPageViewport":false,"showViewportOnboarding":false,"showViewportPlainTextOnboarding":false},{"page":[{"pid":"PA149","highlights":[{"X":62,"Y":234,"W":127,"H":26},{"X":198,"Y":234,"W":139,"H":26},{"X":61,"Y":351,"W":60,"H":14},{"X":373,"Y":387,"W":57,"H":13},{"X":62,"Y":441,"W":57,"H":13},{"X":219,"Y":476,"W":57,"H":15},{"X":227,"Y":568,"W":57,"H":13},{"X":387,"Y":586,"W":57,"H":13},{"X":448,"Y":586,"W":65,"H":13},{"X":182,"Y":622,"W":65,"H":13},{"X":259,"Y":622,"W":57,"H":13},{"X":323,"Y":622,"W":65,"H":13},{"X":296,"Y":640,"W":65,"H":14},{"X":372,"Y":640,"W":57,"H":14},{"X":150,"Y":658,"W":57,"H":12},{"X":102,"Y":715,"W":111,"H":12},{"X":317,"Y":772,"W":58,"H":14}],"flags":8,"order":150,"vq":"\u0026quot;dielectric waveguide"}]},null,{"number_of_results":57,"search_results":[{"page_id":"PP6","snippet_text":"... waveguide walls. Hybrid modes 1.2.4 TEM mode 1.3 Orthogonality of the modal fields 1.3.1 The proof 1.4 Fundamental properties of open waveguides Boundary conditions for open waveguides Eigenwaves in planar \u003cb\u003edielectric waveguides\u003c/b\u003e 1.4.1\u0026nbsp;...","page_url":"https://books.google.com.sg/books?id=CoihHs1Ctp4C\u0026pg=PP6\u0026vq=%22dielectric+waveguide"},{"page_id":"PP7","snippet_text":"... dielectric rod waveguide in air Some properties of rectangular \u003cb\u003edielectric waveguides\u003c/b\u003e How well does Marcatili\u0026#39;s method work? 5.2 Goell\u0026#39;s method 5.3 Open anisotropic waveguides 5.3.1 5.4 84 8587 87 5.3.2 Modification of Marcatili\u0026#39;s method\u0026nbsp;...","page_url":"https://books.google.com.sg/books?id=CoihHs1Ctp4C\u0026pg=PP7\u0026vq=%22dielectric+waveguide"},{"page_id":"PA1","page_number":"1","snippet_text":"... waveguides 8 \u003cb\u003eDielectric waveguide\u003c/b\u003e devices and integrated circuits \u003cb\u003eDielectric waveguides\u003c/b\u003e for integrated circuits 8.1.1 Non-radiative \u003cb\u003edielectric waveguide\u003c/b\u003e 144 146 146 149 149 150 8.1.2 \u003cb\u003eDielectric waveguide\u003c/b\u003e circuits on metal and dielec\u0026nbsp;...","page_url":"https://books.google.com.sg/books?id=CoihHs1Ctp4C\u0026pg=PA1\u0026vq=%22dielectric+waveguide"},{"page_id":"PA3","page_number":"3","snippet_text":"... waveguides and some devices built around millimeter-wave waveguide sections. Due to several reasons, in this frequency range different materials are used to fabricate \u003cb\u003edielectric waveguides\u003c/b\u003e (as compared to fiber optics, for ex- ample)\u0026nbsp;..."},{"page_id":"PA4","page_number":"4","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e are the so-called Marcatili\u0026#39;s (and its variations) and Goell\u0026#39;s methods. In Chapter 5, the classical Marcatili\u0026#39;s and Goell\u0026#39;s methods are described, and then adapted for the anisotropic dielectric case. For instance\u0026nbsp;..."},{"page_id":"PA20","page_number":"20","snippet_text":"... dependence on one of the transverse coordinates then equations (1.62) and (1.63) simplify to For shortness, let us write only equations for TM modes,. 20 MILLIMETER-WAVE WAVEGUIDES Eigenwaves in planar \u003cb\u003edielectric waveguides\u003c/b\u003e 1 2."},{"page_id":"PA57","page_number":"57","snippet_text":"... \u003cb\u003ewaveguide\u003c/b\u003e with an anisotropic filling‚ let us consider again the \u003cb\u003edielectric\u003c/b\u003e plate \u003cb\u003ewaveguide\u003c/b\u003e‚ as shown in Fig- ure 3.3. This will also demonstrate a different approach to the deriva- tion of the dispersion relation for open \u003cb\u003ewaveguides\u003c/b\u003e\u0026nbsp;..."},{"page_id":"PA61","page_number":"61","snippet_text":"... \u003cb\u003ewaveguide\u003c/b\u003e axes TM and TE modes might not exist [ 4 ] , and the calculations become more complicated . In Chapter 5 another approach is described , that is based on the exact averaging method . Furthermore , \u003cb\u003edielectric\u003c/b\u003e rod \u003cb\u003ewaveguides\u003c/b\u003e are\u0026nbsp;..."},{"page_id":"PA74","page_number":"74","snippet_text":"... the wavelength. strip‚ much. 4.3.1 Microsrip line on ferrite substrate . Isolator Figure 5.4 . Dimensions of the \u003cb\u003edielectric waveguide\u003c/b\u003e cross section. 74 MILLIMETER - WAVE WAVEGUIDES Microsrip line on ferrite substrate Isolator."},{"page_id":"PA75","page_number":"75","snippet_text":"... \u003cb\u003edielectric\u003c/b\u003e substrates. Because the height is small‚ we This system splits into three scalar equations for Cartesian components. Looking for fundamental solutions in form we have Eliminating with the use of the last equation‚ we get\u0026nbsp;..."},{"page_id":"PA79","page_number":"79","snippet_text":"... \u003cb\u003eDielectric waveguides\u003c/b\u003e : classical methods for propagation constant calculations \u003cb\u003eDielectric waveguides\u003c/b\u003e are more attractive at millimeter - wave frequencies , as compared with metal waveguides , because of their lower propagation loss\u0026nbsp;..."},{"page_id":"PA80","page_number":"80","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e is the Marcatili method [3]. It was developed for low ratios between the core permittivity and that of the cladding region (slightly more than 1)‚ but it has been shown that it works well even for high permittivity\u0026nbsp;..."},{"page_id":"PA81","page_number":"81","snippet_text":"... waveguide and decaying exponentially outside. That is‚ we express the field components‚ say‚ as follows: where are unknown amplitude ... dielectric rod waveguide in air component‚ at find. \u003cb\u003eDielectric waveguides\u003c/b\u003e: calculations 81."},{"page_id":"PA82","page_number":"82","snippet_text":"... dielectric rod waveguide in air component‚ at find the eigensolutions we should match the components To analyze the open ... waveguide in Some properties of rectangular \u003cb\u003edielectric waveguides\u003c/b\u003e How well does Marcatili\u0026#39;s method work?"},{"page_id":"PA83","page_number":"83","snippet_text":"... waveguide‚ we have to solve equations (5.12) and (5.16) and then find vertical and one horizontal‚ with the thicknesses and respectively. Another approach can be found in [4]‚ where all the ... \u003cb\u003eDielectric waveguides\u003c/b\u003e: calculations 83."},{"page_id":"PA84","page_number":"84","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e is only slightly larger than unity . Let us check what happens if we try to calculate the fundamental E , mode for , say , a Silicon \u003cb\u003edielectric waveguide\u003c/b\u003e ( n = 3.41 ) with the cross section dimensions Frequency\u0026nbsp;..."},{"page_id":"PA85","page_number":"85","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e with 0.5 × 1.0 mm2 cross section , El mode . One can see from Figure 5.3 that in spite of its simplicity Marcatili\u0026#39;s method works quite well for \u003cb\u003edielectric waveguides\u003c/b\u003e made of even high permittivity materials like\u0026nbsp;..."},{"page_id":"PA86","page_number":"86","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e and and distance are shown in Figure 5.4. outside the core. Here and are the trans- verse propagation constants inside and outside of the dielectric rod‚ tions of the second kind‚ respectively. Variables and are\u0026nbsp;..."},{"page_id":"PA87","page_number":"87","snippet_text":"... \u003cb\u003edielectric waveguides\u003c/b\u003e The uniaxial anisotropic dielectric rod waveguide is nowadays of increas- ing interest , because many high - quality dielectric materials available for fabrication of millimeter - wave waveguides are uniaxial\u0026nbsp;..."},{"page_id":"PA88","page_number":"88","snippet_text":"... dielectric rod waveguide , in which case we can avoid excitation of the orthogonal mode and / or rotation of the polarization plane . The E fundamental mode of the rectangular \u003cb\u003edielectric waveguides\u003c/b\u003e with cross section axb is selected\u0026nbsp;..."},{"page_id":"PA92","page_number":"92","snippet_text":"... \u003cb\u003edielectric waveguides\u003c/b\u003e made of a uniaxial anisotropic dielectric material with the optical axis coinciding with the axis of the dielectric rod waveguide. In more general cases (arbitrary direction of the optical axis‚ anisotropic\u0026nbsp;..."},{"page_id":"PA93","page_number":"93","snippet_text":"... waveguide‚ one can obtain an equation similar to. The tangential components of the electric field are COMPARISON OF MODIFIED MARCATILI\u0026#39;S AND GOELL\u0026#39;S METHODS WITH EXPERIMENTAL RESULTS. \u003cb\u003eDielectric waveguides\u003c/b\u003e: calculations 93."},{"page_id":"PA99","page_number":"99","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e with the cross section dimensions of 1.0 × 0.5 mm2 . Also , calculated data for the orthogonal a - polarization are shown . When the frequency drops , the longitudinal component of the. at other frequencies ( Figures\u0026nbsp;..."},{"page_id":"PA100","page_number":"100","snippet_text":"... \u003cb\u003edielectric waveguides\u003c/b\u003e with uniaxial cores ( the axis is parallel to the waveguide axis ) are provided on disk . References [ 1 ] A.Sv. Sudbø , Why are accurate computations of mode fields on rect- angular \u003cb\u003edielectric waveguides\u003c/b\u003e difficult\u0026nbsp;..."},{"page_id":"PA101","page_number":"101","snippet_text":"... \u003cb\u003eDielectric waveguide\u003c/b\u003e - type millimeter - wave integrated cir- cuits , in Infrared and Millimeter Waves , vol . 4 , chapter 5 , New York : Academic Press , 1981 , pp . 199-273 . [ 12 ] S.N. Dudorov , D.V. Lioubtchenko , J.A. Mallat , and\u0026nbsp;..."},{"page_id":"PA115","page_number":"115","snippet_text":"... Figure 7.1 . A transition from a metal to a \u003cb\u003edielectric waveguide\u003c/b\u003e with the same cross sections . In the case of a \u003cb\u003edielectric waveguide\u003c/b\u003e made of, for. 115 Excitation of millimeter-wave \u003cb\u003edielectric waveguides\u003c/b\u003e: com- puter simulations and\u0026nbsp;..."},{"page_id":"PA116","page_number":"116","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e made of, for example, a semi- conductor or a dielectric with a high permittivity, the cross section di- mensions of the dielectric rod required for the fundamental-only mode operation become smaller. Therefore\u0026nbsp;..."},{"page_id":"PA117","page_number":"117","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e Three types of transitions (taper sections) from the standard metal wa- veguide to open dielectric rod waveguides with relatively high dielectric permittivities seem to be the most suitable (Figure 7.4). The “dove\u0026nbsp;..."},{"page_id":"PA118","page_number":"118","snippet_text":"... waveguide so that waves of different polarizations have dif- ferent propagation constants. Therefore, the ... \u003cb\u003edielectric waveguide\u003c/b\u003e, we can have multimode propagation, which is not desirable. It is well known that, in order to\u0026nbsp;..."},{"page_id":"PA122","page_number":"122","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e is made of a fragile material. Different cross-sections of the \u003cb\u003edielectric waveguide\u003c/b\u003e this results in undesirable dips in the characteristic, possibly due to excitation of higher-order modes. Moreover, the central\u0026nbsp;..."},{"page_id":"PA126","page_number":"126","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e is parallel to the axis of the metal waveguide, and 2) when this axis makes an angle of about 4.5° (the angle of the taper is about 9°) (Figure 7.11). It appears that in the second case the transmission coefficient\u0026nbsp;..."},{"page_id":"PA130","page_number":"130","snippet_text":"... dielectric wedge , for example , of the Sapphire \u003cb\u003edielectric waveguide\u003c/b\u003e . In Figure 7.15 de- pendencies of the insertion losses and reflections on the ; frequency are shown separately for a symmetrically tapered Sapphire waveguide with\u0026nbsp;..."},{"page_id":"PA132","page_number":"132","snippet_text":"... waveguide \u0026quot; external \u0026quot; wave magnetic wall \u0026quot; internal \u0026quot; wave \u003cb\u003edielectric waveguide\u003c/b\u003e Figure 7.16 . Electric field strength in a Sapphire wedge at a particular time instance . The signal frequency is 75 GHz . The horizontal ( H ) plane\u0026nbsp;..."},{"page_id":"PA136","page_number":"136","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e Metal waveguide Styrofoam b ) Asymmetrical Holder E y Figure 7.22 . Experimental setup for measuring the characteristics of transi- tions from a metal waveguide to \u003cb\u003edielectric waveguides\u003c/b\u003e : a ) symmetrical case , b\u0026nbsp;..."},{"page_id":"PA137","page_number":"137","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e section. Removing the receiving metal waveguide results in an increase of the reflection coefficient approximately by 10 dB (Figure 7.25). This means that while such a structure results in a well-matched dielectric\u0026nbsp;..."},{"page_id":"PA140","page_number":"140","snippet_text":"... \u003cb\u003ewaveguide\u003c/b\u003e. However, the reflections from an open end of the metal \u003cb\u003ewaveguide\u003c/b\u003e are considerably higher. Moreover, radiation patterns of \u003cb\u003edielectric\u003c/b\u003e rod antennas are rather stable in the whole frequency band. 7.2.3 GaAs \u003cb\u003edielectric\u003c/b\u003e\u0026nbsp;..."},{"page_id":"PA146","page_number":"146","snippet_text":"... \u003cb\u003edielectric\u003c/b\u003e rod \u003cb\u003ewaveguides\u003c/b\u003e can be well matched with a single - mode metal \u003cb\u003ewaveguide\u003c/b\u003e , and they have low insertion loss in the 75 - 110 GHz frequency range . The insertion loss of Sapphire wavegui- des is very low at frequencies 77 - 98\u0026nbsp;..."},{"page_id":"PA148","page_number":"148","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e might be somewhat lower than the losses at a typical flange connection between two metal waveguides. In ... \u003cb\u003eDielectric waveguide\u003c/b\u003e devices and integrated circuits \u003cb\u003eDielectric waveguides\u003c/b\u003e 148 MILLIMETER-WAVE WAVEGUIDES."},{"page_id":"PA149","page_number":"149","snippet_text":"... \u003cb\u003eDielectric waveguide\u003c/b\u003e devices and integrated circuits \u003cb\u003eDielectric waveguides\u003c/b\u003e for millimeter - wave ... waveguide devices and integrated circuits \u003cb\u003eDielectric waveguides\u003c/b\u003e for integrated circuits Non-radiative \u003cb\u003edielectric waveguide\u003c/b\u003e."},{"page_id":"PA150","page_number":"150","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e The non - radiative dielectric ( NRD ) waveguide was first proposed in [ 3 ] . It is known that if two parallel metal plates are separated by a distance smaller than one half of the wavelength , the electromagnetic\u0026nbsp;..."},{"page_id":"PA152","page_number":"152","snippet_text":"... \u003cb\u003edielectric\u003c/b\u003e waveguiding structures are shown in Figure 8.2. The ground metal plane in the image and in- sulated image \u003cb\u003ewaveguides\u003c/b\u003e makes them applicable in active circuits. The insulated image \u003cb\u003ewaveguide\u003c/b\u003e differs from the image \u003cb\u003ewaveguide\u003c/b\u003e\u0026nbsp;..."},{"page_id":"PA153","page_number":"153","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e , b ) inverted strip \u003cb\u003edielectric waveguide\u003c/b\u003e [ 10 ] . the dielectric strip is chosen to be smaller than that of the so - called guid- ing layer . The electromagnetic wave propagates mainly in the guiding layer which\u0026nbsp;..."},{"page_id":"PA156","page_number":"156","snippet_text":"... \u003cb\u003edielectric waveguides\u003c/b\u003e port 4 port 2 port 3 In the third approach , the second waveguide is connected to the first one like a probe . The end of the second \u003cb\u003edielectric waveguide\u003c/b\u003e is close to the surface of the first waveguide ( Figure 8.7 )\u0026nbsp;..."},{"page_id":"PA157","page_number":"157","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e results in a better isolation . Especially , this effect has been observed when the dimensions of the dielectric rod waveguides were increased . Such directional coupler was used in so - called multistate\u0026nbsp;..."},{"page_id":"PA158","page_number":"158","snippet_text":"... waveguide with light radiation above the bandgap. The schematic structure is shown in Figure 8.11. It consists of an open \u003cb\u003edielectric waveguide\u003c/b\u003e with tapered ends to improve matching with standard metal waveguides, and a light source. It\u0026nbsp;..."},{"page_id":"PA160","page_number":"160","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e and a ferrite pillbox working like a whispering gallery resonator . 8.3 ACTIVE DEVICES Electromagnetic wave amplification and generation is one of the key problems in the design and technology of millimeter - wave\u0026nbsp;..."},{"page_id":"PA162","page_number":"162","snippet_text":"... waveguides is considerably different in comparison with the theory of waves in dielectrics and \u003cb\u003edielectric waveguides\u003c/b\u003e, where the conduction current can be neglected, as well as with the theory of wa- veguides on semiconductors with a\u0026nbsp;..."},{"page_id":"PA170","page_number":"170","snippet_text":"... \u003cb\u003eDIELECTRIC WAVEGUIDE\u003c/b\u003e ANTENNAS As we have already seen, dielectric materials can have rather attractive properties like lower loss, cost, much larger tolerances for ... WAVEGUIDES \u003cb\u003eDielectric waveguide\u003c/b\u003e antennas 1 Classification."},{"page_id":"PA171","page_number":"171","snippet_text":"... Dielectric antennas Broad side End fire Lense Leaky wave Dielectric Dielectric Dielectric resonator rod horn - Luneberg Figure 8.17 ... \u003cb\u003edielectric waveguide\u003c/b\u003e is an open transmission. Devices and circuits 171 2 Dielectric rod antennas."},{"page_id":"PA172","page_number":"172","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e is an open transmission line, therefore at any discontinuity at its surface radiation in the surrounding media occurs. Waves traveling along the waveguide and radiating into space from the surface of the dielectric\u0026nbsp;..."},{"page_id":"PA173","page_number":"173","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e is radiated . The rest of the power causes a peak in the end fire direction , and to prevent this effect the power reaching the waveguide end should be absorbed . Therefore , the antenna efficiency is not very high\u0026nbsp;..."},{"page_id":"PA174","page_number":"174","snippet_text":"... \u003cb\u003edielectric waveguide\u003c/b\u003e filters, Electronics and Com- munications in Japan, Part 1, vol. 69, no. 5, 1986, pp. 83-89. [5] K. Wu, Hybrid integration technology of planar circuits and NRD- guide for cost-effective microwave and millimeter\u0026nbsp;..."},{"page_id":"PA176","page_number":"176","snippet_text":"... \u003cb\u003edielectric\u003c/b\u003e image limes, IEEE Transactions on Microwave Theory and Techniques, vol. MTT-29, September 1981, pp. 891-896. [25] K. Solbach, The calculation and the measurement of the coupling properties of \u003cb\u003edielectric\u003c/b\u003e image lines of\u0026nbsp;..."},{"page_id":"PA179","page_number":"179","snippet_text":"... \u003cb\u003ewaveguide\u003c/b\u003e at V band, Electronics Letters, vol 30, no. 11, 1994, pp. 869-870. [59] D. Lioubtchenko, S. Dudorov ... \u003cb\u003edielectric\u003c/b\u003e rod antenna, Proceedings of IEE Seventh International Conference on Antennas and Propaga- tion, 1991, pp\u0026nbsp;..."},{"page_id":"PA187","page_number":"187","snippet_text":"... \u003cb\u003edielectric waveguides\u003c/b\u003e with uniaxial cores with the axis parallel to the waveguide axis are provided on disk. The algorithms, described in detail is Chapter 5, Sections 5.3.1 and 5.3.2, have been realized in Matlab programming language\u0026nbsp;..."},{"page_id":"PA188","page_number":"188","snippet_text":"... \u003cb\u003ewaveguide\u003c/b\u003e 8, 49, 87, 92, 96 antenna \u003cb\u003edielectric\u003c/b\u003e rod 137, 140, 171 leaky-wave 151, 170, 172, 173 bias field 64-67, 70-73 boundary condition Dirichlet 9 for open \u003cb\u003ewaveguides\u003c/b\u003e 19 Neumann 10, 17 bulk element 5 Casimir 63 crystal anisotropic 2\u0026nbsp;...","page_url":"https://books.google.com.sg/books?id=CoihHs1Ctp4C\u0026pg=PA188\u0026vq=%22dielectric+waveguide"},{"page_id":"PA189","page_number":"189","snippet_text":"... , 170- 173 \u003cb\u003edielectric\u003c/b\u003e rod 61, 82, 87, 88, 92, 95, 99, 115-118, 122, 126, 135-137 image 152, 168 insulated image 152 inverted strip \u003cb\u003edielectric\u003c/b\u003e 153 non-radiative 149-151 open 2, 5, 18-20, 22, 57, 71 planar 21, 149 190 MILLIMETER-WAVE\u0026nbsp;...","page_url":"https://books.google.com.sg/books?id=CoihHs1Ctp4C\u0026pg=PA189\u0026vq=%22dielectric+waveguide"}],"search_query_escaped":"\u0026quot;dielectric waveguide"},{});</script></div></div></div><script>(function() {var href = window.location.href;if (href.indexOf('?') !== -1) {var parameters = href.split('?')[1].split('&');for (var i = 0; i < parameters.length; i++) {var param = parameters[i].split('=');if (param[0] == 'focus') {var elem = document.getElementById(param[1]);if (elem) {elem.focus();}}}}})();</script>