Various
\\n\\n
IntechOpen was founded by scientists, for scientists, in order to make book publishing accessible around the globe. Over the last two decades, this has driven Open Access (OA) book publishing whilst levelling the playing field for global academics. Through our innovative publishing model and the support of the research community, we have now published over 5,700 Open Access books and are visited online by over three million academics every month. These researchers are increasingly working in broad technology-based subjects, driving multidisciplinary academic endeavours into human health, environment, and technology.
\\n\\nBy listening to our community, and in order to serve these rapidly growing areas which lie at the core of IntechOpen's expertise, we are launching a portfolio of Open Science journals:
\\n\\nAll three journals will publish under an Open Access model and embrace Open Science policies to help support the changing needs of academics in these fast-moving research areas. There will be direct links to preprint servers and data repositories, allowing full reproducibility and rapid dissemination of published papers to help accelerate the pace of research. Each journal has renowned Editors in Chief who will work alongside a global Editorial Board, delivering robust single-blind peer review. Supported by our internal editorial teams, this will ensure our authors will receive a quick, user-friendly, and personalised publishing experience.
\\n\\n"By launching our journals portfolio we are introducing new, dedicated homes for interdisciplinary technology-focused researchers to publish their work, whilst embracing Open Science and creating a unique global home for academics to disseminate their work. We are taking a leap toward Open Science continuing and expanding our fundamental commitment to openly sharing scientific research across the world, making it available for the benefit of all." Dr. Sara Uhac, IntechOpen CEO
\\n\\n"Our aim is to promote and create better science for a better world by increasing access to information and the latest scientific developments to all scientists, innovators, entrepreneurs and students and give them the opportunity to learn, observe and contribute to knowledge creation. Open Science promotes a swifter path from research to innovation to produce new products and services." Alex Lazinica, IntechOpen founder
\\n\\nIn conclusion, Natalia Reinic Babic, Head of Journal Publishing and Open Science at IntechOpen adds:
\\n\\n“On behalf of the journal team I’d like to thank all our Editors in Chief, Editorial Boards, internal supporting teams, and our scientific community for their continuous support in making this portfolio a reality - we couldn’t have done it without you! With your support in place, we are confident these journals will become as impactful and successful as our book publishing program and bring us closer to a more open (science) future.”
\\n\\nWe invite you to visit the journals homepage and learn more about the journal’s Editorial Boards, scope and vision as all three journals are now open for submissions.
\\n\\nFeel free to share this news on social media and help us mark this memorable moment!
\\n\\n\\n"}]',published:!0,mainMedia:{caption:"",originalUrl:"/media/original/237"}},components:[{type:"htmlEditorComponent",content:'
After years of being acknowledged as the world's leading publisher of Open Access books, today, we are proud to announce we’ve successfully launched a portfolio of Open Science journals covering rapidly expanding areas of interdisciplinary research.
\n\n\n\nIntechOpen was founded by scientists, for scientists, in order to make book publishing accessible around the globe. Over the last two decades, this has driven Open Access (OA) book publishing whilst levelling the playing field for global academics. Through our innovative publishing model and the support of the research community, we have now published over 5,700 Open Access books and are visited online by over three million academics every month. These researchers are increasingly working in broad technology-based subjects, driving multidisciplinary academic endeavours into human health, environment, and technology.
\n\nBy listening to our community, and in order to serve these rapidly growing areas which lie at the core of IntechOpen's expertise, we are launching a portfolio of Open Science journals:
\n\nAll three journals will publish under an Open Access model and embrace Open Science policies to help support the changing needs of academics in these fast-moving research areas. There will be direct links to preprint servers and data repositories, allowing full reproducibility and rapid dissemination of published papers to help accelerate the pace of research. Each journal has renowned Editors in Chief who will work alongside a global Editorial Board, delivering robust single-blind peer review. Supported by our internal editorial teams, this will ensure our authors will receive a quick, user-friendly, and personalised publishing experience.
\n\n"By launching our journals portfolio we are introducing new, dedicated homes for interdisciplinary technology-focused researchers to publish their work, whilst embracing Open Science and creating a unique global home for academics to disseminate their work. We are taking a leap toward Open Science continuing and expanding our fundamental commitment to openly sharing scientific research across the world, making it available for the benefit of all." Dr. Sara Uhac, IntechOpen CEO
\n\n"Our aim is to promote and create better science for a better world by increasing access to information and the latest scientific developments to all scientists, innovators, entrepreneurs and students and give them the opportunity to learn, observe and contribute to knowledge creation. Open Science promotes a swifter path from research to innovation to produce new products and services." Alex Lazinica, IntechOpen founder
\n\nIn conclusion, Natalia Reinic Babic, Head of Journal Publishing and Open Science at IntechOpen adds:
\n\n“On behalf of the journal team I’d like to thank all our Editors in Chief, Editorial Boards, internal supporting teams, and our scientific community for their continuous support in making this portfolio a reality - we couldn’t have done it without you! With your support in place, we are confident these journals will become as impactful and successful as our book publishing program and bring us closer to a more open (science) future.”
\n\nWe invite you to visit the journals homepage and learn more about the journal’s Editorial Boards, scope and vision as all three journals are now open for submissions.
\n\nFeel free to share this news on social media and help us mark this memorable moment!
\n\n\n'}],latestNews:[{slug:"step-in-the-right-direction-intechopen-launches-a-portfolio-of-open-science-journals-20220414",title:"Step in the Right Direction: IntechOpen Launches a Portfolio of Open Science Journals"},{slug:"let-s-meet-at-london-book-fair-5-7-april-2022-olympia-london-20220321",title:"Let’s meet at London Book Fair, 5-7 April 2022, Olympia London"},{slug:"50-books-published-as-part-of-intechopen-and-knowledge-unlatched-ku-collaboration-20220316",title:"50 Books published as part of IntechOpen and Knowledge Unlatched (KU) Collaboration"},{slug:"intechopen-joins-the-united-nations-sustainable-development-goals-publishers-compact-20221702",title:"IntechOpen joins the United Nations Sustainable Development Goals Publishers Compact"},{slug:"intechopen-signs-exclusive-representation-agreement-with-lsr-libros-servicios-y-representaciones-s-a-de-c-v-20211123",title:"IntechOpen Signs Exclusive Representation Agreement with LSR Libros Servicios y Representaciones S.A. de C.V"},{slug:"intechopen-expands-partnership-with-research4life-20211110",title:"IntechOpen Expands Partnership with Research4Life"},{slug:"introducing-intechopen-book-series-a-new-publishing-format-for-oa-books-20210915",title:"Introducing IntechOpen Book Series - A New Publishing Format for OA Books"},{slug:"intechopen-identified-as-one-of-the-most-significant-contributor-to-oa-book-growth-in-doab-20210809",title:"IntechOpen Identified as One of the Most Significant Contributors to OA Book Growth in DOAB"}]},book:{item:{type:"book",id:"6515",leadTitle:null,fullTitle:"Emerging Waveguide Technology",title:"Emerging Waveguide Technology",subtitle:null,reviewType:"peer-reviewed",abstract:"Recently, the rapid development of radiofrequency (RF)/microwave and photonic/optical waveguide technologies has had a significant impact on the current electronic industrial, medical and information and communication technology (ICT) fields. This book is a self-contained collection of valuable scholarly papers related to waveguide design, modeling, and applications. This book contains 20 chapters that cover three main subtopics of waveguide technologies, namely RF and microwave waveguide, photonic and optical waveguide and waveguide analytical solutions. Hence, this book is particularly useful to the academics, scientists, practicing researchers and postgraduate students whose work relates to the latest waveguide technologies.",isbn:"978-1-78923-493-0",printIsbn:"978-1-78923-492-3",pdfIsbn:"978-1-83881-516-5",doi:"10.5772/intechopen.71142",price:139,priceEur:155,priceUsd:179,slug:"emerging-waveguide-technology",numberOfPages:384,isOpenForSubmission:!1,isInWos:1,isInBkci:!1,hash:"12ab2b13b1ca330409dc239647a53895",bookSignature:"Kok Yeow You",publishedDate:"August 1st 2018",coverURL:"https://cdn.intechopen.com/books/images_new/6515.jpg",numberOfDownloads:25837,numberOfWosCitations:45,numberOfCrossrefCitations:46,numberOfCrossrefCitationsByBook:6,numberOfDimensionsCitations:68,numberOfDimensionsCitationsByBook:5,hasAltmetrics:1,numberOfTotalCitations:159,isAvailableForWebshopOrdering:!0,dateEndFirstStepPublish:"September 26th 2017",dateEndSecondStepPublish:"October 17th 2017",dateEndThirdStepPublish:"December 16th 2017",dateEndFourthStepPublish:"March 6th 2018",dateEndFifthStepPublish:"May 5th 2018",currentStepOfPublishingProcess:5,indexedIn:"1,2,3,4,5,6,7",editedByType:"Edited by",kuFlag:!1,featuredMarkup:null,editors:[{id:"188673",title:"Dr.",name:"Kok Yeow",middleName:null,surname:"You",slug:"kok-yeow-you",fullName:"Kok Yeow You",profilePictureURL:"https://mts.intechopen.com/storage/users/188673/images/5521_n.jpg",biography:"Dr. Kok Yeow You obtained his BSc degree in Physics (Honors) from the Universiti Kebangsaan Malaysia (UKM) in 2001. He pursued his MSc degree in Microwave from the Faculty of Science in 2003 and his PhD degree in Wave Propagation from the Institute for Mathematical Research, Universiti Putra Malaysia (UPM), Serdang, Selangor, Malaysia in 2006. His main personal research interest includes the theory, simulation, and instrumentation of electromagnetic wave propagation at microwave frequencies focusing on the development of microwave passive devices and sensors for medical and agricultural applications. For the past 17 years, he has developed numerous projects concerning microwave waveguide measurement systems for agri-/food, biomedical processing, and microwave devices for biomedical treatments, as well as numerical electromagnetic modeling.",institutionString:null,position:null,outsideEditionCount:0,totalCites:0,totalAuthoredChapters:"3",totalChapterViews:"0",totalEditedBooks:"2",institution:{name:"University of Technology Malaysia",institutionURL:null,country:{name:"Malaysia"}}}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,coeditorOne:null,coeditorTwo:null,coeditorThree:null,coeditorFour:null,coeditorFive:null,topics:[{id:"116",title:"Electrical and Electronic Engineering",slug:"electrical-and-electronic-engineering"}],chapters:[{id:"61901",title:"Broadband Slotted Waveguide Array Antenna",doi:"10.5772/intechopen.78308",slug:"broadband-slotted-waveguide-array-antenna",totalDownloads:1899,totalCrossrefCites:4,totalDimensionsCites:4,hasAltmetrics:1,abstract:"This chapter describes the design and development of broadband slotted waveguide array (SWA) antenna. Conventional SWA antenna offers a few percentages of bandwidth, which can be enhanced using proposed novel differential feeding technique which electrically divides large resonating SWA into wideband subarrays by creating virtual shorts. This chapter discusses concepts to achieve broadband nature of SWA antennas, design, development, and characterization of edge fed slotted waveguide array antenna, coupling slot fed SWA antenna, and high efficiency broadband slotted waveguide array. The developed SWA antennas are characterized and their measured results are presented. The developed prototype of proposed SWA antenna demonstrates measured return loss better than −17 dB over 7.6% bandwidth and achieves 90.2% antenna efficiency. This chapter also briefs about planar broadband SWA antenna and its prototype development and characterization.",signatures:"Yogesh Tyagi and Pratik Mevada",downloadPdfUrl:"/chapter/pdf-download/61901",previewPdfUrl:"/chapter/pdf-preview/61901",authors:[{id:"228031",title:"Mr.",name:"Yogesh",surname:"Tyagi",slug:"yogesh-tyagi",fullName:"Yogesh Tyagi"},{id:"228559",title:"Mr.",name:"Pratik",surname:"Mevada",slug:"pratik-mevada",fullName:"Pratik Mevada"}],corrections:null},{id:"61284",title:"Photonic Crystal Waveguides",doi:"10.5772/intechopen.76797",slug:"photonic-crystal-waveguides",totalDownloads:1342,totalCrossrefCites:0,totalDimensionsCites:0,hasAltmetrics:0,abstract:"The original results of theoretical and experimental studies and the properties of microwave one-dimensional waveguide photonic crystals have been generalized. Methods for describing the electrodynamic characteristics of photonic crystals and their relationship with the parameters of periodic structures filling the waveguides have been presented. The results of an investigation on the characteristics of microwave waveguide photonic crystals made in the form of dielectric matrices with air inclusions have been presented. The model of effective dielectric permittivity has been proposed for describing the characteristics of the investigated photonic crystals containing layers with a large number of air inclusions. New types of microwave low-dimensional waveguide photonic crystals containing periodically alternating elements that are sources of higher type waves have been described. The possibility of effective control of the amplitude-frequency characteristics of microwave photonic crystals by means of electric and magnetic fields has been analyzed. Examples of new applications of waveguide photonic crystals in the microwave range have been given: the measuring parameters of the materials and semiconductor nanostructures that play the role of the microwave photonic crystals' periodicity defect; the resonators of near-field microwave microscopes; small-sized matched loads for centimeter and millimeter wavelength ranges on the basis of microwave photonic crystals.",signatures:"Dmitry Usanov and Alexander Skripal",downloadPdfUrl:"/chapter/pdf-download/61284",previewPdfUrl:"/chapter/pdf-preview/61284",authors:[{id:"228739",title:"Prof.",name:"Dmitry",surname:"Usanov",slug:"dmitry-usanov",fullName:"Dmitry Usanov"},{id:"230179",title:"Prof.",name:"Alexander",surname:"Skripal",slug:"alexander-skripal",fullName:"Alexander Skripal"}],corrections:null},{id:"60948",title:"High-Gain Amplifier Module Integrating a Waveguide into the Module Case for Millimeter Wave Applications",doi:"10.5772/intechopen.76622",slug:"high-gain-amplifier-module-integrating-a-waveguide-into-the-module-case-for-millimeter-wave-applicat",totalDownloads:820,totalCrossrefCites:0,totalDimensionsCites:0,hasAltmetrics:0,abstract:"A high-gain amplifier module with integrated waveguide (WG) has been presented for millimeter wave applications. In order to improve the isolation between the amplification stages in the multi-stage amplifier module, an isolated WG is integrated into the module case. It is possible to effectively suppress the oscillation occurring in the high gain stage. Microstrip line (MSL)-to-WG transitions are designed and fabricated on a 5 mil thick RT5880 substrate for interconnection of the isolated WG, input/output WG and amplifier PCB in a cascaded two-stage high gain amplifier module. The transition loss of −0.44 dB is obtained at 40 GHz and return-loss (S11) bandwidth below −10 dB is from 34.1 to 50 GHz. The fabricated high-gain amplifier module shows a high gain over 39.7 dB from 38 to 41 GHz. At 38.7 GHz, its maximum gain of 44.25 dB is achieved.",signatures:"Young Chul Lee",downloadPdfUrl:"/chapter/pdf-download/60948",previewPdfUrl:"/chapter/pdf-preview/60948",authors:[{id:"188444",title:"Prof.",name:"Young Chul",surname:"Lee",slug:"young-chul-lee",fullName:"Young Chul Lee"}],corrections:null},{id:"61194",title:"Mathematical Analysis of Electrical Breakdown Effects in Waveguides",doi:"10.5772/intechopen.76973",slug:"mathematical-analysis-of-electrical-breakdown-effects-in-waveguides",totalDownloads:892,totalCrossrefCites:0,totalDimensionsCites:0,hasAltmetrics:0,abstract:"The designers of microwave devices in the industry use the analytical solutions of the corona discharge equation to determine the minimum power breakdown threshold, in a particular device, such as waveguides and filters, and know whether it is in the established margins. There are two main ways to determine the breakdown threshold of a waveguide analytically; the most commonly used describes the plasma density generation completely as a function of the geometry by using the characteristic diffusion length, while the second is a more thorough method that involves the use of the effective diffusion length which considers collision frequency and electric field into the equations. Hence the aim of the designers is to obtain the closest results to experimental results, both methods must be considered in addition to the environmental changes so that they know the operational limits. This chapter describes the different methods to obtain analytical results for the breakdown threshold in any rectangular waveguide device, the influence of environmental conditions in the analysis and the inhomogeneous electric field effect inside the devices.",signatures:"Isaac Medina and Primo-Alberto Calva",downloadPdfUrl:"/chapter/pdf-download/61194",previewPdfUrl:"/chapter/pdf-preview/61194",authors:[{id:"225982",title:"Dr.",name:"Isaac",surname:"Medina",slug:"isaac-medina",fullName:"Isaac Medina"},{id:"225986",title:"Dr.",name:"Primo",surname:"Calva",slug:"primo-calva",fullName:"Primo Calva"}],corrections:null},{id:"62346",title:"Optical Waveguide for Measurement Application",doi:"10.5772/intechopen.76781",slug:"optical-waveguide-for-measurement-application",totalDownloads:902,totalCrossrefCites:0,totalDimensionsCites:0,hasAltmetrics:0,abstract:"The chapter provides the analysis of the behaviour of Mach Zehnder interferometer waveguide (MZIW) sensing structure and establishes the general design principles. Photonics interferometers have been widely used because of their highly sensitive detection technique. The present study is based on the MZIW structure for sensing application and deals with interferometer single-mode transmission. Theoretically, short wavelength and high difference in index (Δη) results in the low depth of the evanescence wave and increase in sensitivity. MZIW under consideration is very small in size hence it is very difficult to guide the light into waveguide. The output monitor detection sensitivity of the entire MZI structure depends on light-guiding efficiency. To maintain minimum losses at various micro-branches of the entire MZIW structure, effective light propagation is important and it is a critical parameter of the entire interferometer. Various tests have been carried out to study the effects of the Y branch angle variation on light guiding into the MZIW structure especially in measurement application.",signatures:"Prashant Bansilal Patel and Satish T. Hamde",downloadPdfUrl:"/chapter/pdf-download/62346",previewPdfUrl:"/chapter/pdf-preview/62346",authors:[{id:"223158",title:"Mr.",name:"Prashant",surname:"Patel",slug:"prashant-patel",fullName:"Prashant Patel"},{id:"245227",title:"Prof.",name:"Satish",surname:"Hamde",slug:"satish-hamde",fullName:"Satish Hamde"}],corrections:null},{id:"61838",title:"Review on Optical Waveguides",doi:"10.5772/intechopen.77150",slug:"review-on-optical-waveguides",totalDownloads:4777,totalCrossrefCites:19,totalDimensionsCites:29,hasAltmetrics:1,abstract:"Optical devices are necessary to meet the anticipated future requirements for ultrafast and ultrahigh bandwidth communication and computing. All optical information processing can overcome optoelectronic conversions that limit both the speed and bandwidth and are also power consuming. The building block of an optical device/circuit is the optical waveguide, which enables low-loss light propagation and is thereby used to connect components and devices. This chapter reviews optical waveguides and their classification on the basis of geometry (Non-Planar (Slab/Optical Fiber)/Planar (Buried Channel, Strip-Loaded, Wire, Rib, Diffused, Slot, etc.)), refractive index (Step/Gradient Index), mode propagation (Single/Multimode), and material platform (Glass/Polymer/Semiconductor, etc.). A comparative analysis of waveguides realized in different material platforms along with the propagation loss is also presented.",signatures:"Shankar Kumar Selvaraja and Purnima Sethi",downloadPdfUrl:"/chapter/pdf-download/61838",previewPdfUrl:"/chapter/pdf-preview/61838",authors:[{id:"236949",title:"Prof.",name:"Shankar Kumar",surname:"Selvaraja",slug:"shankar-kumar-selvaraja",fullName:"Shankar Kumar Selvaraja"},{id:"249514",title:"Dr.",name:"Purnima",surname:"Sethi",slug:"purnima-sethi",fullName:"Purnima Sethi"}],corrections:null},{id:"61264",title:"Graphene Based Waveguides",doi:"10.5772/intechopen.76796",slug:"graphene-based-waveguides",totalDownloads:1521,totalCrossrefCites:0,totalDimensionsCites:0,hasAltmetrics:0,abstract:"Graphene, which is well known as a one-atom thick carbon allotrope, has drawn lots of attention since its first announcement due to remarkable performance in mechanical, electrical, magnetic, thermal, and optical areas. In particular, unique properties of graphene such as low net absorption in broadband optical band, notably high nonlinear optical effects, and gate-variable optical conductivity make it an excellent candidate for high speed, high performance, and broadband electronic and photonics devices. Embedding graphene into optical devices longitudinally would enhance the light-graphene interaction, which shows great potential in photonic components. Since the carrier density of graphene could be tuned by external gate voltage, chemical doping, light excitation, graphene-based waveguide modulator could be designed to have high flexibility in controlling the absorption and modulation depth. Furthermore, graphene-based waveguides could take advantages in detection, sensing, polarizer, and so on.",signatures:"Xianglian Song, Xiaoyu Dai and Yuanjiang Xiang",downloadPdfUrl:"/chapter/pdf-download/61264",previewPdfUrl:"/chapter/pdf-preview/61264",authors:[{id:"106075",title:"Dr.",name:"Yuanjiang",surname:"Xiang",slug:"yuanjiang-xiang",fullName:"Yuanjiang Xiang"},{id:"226350",title:"Dr.",name:"Xianglian",surname:"Song",slug:"xianglian-song",fullName:"Xianglian Song"},{id:"226500",title:"Prof.",name:"Xiaoyu",surname:"Dai",slug:"xiaoyu-dai",fullName:"Xiaoyu Dai"}],corrections:null},{id:"61408",title:"Lithium Niobate Optical Waveguides and Microwaveguides",doi:"10.5772/intechopen.76798",slug:"lithium-niobate-optical-waveguides-and-microwaveguides",totalDownloads:2259,totalCrossrefCites:5,totalDimensionsCites:5,hasAltmetrics:1,abstract:"Lithium niobate has attracted much attention since the 1970s due to its capacity to modify the light by means of an electric control. In this chapter, we review the evolution of electro-optical (EO) lithium niobate waveguides throughout the years, from Ti-indiffused waveguides to photonic crystals. The race toward ever smaller EO components with ever-lower optical losses and power consumption has stimulated numerous studies, the challenge consisting of strongly confining the light while preserving low losses. We show how waveguides have evolved toward ridges or thin film-based microguides to increase the EO efficiency and reduce the driving voltage. In particular, a focus is made on an easy-to-implement technique using a circular precision saw to produce thin ridge waveguides or suspended membranes with low losses.",signatures:"Nadège Courjal, Maria-Pilar Bernal, Alexis Caspar, Gwenn Ulliac,\nFlorent Bassignot, Ludovic Gauthier-Manuel and Miguel Suarez",downloadPdfUrl:"/chapter/pdf-download/61408",previewPdfUrl:"/chapter/pdf-preview/61408",authors:[{id:"31946",title:"Mr.",name:"Gwenn",surname:"Ulliac",slug:"gwenn-ulliac",fullName:"Gwenn Ulliac"},{id:"31950",title:"Mr.",name:"Florent",surname:"Bassignot",slug:"florent-bassignot",fullName:"Florent Bassignot"},{id:"223063",title:"Associate Prof.",name:"Nadege",surname:"Bodin Courjal",slug:"nadege-bodin-courjal",fullName:"Nadege Bodin Courjal"},{id:"227862",title:"Prof.",name:"Maria-Pilar",surname:"Bernal",slug:"maria-pilar-bernal",fullName:"Maria-Pilar Bernal"},{id:"239866",title:"Mr.",name:"Alexis",surname:"Caspar",slug:"alexis-caspar",fullName:"Alexis Caspar"},{id:"239868",title:"Mr.",name:"Ludovic",surname:"Gautier-Manuel",slug:"ludovic-gautier-manuel",fullName:"Ludovic Gautier-Manuel"},{id:"239932",title:"Dr.",name:"Miguel",surname:"Suarez",slug:"miguel-suarez",fullName:"Miguel Suarez"}],corrections:null},{id:"59919",title:"Raman Solitons in Nanoscale Optical Waveguides, with Metamaterials, Having Polynomial Law Nonlinearity Using Collective Variables",doi:"10.5772/intechopen.75121",slug:"raman-solitons-in-nanoscale-optical-waveguides-with-metamaterials-having-polynomial-law-nonlinearity",totalDownloads:985,totalCrossrefCites:0,totalDimensionsCites:0,hasAltmetrics:0,abstract:"A mathematical analysis is conducted to illustrate the controllability of the Raman soliton self-frequency shift with polynomial nonlinearity in metamaterials by using collective variable method. The polynomial nonlinearity is due to the expanding nonlinear polarization \n\n\nP\nNL\n\n\n in a series over the field \n\nE\n\n up to the seventh order. Gaussian assumption is selected to these pulses on a generalized mode. The numerical simulation of soliton parameter variation is given for the Gaussian pulse parameters.",signatures:"Yanan Xu, Jun Ren and Matthew C. Tanzy",downloadPdfUrl:"/chapter/pdf-download/59919",previewPdfUrl:"/chapter/pdf-preview/59919",authors:[{id:"223008",title:"Dr.",name:"Yanan",surname:"Xu",slug:"yanan-xu",fullName:"Yanan Xu"},{id:"223668",title:"Dr.",name:"Matthew",surname:"Tanzy",slug:"matthew-tanzy",fullName:"Matthew Tanzy"},{id:"248250",title:"Dr.",name:"Jun",surname:"Ren",slug:"jun-ren",fullName:"Jun Ren"}],corrections:null},{id:"60221",title:"Silicon-on-Insulator Slot Waveguides: Theory and Applications in Electro-Optics and Optical Sensing",doi:"10.5772/intechopen.75539",slug:"silicon-on-insulator-slot-waveguides-theory-and-applications-in-electro-optics-and-optical-sensing",totalDownloads:1855,totalCrossrefCites:16,totalDimensionsCites:26,hasAltmetrics:0,abstract:"This chapter deals with the basic concept of silicon-on-insulator (SOI) slot waveguides, including slot waveguide theory, fabrication steps, and applications. First, in the theory section, a modal field expression and the characteristic equation is derived, which is also valid for higher-order modes. SOI slot waveguide structures are simulated and characteristic values like the effective refractive indices and the field confinement factors are determined. The fabrication section describes typical SOI fabrication steps and the limits of current fabrication techniques. Additionally, developments regarding loss reduction in SOI slot waveguides are given from the fabrication point of view. This is followed by the theory and practice of slot waveguide based electro-optical modulators. Here, the SOI slot waveguide is embedded in an organic nonlinear optical material in order to achieve record-low voltage-length products. In the field of optical sensors, it is shown that slot waveguides enable remarkable waveguide sensitivity for both refractive index sensing and surface sensing.",signatures:"Patrick Steglich",downloadPdfUrl:"/chapter/pdf-download/60221",previewPdfUrl:"/chapter/pdf-preview/60221",authors:[{id:"223128",title:"Dr.",name:"Patrick",surname:"Steglich",slug:"patrick-steglich",fullName:"Patrick Steglich"}],corrections:null},{id:"61148",title:"Investigation of Ring Waveguide Add/Drop with Grating Couple",doi:"10.5772/intechopen.76800",slug:"investigation-of-ring-waveguide-add-drop-with-grating-couple",totalDownloads:908,totalCrossrefCites:0,totalDimensionsCites:0,hasAltmetrics:0,abstract:"The silicon photon technology platform is low transmission loss, small size, low cost of the process and easy integration with electronic components and other characteristics. It is designed to design high-density optical communication network system has a considerable advantage. Such as high-density wavelength division multiplexing (DWDM) system, that is through the different wavelengths of signal processing. So that it can be used for optical connection switches, routing and other applications. It composed of a DWDM system, through the Mach-Zehnder interferometer, ring resonator (Add/Drop), array waveguide grating (AWG) and grating coupler and other structural components. It is designed by components to filter, switch, adjust and detect functions. The characteristics of the ring resonator are for wavelength selection. It is suitable for the design of optical switches, signal switching and modulation applications. It is also the focus of this lab and this chapter to explore and study. The general edge coupling, between the optical fiber and the waveguide dimension is very different. As a result, larger insertion loss is caused. This study uses the vertical coupling method to investigate the characteristics of a ring resonator.",signatures:"Jian-Chiun Liou",downloadPdfUrl:"/chapter/pdf-download/61148",previewPdfUrl:"/chapter/pdf-preview/61148",authors:[{id:"222901",title:"Prof.",name:"Jian-Chiun",surname:"Liou",slug:"jian-chiun-liou",fullName:"Jian-Chiun Liou"}],corrections:null},{id:"60915",title:"Multimode Waveguides on an SOI Platform for Arbitrary Power Splitting Ratio Couplers",doi:"10.5772/intechopen.76799",slug:"multimode-waveguides-on-an-soi-platform-for-arbitrary-power-splitting-ratio-couplers",totalDownloads:921,totalCrossrefCites:0,totalDimensionsCites:1,hasAltmetrics:0,abstract:"Optical power couplers with arbitrary power splitting ratios are important components for many applications such as Mach-Zehnder interferometer-based structures, filters, switches, dispersion compensations, optical interconnects, and microring resonators. In this chapter, we present a new approach to achieve a very high compact coupler with arbitrary power splitting ratios on silicon on insulator (SOI) waveguides. The proposed device requires only one 4×4 multimode interference (MMI) coupler. We use a passive wide SOI waveguide to achieve the phase shifter. The footprint of the whole device is only about 6×150 μm2. A large fabrication tolerance of ±50 nm can be achieved. The modified effective index method, beam propagation method, finite difference method, and finite difference-time difference method are used to optimally design the whole device.",signatures:"Trung-Thanh Le and Duy-Tien Le",downloadPdfUrl:"/chapter/pdf-download/60915",previewPdfUrl:"/chapter/pdf-preview/60915",authors:[{id:"223579",title:"Prof.",name:"Trung-Thanh",surname:"Le",slug:"trung-thanh-le",fullName:"Trung-Thanh Le"},{id:"240025",title:"Dr.",name:"Duy-Tien",surname:"Le",slug:"duy-tien-le",fullName:"Duy-Tien Le"}],corrections:null},{id:"60830",title:"Longitudinal Differential Protection of Power Systems Transmission Lines Using Optical Waveguide",doi:"10.5772/intechopen.76621",slug:"longitudinal-differential-protection-of-power-systems-transmission-lines-using-optical-waveguide",totalDownloads:1159,totalCrossrefCites:0,totalDimensionsCites:0,hasAltmetrics:0,abstract:"This chapter describes using optical waveguide for communication between two relays on the opposite ends of the power systems transmission line (or transmission line). Transmission lines are a very important part of the power system. Because of that, relay protection must be fast and safe. Longitudinal differential protection satisfies these requirements. Pilot wire differential relays are commonly used for the protection of short lines. The existence of the pilot wires is a disadvantage. This protection is limited to lines of a few tens of kilometers. However, if optical protection ground wires (OPGWs) are used, instead of pilot wires, the length of the line ceases to be a limiting factor. The following sections tell more about constructions, assembly and utilization of the optical waveguides in differential protection. Also, the newest algorithms of this protection are listed.",signatures:"Tomislav Rajić",downloadPdfUrl:"/chapter/pdf-download/60830",previewPdfUrl:"/chapter/pdf-preview/60830",authors:[{id:"227492",title:"M.Sc.",name:"Tomislav",surname:"Rajić",slug:"tomislav-rajic",fullName:"Tomislav Rajić"}],corrections:null},{id:"60096",title:"End-Fire Mode Spectroscopy: A Measuring Technique for Optical Waveguides",doi:"10.5772/intechopen.75558",slug:"end-fire-mode-spectroscopy-a-measuring-technique-for-optical-waveguides",totalDownloads:898,totalCrossrefCites:0,totalDimensionsCites:0,hasAltmetrics:0,abstract:"End-fire mode spectroscopy technique provides reliable measurement of the whole mode spectrum of optical waveguides having arbitrary cross refractive index profile. The method is based on registration of light beams radiated from the abrupt output edge of the waveguide, with each beam corresponding to the individual waveguide mode. Due to different values of mode propagation constants, modes of different orders demonstrate different refraction angles at the output waveguide face when modes reach that face under the same nonzero inclination angle. Just this feature is used in the technique. Mode excitation is performed directly through the input waveguide face, and therefore the technique can be applied to analyze mode spectrum of arbitrary waveguides, including the ones with non-monotonic index profiles (particularly, symmetric step-index profiles or buried graded-index waveguides with any burying depths).",signatures:"Dmitry V. Svistunov",downloadPdfUrl:"/chapter/pdf-download/60096",previewPdfUrl:"/chapter/pdf-preview/60096",authors:[{id:"200376",title:"Dr.",name:"Dmitry",surname:"Svistunov",slug:"dmitry-svistunov",fullName:"Dmitry Svistunov"}],corrections:null},{id:"61252",title:"Polymer Resonant Waveguide Gratings",doi:"10.5772/intechopen.76917",slug:"polymer-resonant-waveguide-gratings",totalDownloads:1082,totalCrossrefCites:1,totalDimensionsCites:1,hasAltmetrics:0,abstract:"This chapter deals with the advances in polymeric waveguide gratings for filtering and integrated optics applications. Optical polymer materials are widely used for planar and corrugated micro-optical waveguide grating structures ranging from down a micrometer to several hundred micrometers. Light in a polymeric waveguide is transmitted in discrete modes whose propagation orders depend on incident wavelength, waveguide dimensional parameters, and material properties. Diffracted optical structures are permittivity-modulated microstructures whose micro-relief surface profiles exhibit global/local periodicity. The resonant nature and location of such globally periodic structures (diffraction gratings) excite leaky waveguide modes which couple incident light into reflected/transmitted plane wave diffraction orders. It describes design & analysis, fabrication, and characterization of sub-wavelength polymer grating structures replicated in different polymeric materials (polycarbonate, cyclic olefin copolymer, Ormocomp) by a simple, cost-effective, accurate, and large scale production method. The master stamp (mold) for polymer replication is fabricated with an etchless process with smooth surface profile.",signatures:"Muhammad Rizwan Saleem and Rizwan Ali",downloadPdfUrl:"/chapter/pdf-download/61252",previewPdfUrl:"/chapter/pdf-preview/61252",authors:[{id:"227567",title:"Prof.",name:"Muhammad Rizwan",surname:"Saleem",slug:"muhammad-rizwan-saleem",fullName:"Muhammad Rizwan Saleem"},{id:"398554",title:"Dr.",name:"Rizwan",surname:"Ali",slug:"rizwan-ali",fullName:"Rizwan Ali"}],corrections:null},{id:"61296",title:"Applications and Solving Techniques of Propagated Wave in Waveguides Filled with Inhomogeneous Dielectric Materials",doi:"10.5772/intechopen.76793",slug:"applications-and-solving-techniques-of-propagated-wave-in-waveguides-filled-with-inhomogeneous-diele",totalDownloads:1026,totalCrossrefCites:0,totalDimensionsCites:0,hasAltmetrics:0,abstract:"This chapter presents techniques to solve problems of propagation along the straight rectangular and circular waveguides with inhomogeneous dielectric materials in the cross section. These techniques are very important to improve the methods that are based on Laplace and Fourier transforms and their inverse transforms also for the discontinuous rectangular and circular profiles in the cross section (and not only for the continuous profiles). The main objective of this chapter is to develop the techniques that enable us to solve problems with inhomogeneous dielectric materials in the cross section of the straight rectangular and circular waveguides. The second objective is to understand the influence of the inhomogeneous dielectric materials on the output fields. The method in this chapter is based on the Laplace and Fourier transforms and their inverse transforms. The proposed techniques together with the methods that are based on Laplace and Fourier transforms and their inverse transforms are important to improve the methods also for the discontinuous rectangular and circular profiles in the cross section. The applications are useful for straight waveguides in the microwave and the millimeter-wave regimes, for the straight hollow waveguide and for infrared field, also in the cases of inhomogeneous dielectric materials in the cross section.",signatures:"Zion Menachem",downloadPdfUrl:"/chapter/pdf-download/61296",previewPdfUrl:"/chapter/pdf-preview/61296",authors:[{id:"147585",title:"Dr.",name:"Zion",surname:"Menachem",slug:"zion-menachem",fullName:"Zion Menachem"}],corrections:null},{id:"61256",title:"Periodic Rectangular and Circular Profiles in the Cross Section of the Straight Waveguide Based on Laplace and Fourier Transforms and Their Inverse Transforms and Applications",doi:"10.5772/intechopen.76794",slug:"periodic-rectangular-and-circular-profiles-in-the-cross-section-of-the-straight-waveguide-based-on-l",totalDownloads:955,totalCrossrefCites:0,totalDimensionsCites:0,hasAltmetrics:0,abstract:"This chapter presents propagation along the straight rectangular waveguide with periodic rectangular and circular profiles in the cross section. The objectives in this study are to explore the effect of the periodic rectangular and circular profiles in the cross section of the straight waveguide on the output field and to develop the technique to calculate two kinds of the periodic profiles. The method is based on Laplace and Fourier transforms and the inverse Laplace and Fourier transforms. The contribution of the proposed technique is important to improve the method that is based on Laplace and Fourier transforms and their inverse transforms also for the discontinuous periodic rectangular and circular profiles in the cross section (and not only for the continuous profiles). The proposed technique is very effective to solve complex problems, in relation to the conventional methods, especially when we have a large numbers of dielectric profiles. The application is useful for straight waveguides in the microwave and the millimeter wave regimes, with periodic rectangular and circular profiles in the cross section of the straight waveguide.",signatures:"Zion Menachem",downloadPdfUrl:"/chapter/pdf-download/61256",previewPdfUrl:"/chapter/pdf-preview/61256",authors:[{id:"147585",title:"Dr.",name:"Zion",surname:"Menachem",slug:"zion-menachem",fullName:"Zion Menachem"}],corrections:null},{id:"59870",title:"A Theoretical Model of the Holographic Formation of Controllable Waveguide Channels System in Photopolymer Liquid Crystalline Composition",doi:"10.5772/intechopen.74838",slug:"a-theoretical-model-of-the-holographic-formation-of-controllable-waveguide-channels-system-in-photop",totalDownloads:806,totalCrossrefCites:0,totalDimensionsCites:1,hasAltmetrics:0,abstract:"Rapid development of the integrated optics and photonics makes it necessary to create cheap and simple technology of optical waveguide systems formation. Photolithography methods, widely used for these tasks recently, require the production of a number of precision amplitude and phase masks. This fact makes this technology expensive and the formation process long. On another side there is a cheap and one-step holographic recording method in photopolymer compositions. Parameters of the waveguide system formed by this method are determined by recording geometry and material’s properties. Besides, compositions may contain liquid crystals that make it possible to create elements, controllable by external electric field. In this chapter, the theoretical model of the holographic formation of controllable waveguide channels system in photopolymer liquid crystalline composition is developed. Special attention is paid to localization of waveguides in the media caused by light field attenuation during the formation process.",signatures:"Artem Semkin and Sergey Sharangovich",downloadPdfUrl:"/chapter/pdf-download/59870",previewPdfUrl:"/chapter/pdf-preview/59870",authors:[{id:"226143",title:"Ph.D.",name:"Sergey",surname:"Sharangovich",slug:"sergey-sharangovich",fullName:"Sergey Sharangovich"},{id:"226145",title:"Dr.",name:"Artem",surname:"Semkin",slug:"artem-semkin",fullName:"Artem Semkin"}],corrections:null},{id:"59829",title:"Application of Numeric Routine for Simulating Transients in Power Line Communication (PLC) Systems",doi:"10.5772/intechopen.74753",slug:"application-of-numeric-routine-for-simulating-transients-in-power-line-communication-plc-systems",totalDownloads:830,totalCrossrefCites:1,totalDimensionsCites:1,hasAltmetrics:0,abstract:"Applying numerical routines based on trapezoidal rule of integration (Heun’s method for numerical integration), simple models of transmission lines are used to analyze and simulate the propagation of communication signals in PLC-type systems (power line communication systems). Such systems are shared by the same systems for the transfer of electrical power and signal transmission. For the mentioned routines, the main objectives are: simulate the propagation of electromagnetic transients in these systems and analyze the interference of such phenomena in the transmitted signal. Such simulations are performed with classical structures that represent infinitesimal units of transmission lines. Modifications in the structure of such units are analyzed to improve the results obtained by the mentioned simulations.",signatures:"Afonso José do Prado, Luis Henrique Jus, Melissa de Oliveira Santos,\nElmer Mateus Gennaro, André Alves Ferreira, Thainá Guimarães\nPereira, Aghatta Cioqueta Moreira, Juliana Semiramis Menzinger,\nCaio Vinícius Colozzo Grilo, Marinez Cargnin Stieler and José\nPissolato Filho",downloadPdfUrl:"/chapter/pdf-download/59829",previewPdfUrl:"/chapter/pdf-preview/59829",authors:[{id:"148612",title:"Dr.",name:"Afonso",surname:"Prado",slug:"afonso-prado",fullName:"Afonso Prado"},{id:"148614",title:"Dr.",name:"José",surname:"Pissolato Filho",slug:"jose-pissolato-filho",fullName:"José Pissolato Filho"},{id:"239891",title:"Mr.",name:"Luis Henrique",surname:"Jus",slug:"luis-henrique-jus",fullName:"Luis Henrique Jus"},{id:"239892",title:"Ms.",name:"Melissa De Oliveira",surname:"Santos",slug:"melissa-de-oliveira-santos",fullName:"Melissa De Oliveira Santos"},{id:"239893",title:"Dr.",name:"Elmer Mateus",surname:"Gennaro",slug:"elmer-mateus-gennaro",fullName:"Elmer Mateus Gennaro"},{id:"239894",title:"Dr.",name:"André",surname:"Ferreira",slug:"andre-ferreira",fullName:"André Ferreira"},{id:"239895",title:"Ms.",name:"Thainá Guimarães",surname:"Pereira",slug:"thaina-guimaraes-pereira",fullName:"Thainá Guimarães Pereira"},{id:"239896",title:"Ms.",name:"Aghatta Cioqueta",surname:"Moreira",slug:"aghatta-cioqueta-moreira",fullName:"Aghatta Cioqueta Moreira"},{id:"239897",title:"Ms.",name:"Juliana Semiramis",surname:"Menzinger",slug:"juliana-semiramis-menzinger",fullName:"Juliana Semiramis Menzinger"},{id:"239898",title:"Mr.",name:"Caio Vinícius Colozzo",surname:"Grilo",slug:"caio-vinicius-colozzo-grilo",fullName:"Caio Vinícius Colozzo Grilo"},{id:"239899",title:"Dr.",name:"Marinez",surname:"Cargnin Stieler",slug:"marinez-cargnin-stieler",fullName:"Marinez Cargnin Stieler"}],corrections:null}],productType:{id:"1",title:"Edited Volume",chapterContentType:"chapter",authoredCaption:"Edited by"},subseries:null,tags:null},relatedBooks:[{type:"book",id:"6318",title:"Emerging Microwave Technologies in Industrial, Agricultural, Medical and Food Processing",subtitle:null,isOpenForSubmission:!1,hash:"67de575df6dcd16554dd8f575e8c8368",slug:"emerging-microwave-technologies-in-industrial-agricultural-medical-and-food-processing",bookSignature:"Kok Yeow You",coverURL:"https://cdn.intechopen.com/books/images_new/6318.jpg",editedByType:"Edited by",editors:[{id:"188673",title:"Dr.",name:"Kok Yeow",surname:"You",slug:"kok-yeow-you",fullName:"Kok Yeow You"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"6362",title:"Electric Field",subtitle:null,isOpenForSubmission:!1,hash:"70b535bf877d17b46ddd1678574792a0",slug:"electric-field",bookSignature:"Mohsen Sheikholeslami Kandelousi",coverURL:"https://cdn.intechopen.com/books/images_new/6362.jpg",editedByType:"Edited by",editors:[{id:"185811",title:"Dr.",name:"Mohsen",surname:"Sheikholeslami Kandelousi",slug:"mohsen-sheikholeslami-kandelousi",fullName:"Mohsen Sheikholeslami Kandelousi"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"6603",title:"Actuators",subtitle:null,isOpenForSubmission:!1,hash:"33056f58590b5920dd938eff4810e8dc",slug:"actuators",bookSignature:"Constantin Volosencu",coverURL:"https://cdn.intechopen.com/books/images_new/6603.jpg",editedByType:"Edited by",editors:[{id:"1063",title:"Prof.",name:"Constantin",surname:"Volosencu",slug:"constantin-volosencu",fullName:"Constantin Volosencu"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"7210",title:"New Trends in High Voltage Engineering",subtitle:null,isOpenForSubmission:!1,hash:"a6e25d2b75bbeb9b7e4719aa5d90e58c",slug:"new-trends-in-high-voltage-engineering",bookSignature:"Reza Shariatinasab",coverURL:"https://cdn.intechopen.com/books/images_new/7210.jpg",editedByType:"Edited by",editors:[{id:"110072",title:"Prof.",name:"Reza",surname:"Shariatinasab",slug:"reza-shariatinasab",fullName:"Reza Shariatinasab"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"9290",title:"Applied Electromechanical Devices and Machines for Electric Mobility Solutions",subtitle:null,isOpenForSubmission:!1,hash:"2e50c2d9cf3922f5f8fff01aaef1053e",slug:"applied-electromechanical-devices-and-machines-for-electric-mobility-solutions",bookSignature:"Adel El-Shahat and Mircea Ruba",coverURL:"https://cdn.intechopen.com/books/images_new/9290.jpg",editedByType:"Edited by",editors:[{id:"193331",title:"Dr.",name:"Adel",surname:"El-Shahat",slug:"adel-el-shahat",fullName:"Adel El-Shahat"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"1591",title:"Infrared Spectroscopy",subtitle:"Materials Science, Engineering and Technology",isOpenForSubmission:!1,hash:"99b4b7b71a8caeb693ed762b40b017f4",slug:"infrared-spectroscopy-materials-science-engineering-and-technology",bookSignature:"Theophile Theophanides",coverURL:"https://cdn.intechopen.com/books/images_new/1591.jpg",editedByType:"Edited by",editors:[{id:"37194",title:"Dr.",name:"Theophile",surname:"Theophanides",slug:"theophile-theophanides",fullName:"Theophile Theophanides"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"3161",title:"Frontiers in Guided Wave Optics and Optoelectronics",subtitle:null,isOpenForSubmission:!1,hash:"deb44e9c99f82bbce1083abea743146c",slug:"frontiers-in-guided-wave-optics-and-optoelectronics",bookSignature:"Bishnu Pal",coverURL:"https://cdn.intechopen.com/books/images_new/3161.jpg",editedByType:"Edited by",editors:[{id:"4782",title:"Prof.",name:"Bishnu",surname:"Pal",slug:"bishnu-pal",fullName:"Bishnu Pal"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"3092",title:"Anopheles mosquitoes",subtitle:"New insights into malaria vectors",isOpenForSubmission:!1,hash:"c9e622485316d5e296288bf24d2b0d64",slug:"anopheles-mosquitoes-new-insights-into-malaria-vectors",bookSignature:"Sylvie Manguin",coverURL:"https://cdn.intechopen.com/books/images_new/3092.jpg",editedByType:"Edited by",editors:[{id:"50017",title:"Prof.",name:"Sylvie",surname:"Manguin",slug:"sylvie-manguin",fullName:"Sylvie Manguin"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"371",title:"Abiotic Stress in Plants",subtitle:"Mechanisms and Adaptations",isOpenForSubmission:!1,hash:"588466f487e307619849d72389178a74",slug:"abiotic-stress-in-plants-mechanisms-and-adaptations",bookSignature:"Arun Shanker and B. Venkateswarlu",coverURL:"https://cdn.intechopen.com/books/images_new/371.jpg",editedByType:"Edited by",editors:[{id:"58592",title:"Dr.",name:"Arun",surname:"Shanker",slug:"arun-shanker",fullName:"Arun Shanker"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"72",title:"Ionic Liquids",subtitle:"Theory, Properties, New Approaches",isOpenForSubmission:!1,hash:"d94ffa3cfa10505e3b1d676d46fcd3f5",slug:"ionic-liquids-theory-properties-new-approaches",bookSignature:"Alexander Kokorin",coverURL:"https://cdn.intechopen.com/books/images_new/72.jpg",editedByType:"Edited by",editors:[{id:"19816",title:"Prof.",name:"Alexander",surname:"Kokorin",slug:"alexander-kokorin",fullName:"Alexander Kokorin"}],equalEditorOne:null,equalEditorTwo:null,equalEditorThree:null,productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}}],ofsBooks:[]},correction:{item:{id:"79244",slug:"corrigendum-to-vascular-repair-and-remodeling-a-review",title:"Corrigendum to: Vascular Repair and Remodeling: A Review",doi:null,correctionPDFUrl:"https://cdn.intechopen.com/pdfs/79244.pdf",downloadPdfUrl:"/chapter/pdf-download/79244",previewPdfUrl:"/chapter/pdf-preview/79244",totalDownloads:null,totalCrossrefCites:null,bibtexUrl:"/chapter/bibtex/79244",risUrl:"/chapter/ris/79244",chapter:{id:"54438",slug:"vascular-repair-and-remodeling-a-review",signatures:"Nicolás F. Renna, Rodrigo Garcia, Jesica Ramirez and Roberto M.\nMiatello",dateSubmitted:"May 26th 2016",dateReviewed:"January 16th 2017",datePrePublished:null,datePublished:"April 5th 2017",book:{id:"5682",title:"Physiologic and Pathologic Angiogenesis",subtitle:"Signaling Mechanisms and Targeted Therapy",fullTitle:"Physiologic and Pathologic Angiogenesis - Signaling Mechanisms and Targeted Therapy",slug:"physiologic-and-pathologic-angiogenesis-signaling-mechanisms-and-targeted-therapy",publishedDate:"April 5th 2017",bookSignature:"Dan Simionescu and Agneta Simionescu",coverURL:"https://cdn.intechopen.com/books/images_new/5682.jpg",licenceType:"CC BY 3.0",editedByType:"Edited by",editors:[{id:"66196",title:"Dr.",name:"Dan",middleName:"T.",surname:"Simionescu",slug:"dan-simionescu",fullName:"Dan Simionescu"}],productType:{id:"1",title:"Edited Volume",chapterContentType:"chapter",authoredCaption:"Edited by"}},authors:[{id:"192616",title:"Dr.",name:"Nicolás",middleName:null,surname:"Renna",fullName:"Nicolás Renna",slug:"nicolas-renna",email:"nicolasfede@gmail.com",position:null,institution:{name:"National University of Cuyo",institutionURL:null,country:{name:"Argentina"}}},{id:"202536",title:"Dr.",name:"Rodrigo",middleName:"Damián",surname:"García",fullName:"Rodrigo García",slug:"rodrigo-garcia",email:"rodridg@hotmail.com",position:null,institution:null},{id:"202537",title:"Dr.",name:"Jesica",middleName:null,surname:"Ramirez",fullName:"Jesica Ramirez",slug:"jesica-ramirez",email:"jesicamagali@hotmail.com",position:null,institution:null},{id:"202539",title:"Dr.",name:"Roberto M.",middleName:null,surname:"Miatello",fullName:"Roberto M. Miatello",slug:"roberto-m.-miatello",email:"rmmiatello@gmail.com",position:null,institution:null}]}},chapter:{id:"54438",slug:"vascular-repair-and-remodeling-a-review",signatures:"Nicolás F. Renna, Rodrigo Garcia, Jesica Ramirez and Roberto M.\nMiatello",dateSubmitted:"May 26th 2016",dateReviewed:"January 16th 2017",datePrePublished:null,datePublished:"April 5th 2017",book:{id:"5682",title:"Physiologic and Pathologic Angiogenesis",subtitle:"Signaling Mechanisms and Targeted Therapy",fullTitle:"Physiologic and Pathologic Angiogenesis - Signaling Mechanisms and Targeted Therapy",slug:"physiologic-and-pathologic-angiogenesis-signaling-mechanisms-and-targeted-therapy",publishedDate:"April 5th 2017",bookSignature:"Dan Simionescu and Agneta Simionescu",coverURL:"https://cdn.intechopen.com/books/images_new/5682.jpg",licenceType:"CC BY 3.0",editedByType:"Edited by",editors:[{id:"66196",title:"Dr.",name:"Dan",middleName:"T.",surname:"Simionescu",slug:"dan-simionescu",fullName:"Dan Simionescu"}],productType:{id:"1",title:"Edited Volume",chapterContentType:"chapter",authoredCaption:"Edited by"}},authors:[{id:"192616",title:"Dr.",name:"Nicolás",middleName:null,surname:"Renna",fullName:"Nicolás Renna",slug:"nicolas-renna",email:"nicolasfede@gmail.com",position:null,institution:{name:"National University of Cuyo",institutionURL:null,country:{name:"Argentina"}}},{id:"202536",title:"Dr.",name:"Rodrigo",middleName:"Damián",surname:"García",fullName:"Rodrigo García",slug:"rodrigo-garcia",email:"rodridg@hotmail.com",position:null,institution:null},{id:"202537",title:"Dr.",name:"Jesica",middleName:null,surname:"Ramirez",fullName:"Jesica Ramirez",slug:"jesica-ramirez",email:"jesicamagali@hotmail.com",position:null,institution:null},{id:"202539",title:"Dr.",name:"Roberto M.",middleName:null,surname:"Miatello",fullName:"Roberto M. Miatello",slug:"roberto-m.-miatello",email:"rmmiatello@gmail.com",position:null,institution:null}]},book:{id:"5682",title:"Physiologic and Pathologic Angiogenesis",subtitle:"Signaling Mechanisms and Targeted Therapy",fullTitle:"Physiologic and Pathologic Angiogenesis - Signaling Mechanisms and Targeted Therapy",slug:"physiologic-and-pathologic-angiogenesis-signaling-mechanisms-and-targeted-therapy",publishedDate:"April 5th 2017",bookSignature:"Dan Simionescu and Agneta Simionescu",coverURL:"https://cdn.intechopen.com/books/images_new/5682.jpg",licenceType:"CC BY 3.0",editedByType:"Edited by",editors:[{id:"66196",title:"Dr.",name:"Dan",middleName:"T.",surname:"Simionescu",slug:"dan-simionescu",fullName:"Dan Simionescu"}],productType:{id:"1",title:"Edited Volume",chapterContentType:"chapter",authoredCaption:"Edited by"}}},ofsBook:{item:{type:"book",id:"8621",leadTitle:null,title:"Synchotron Radiation",subtitle:null,reviewType:"peer-reviewed",abstract:"
\r\n\tHydroxyapatite
",isbn:null,printIsbn:null,pdfIsbn:null,doi:null,price:0,priceEur:0,priceUsd:0,slug:null,numberOfPages:0,isOpenForSubmission:!1,isSalesforceBook:!1,hash:"c78cef62eb36d6440937ac6cac0b0bb3",bookSignature:"",publishedDate:null,coverURL:"//cdnintech.com/web/frontend/www/assets/cover.jpg",keywords:null,numberOfDownloads:null,numberOfWosCitations:0,numberOfCrossrefCitations:0,numberOfDimensionsCitations:null,numberOfTotalCitations:null,isAvailableForWebshopOrdering:!0,dateEndFirstStepPublish:"June 1st 2018",dateEndSecondStepPublish:"June 22nd 2018",dateEndThirdStepPublish:"August 21st 2018",dateEndFourthStepPublish:"November 9th 2018",dateEndFifthStepPublish:"January 8th 2019",remainingDaysToSecondStep:"4 years",secondStepPassed:!0,currentStepOfPublishingProcess:1,editedByType:null,kuFlag:!1,biosketch:null,coeditorOneBiosketch:null,coeditorTwoBiosketch:null,coeditorThreeBiosketch:null,coeditorFourBiosketch:null,coeditorFiveBiosketch:null,editors:null,coeditorOne:null,coeditorTwo:null,coeditorThree:null,coeditorFour:null,coeditorFive:null,topics:[{id:"20",title:"Physics",slug:"physics"}],chapters:null,productType:{id:"1",title:"Edited Volume",chapterContentType:"chapter",authoredCaption:"Edited by"},personalPublishingAssistant:null},relatedBooks:[{type:"book",id:"8356",title:"Metastable, Spintronics Materials and Mechanics of Deformable Bodies",subtitle:"Recent Progress",isOpenForSubmission:!1,hash:"1550f1986ce9bcc0db87d407a8b47078",slug:"solid-state-physics-metastable-spintronics-materials-and-mechanics-of-deformable-bodies-recent-progress",bookSignature:"Subbarayan Sivasankaran, Pramoda Kumar Nayak and Ezgi Günay",coverURL:"https://cdn.intechopen.com/books/images_new/8356.jpg",editedByType:"Edited by",editors:[{id:"190989",title:"Dr.",name:"Subbarayan",surname:"Sivasankaran",slug:"subbarayan-sivasankaran",fullName:"Subbarayan Sivasankaran"}],productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"1591",title:"Infrared Spectroscopy",subtitle:"Materials Science, Engineering and Technology",isOpenForSubmission:!1,hash:"99b4b7b71a8caeb693ed762b40b017f4",slug:"infrared-spectroscopy-materials-science-engineering-and-technology",bookSignature:"Theophile Theophanides",coverURL:"https://cdn.intechopen.com/books/images_new/1591.jpg",editedByType:"Edited by",editors:[{id:"37194",title:"Dr.",name:"Theophile",surname:"Theophanides",slug:"theophile-theophanides",fullName:"Theophile Theophanides"}],productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"3161",title:"Frontiers in Guided Wave Optics and Optoelectronics",subtitle:null,isOpenForSubmission:!1,hash:"deb44e9c99f82bbce1083abea743146c",slug:"frontiers-in-guided-wave-optics-and-optoelectronics",bookSignature:"Bishnu Pal",coverURL:"https://cdn.intechopen.com/books/images_new/3161.jpg",editedByType:"Edited by",editors:[{id:"4782",title:"Prof.",name:"Bishnu",surname:"Pal",slug:"bishnu-pal",fullName:"Bishnu Pal"}],productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"371",title:"Abiotic Stress in Plants",subtitle:"Mechanisms and Adaptations",isOpenForSubmission:!1,hash:"588466f487e307619849d72389178a74",slug:"abiotic-stress-in-plants-mechanisms-and-adaptations",bookSignature:"Arun Shanker and B. Venkateswarlu",coverURL:"https://cdn.intechopen.com/books/images_new/371.jpg",editedByType:"Edited by",editors:[{id:"58592",title:"Dr.",name:"Arun",surname:"Shanker",slug:"arun-shanker",fullName:"Arun Shanker"}],productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"3092",title:"Anopheles mosquitoes",subtitle:"New insights into malaria vectors",isOpenForSubmission:!1,hash:"c9e622485316d5e296288bf24d2b0d64",slug:"anopheles-mosquitoes-new-insights-into-malaria-vectors",bookSignature:"Sylvie Manguin",coverURL:"https://cdn.intechopen.com/books/images_new/3092.jpg",editedByType:"Edited by",editors:[{id:"50017",title:"Prof.",name:"Sylvie",surname:"Manguin",slug:"sylvie-manguin",fullName:"Sylvie Manguin"}],productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"72",title:"Ionic Liquids",subtitle:"Theory, Properties, New Approaches",isOpenForSubmission:!1,hash:"d94ffa3cfa10505e3b1d676d46fcd3f5",slug:"ionic-liquids-theory-properties-new-approaches",bookSignature:"Alexander Kokorin",coverURL:"https://cdn.intechopen.com/books/images_new/72.jpg",editedByType:"Edited by",editors:[{id:"19816",title:"Prof.",name:"Alexander",surname:"Kokorin",slug:"alexander-kokorin",fullName:"Alexander Kokorin"}],productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"2270",title:"Fourier Transform",subtitle:"Materials Analysis",isOpenForSubmission:!1,hash:"5e094b066da527193e878e160b4772af",slug:"fourier-transform-materials-analysis",bookSignature:"Salih Mohammed Salih",coverURL:"https://cdn.intechopen.com/books/images_new/2270.jpg",editedByType:"Edited by",editors:[{id:"111691",title:"Dr.Ing.",name:"Salih",surname:"Salih",slug:"salih-salih",fullName:"Salih Salih"}],productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"117",title:"Artificial Neural Networks",subtitle:"Methodological Advances and Biomedical Applications",isOpenForSubmission:!1,hash:null,slug:"artificial-neural-networks-methodological-advances-and-biomedical-applications",bookSignature:"Kenji Suzuki",coverURL:"https://cdn.intechopen.com/books/images_new/117.jpg",editedByType:"Edited by",editors:[{id:"3095",title:"Prof.",name:"Kenji",surname:"Suzuki",slug:"kenji-suzuki",fullName:"Kenji Suzuki"}],productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"3828",title:"Application of Nanotechnology in Drug Delivery",subtitle:null,isOpenForSubmission:!1,hash:"51a27e7adbfafcfedb6e9683f209cba4",slug:"application-of-nanotechnology-in-drug-delivery",bookSignature:"Ali Demir Sezer",coverURL:"https://cdn.intechopen.com/books/images_new/3828.jpg",editedByType:"Edited by",editors:[{id:"62389",title:"PhD.",name:"Ali Demir",surname:"Sezer",slug:"ali-demir-sezer",fullName:"Ali Demir Sezer"}],productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"872",title:"Organic Pollutants Ten Years After the Stockholm Convention",subtitle:"Environmental and Analytical Update",isOpenForSubmission:!1,hash:"f01dc7077e1d23f3d8f5454985cafa0a",slug:"organic-pollutants-ten-years-after-the-stockholm-convention-environmental-and-analytical-update",bookSignature:"Tomasz Puzyn and Aleksandra Mostrag-Szlichtyng",coverURL:"https://cdn.intechopen.com/books/images_new/872.jpg",editedByType:"Edited by",editors:[{id:"84887",title:"Dr.",name:"Tomasz",surname:"Puzyn",slug:"tomasz-puzyn",fullName:"Tomasz Puzyn"}],productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}}]},chapter:{item:{type:"chapter",id:"64860",title:"Modeling of Fluid-Solid Two-Phase Geophysical Flows",doi:"10.5772/intechopen.81449",slug:"modeling-of-fluid-solid-two-phase-geophysical-flows",body:'\nFluid-solid two-phase flows are important in many geophysical problems such as sediment erosion, transport and deposition in rivers or coastal environment, debris flows, scour at river or marine structures, and submarine landslides. Behaviors of fluid-solid two-phase flows are very different from those of liquid-gas two-phase flows where bubbles are dispersed in the liquid or droplets dispersed in the gas. Vast numbers of experiments on various scales have been carried out for different applications of fluid-solid two-phase flows; these experiments have advanced our understanding of bulk behaviors of some important flow characteristics. However, development of measurement techniques suitable for collecting data that contribute to understanding important physics involved in fluid-solid two-phase flows is a still-evolving science. With the modern computer technology, many data that are not obtainable currently in the experiment can be easily produced by performing time-dependent, multidimensional numerical simulations. Of course, empirical closure models required to close the governing equations still need high-quality experimental data for model validation.
\nNumerical approaches to two-phase flows include Eulerian-Eulerian approach, direct numerical simulations (DNS) based on Eulerian-Lagrangian formulations (Lagrangian point-particle approach), and fully resolved DNS approach [1]. Fully resolved DNS can resolve all important scales of the fluid and particles, but these simulations are currently limited to about 10 k uniform-size spheres on a Cray XE6 with 2048 cores [2], and it is not practical to use this method to model large-scale geophysical flow problems in the foreseeable future [1]. Lagrangian point-particle approach uses Eulerian formulation for the fluid phase and Lagrangian formulation for tracking the instantaneous positions of the particles. Lagrangian point-particle simulations make use of semiempirical relationships to provide both hydrodynamic force and torque acting on each particle and thus avoid modeling processes on scales smaller than Kolmogorov scale [1], making it possible to include more particles and run in a domain larger than that for fully resolved DNS. The application of Lagrangian point-particle approach is crucially dependent on the availability and accuracy of such semiempirical relationships. A recent study shows that good results can be obtained for about 100k uniform-size spherical particles in a vertical channel flow [3]; however, using this approach to investigate large-scale two-phase flow problems is still beyond the current computing capacity. Two-phase Eulerian-Eulerian approach treats both the fluid and particle phases as continuum media and is suitable for solving large-scale two-phase flow problems.
\nEulerian-Eulerian two-phase flow models based on large-eddy-simulations solve a separate set of equations describing conservation of mass, momentum, and kinetic energy for each phase [4, 5, 6, 7] and thus have the potential to consider all important processes involved in the interactions between the two phases through parameterization of particle-scale processes. This chapter introduces the basics of Eulerian-Eulerian two-phase flow modeling, its implementation in the finite-volume framework of OpenFOAM®, and two applications in geophysical flow problems.
\nLet us consider a mixture of fluid and solid particles. Fluid can be gas, water, or a mixture of water and gas. In DNS and Lagrangian point-particle approaches to two-phase flows, the flow field is solved by solving the Navier-Stokes equations, and the motion of each particle is determined by the Newton’s equation of motion. In Eulerian-Eulerian two-phase flow approaches, however, the motions of individual particles are not of the interest, and the focus is on the macroscopic motion of the fluid and solid particles instead. For this purpose, the solid particles are modeled as a continuum mass through an ensemble averaging operation, which is based on the existence of possible equivalent realizations. After taking ensemble average, the mixture of fluid and particles consists of two continuous phases: the fluid (water, gas, or a mixture of water and gas) is the fluid phase, and the solid particle is the solid phase. Both phases are incompressible. The motions of the fluid and solid phases are governed by their own equations, which are obtained by taking ensemble average of the microscopic governing equations for each phase [8]. Even though some aspects of fluid-solid interaction can be considered through the ensemble average, the ensemble averaging operation itself, however, does not explicitly introduce any turbulent dispersion in the resulting equations. To consider the turbulent dispersion in the Eulerian-Eulerian description of the fluid-solid two-phase flows, another averaging operation (usually a Favre average) is needed to consider the correlations of turbulent components [5, 9].
\nAt the microscopic scale, the fluid-solid mixture is a discrete system. The purpose of performing an ensemble averaging operation is to derive a set of equations describing this discrete system as a continuous system at the macroscopic scale, where the typical length scale should be much larger than one particle diameter.
\nIn the Eulerian-Eulerian approach to two-phase flows, it is assumed that the equations governing the motion of phase \n
and
\nwhere \n
where \n
Because the fluid phase and the solid phase are immiscible, at any time \n
The volumetric concentration of phase \n
There are several methods to derive the ensemble averaged equations governing the motion of phase \n
where \n
The ensemble averaged equations governing the motion of phase \n
and
\nThe resulting equations governing the ensemble average motion of phase \n
and
\nwith
\nNote that \n
which is the density of the interfacial force [8]. Physically, \n
After using Eq. (3) for \n
and
\nwhere \n
and \n
For compressible materials \n
Now we examine the limiting case where the fluid-solid system is at its static state. Because the phase functions for the two phases satisfy \n
for the fluid phase, and
\nfor the solid phase.
\nBecause \n
which, physically, is the buoyancy acting on the solid phase. Now Eq. (18) becomes
\nwhich states that the weight of the solid particles is supported by the buoyancy and the interparticle forces. Therefore, the ensemble pressure of the solid phase can be written as \n
For brevity of the presentation, we shall denote simply \n
and
\nThe ensemble averaged equations governing the motion of the solid phase are
\nand
\nwhere \n
To close the equations for the fluid and solid phases, closure models are needed for \n
It is remarked here that the definitions of the ensemble averages given in Eq. (14) do not consider the contribution from the correlations between the fluctuations of the velocities and the fluctuations of phase functions at microscopic scale; therefore, the effects of turbulent dispersion are not directly included in the ensemble averaged equations describing the motion of the each phase. In the literature, two approaches have been used to consider the turbulent dispersion: (i) considering the correlation between the fluctuations of \n
In the absence of the turbulent dispersion from \n
This expression for \n
where \n
The volumetric concentration and the velocities can be written as
\nwhere the Favre averages are defined as
\nand the overline stands for an integration with respect to time over a time scale longer than small-scale turbulent fluctuations but shorter than the variation of the mean flow field.
\nThe averaged equations for the mean flow fields of the two phases are obtained by taking the following steps: (i) substituting Eq. (25) with Eq. (26) in Eqs. (22) and (24), (ii) substituting Eq. (27) in the equations obtained at step (i), and (iii) taking average of the equations obtained at step (ii) to obtain the following equations:
\nfor the fluid phase, with \n
and
\nfor the solid phase, with \n
It is remarked here that the terms \n
In order to close these averaged equations, closure models are required for the following terms: \n
where \n
For brevity of the presentation, the symbols representing Favre averages are dropped hereinafter, and the final equations governing the conservation of mass and momentum of each phase are
\nfor the fluid phase and
\nfor the solid phase.
\nThe stress tensor for the fluid phase \n
The viscous stress tensor \n
where \n
The stress tensor \n
where \n
with \n
The equations governing \n
and
\nwhere coefficients \n
where \n
with \n
It is remarked here that the presence of solid particles in the turbulent flow may either enhance (for large particles) or reduce (for small particles) the turbulence [18]. The \n
The closure models for \n
where \n
For solid particles in a compact bed, the formula proposed by Hsu et al. [19] can be used to compute \n
where \n
The closure models for \n
The kinematic viscosity of the solid phase \n
where \n
Based on an analysis of heavy and small particles in homogeneous steady turbulent flows, Hinze [20] suggests that \n
and
\nwhere the coefficient \n
For dense fluid-solid two-phase flows, the visco-plastic rheological characteristics depend on a dimensionless parameter \n
Following the work of Boyer et al. [22], Lee et al. [16] assumed
\nwhere \n
where \n
which considers the solid phase in its static state as a very viscous fluid and
\nwhere \n
The drag force between the two phases is modeled through the particle response time \n
The first model is based on particle sedimentation in still water, which can be simplified as a one-dimensional problem, where the steady sedimentation assures that there are no stresses in both the solid and fluid phases in the vertical direction \n
and
\nwhere \n
Because net volume flux through any horizontal plane must be zero, we have
\nCombining Eqs. (59) and (61) yields
\nSubstituting Eqs. (61) and (62) into Eq. (60) leads to
\nwhere the solid-phase velocity \n
where the coefficient \n
The terminal velocity of a single particle \n
where \n
where \n
It is remarked that Eq. (64) is validated only for \n
Another model for particle response time can be derived by examining the pressure drop in the steady flow through a porous media. For a one-dimensional problem of a horizontal, steady flow through porous media, the terms containing the stresses of the fluid phase disappear, and Eq. (38) reduces to
\nwhere the horizontal coordinate \n
For this problem, Forchheimer [29] suggested
\nwhere \n
Comparing Eqs. (69) and (70) and using Eq.(71) give
\nwhere \n
For flow in a porous media, the particle response time can also be related to its permeability \n
where \n
When the flow is very slow, Eqs. (70), (71), and (73) suggest that
\nwhich means that the particle response time can be related to the permeability.
\nEquation (64) is validated only for \n
where \n
Combining Eqs. (63), (76), and (66)–(67) gives
\nWe stress that \n
where \n
For given values of \n
This section introduces how to use OpenFOAM® to solve the governing equations with the closure models presented in the previous section. OpenFOAM® is a C++ toolbox developed based on the finite-volume method; it allows CFD code developers to sidestep the discretization of derivative terms on unstructured grids.
\nTo avoid numerical noises occurring when \n
and
\nThe solutions of Eqs. (80) and (81) are expressed in the following semidiscretized forms:
\nwhere \n
If Eq. (83) is directly used to calculate \n
which is corrected by the following corrector
\nThis predictor-corrector scheme can improve the numerical stability by introducing a numerical diffusion term. To see this, we combine Eqs. (39) and (85) to obtain the following equation describing the evolution of \n
The right-hand side of Eq. (86) now has a diffusive term introduced by the numerical scheme. High sediment concentration and large \n
For the velocity-pressure coupling, Eq. (82) is similarly solved using a predictor \n
which is corrected by the following corrector
\nSubstituting Eq. (88) into Eq. (37) gives a pressure equation. However, when using this pressure equation to simulate air-water flows, numerical experiments have shown that the lighter material is poorly conserved [36]. The poor conservation of lighter material can be avoided by combining Eqs. (37) and (39) into the following Eq. (37):
\nand using Eq. (89) to correct \n
and combine Eqs. (83) and (88)–(90) to obtain the following equation
\nThe numerical diffusion term on the right-hand side of Eq. (91) can help improve the numerical stability.
\nThe prediction-correction method presented here deals with velocity-pressure coupling and avoids the numerical instability caused by high concentration. The turbulence closure \n
When \n
An iteration procedure is needed to solve the governing equations at each time step for the values of \n
Compute \n
Solve Eq. (86) for \n
Compute \n
Compute \n
Compute \n
Solve Eq. (91) for \n
Repeat Eqs. (5)–(7) for \n
Compute \n
Set \n
Repeat Eqs. (1)–(10) with the updated \n
Solve Eqs. (45) and (46) for \n
Figure 1 is a flowchart showing these 12 solution steps.
\nA flow chart showing the solution procedure using OpenFOAM®.
In the absence of the solid phase, the numerical scheme outlined here reduces to the “PIMPLE” scheme, which is a combination of the “pressure implicit with splitting of operator” (PISO) scheme and the “semi-implicit method for pressure-linked equations” (SIMPLE) scheme. Iterations need to be done separately to solve Eq. (80) for \n
To ensure the stability of the overall numerical scheme, the Courant-Friedrichs-Lewy (CFL) condition must be satisfied for each cell. The local Courant number for each cell, which is related to the ratio between the distance of a particle moving within \n
where in \n
This section briefly describes two examples that have been studied using the two-phase flow models described. The problem descriptions and numerical setups for these two problems are included here; for other relevant information, the reader is referred to Lee and Huang [35] and Lee et al. [38].
\nA sluice gate is a hydraulic structure used to control the flow in a water channel. Sluice gate structures usually have a rigid floor followed by an erodible bed. The scour downstream of a sluice gate is caused by the horizontal submerged water jet issuing from the sluice gate. It is of practical importance to understand the maximum scour depth for the safety of a sluice gate structure. Many experimental studies have been done to investigate the maximum scour depth and the evolution of scour profile (e.g., Chatterjee et al. [39]). For numerical simulations, this problem includes water (fluid phase) and sediment (solid phase) and is best modeled by a liquid-solid two-phase flow approach. In the following, the numerical setup and main conclusions used in Lee et al. [38] are briefly described. The experimental setup of Chatterjee et al. [39] is shown in Figure 2. To numerically simulate the experiment of [8], we use the same sand and dimensions to set up the numerical simulations: quartz sand with \n
A sketch of the experimental setup for scour induced by a submerged water jet.
Comparison of the computed scour depth with measurements of Chatterjee et al. [
The problem involves also an air-water surface, which can be tracked using a modified volume-of-fluid method introduced in [38]. A nonuniform mesh is used in the two-phase flow simulation because of the air-water interface, the interfacial momentum transfer at the bed, and the large velocity variation due to the water jet. The finest mesh with a vertical mesh resolution of \n
The scour process is sensitive to the model for particle response time used in the simulation. Because Eq. (72) can provide a better prediction of sediment transport rate for small values of Shields parameter, it is recommended for this problem. The two-phase flow model can reproduce well the measured scour depth and the location of sand dune downstream of the scour hole.
\nAnother application of the fluid-solid two-phase flow simulation is the simulation of the collapse of a deeply submerged granular column. The problem is best described as a granular flow problem, which involves sediment (a solid phase) and water (fluid phase). Many experimental studies have been reported in the literature on this topic. This section describes a numerical simulation using the fluid-solid two-phase flow model described in this chapter.
\nFigure 4 shows the experimental setup of Rondon et al. [40]. A 1:1 scale two-phase flow simulation was performed by Lee and Huang [35] using the fluid-solid two-phase flow model presented in this chapter. The diameter and the density of the sand grain are 0.225 mm and 2500 kg/m3, respectively. The density and the dynamic viscosity of the liquid are 1010 kg/m3 and 12 mPa s, respectively. Note that the viscosity of the liquid in the experiment is ten times larger than that for water at room temperature. For this problem, using a mesh of 1.0 × 1.0 mm and the particle response model given by Eq. (78), the fluid-solid two-phase flow model presented in this chapter can reproduce well the collapse process reported in Rondon et al. [40]. Figure 5 shows the simulated collapsing processes compared with the measurement for two initial packing conditions: initially loosely packed condition and initially densely packed condition.
\nA sketch of the experimental setup for the collapse of a deeply submerged granular column.
The simulated collapsing processes for the initially loose condition (a)–(d) and the initially dense condition (e)–(h). The lines represent contours of the computed concentrations, and the symbols were experimental data of Rondon et al. [
The two-phase model and closure models presented in this chapter are able to deal with both initially loose packing and initially dense packing conditions and reveal the roles played by the contractancy inside the granular column with a loose packing and dilatancy inside a granular column with a dense packing. One of the conclusions of Lee and Huang [35] is that the collapse process of a densely packed granular column is more sensitive to the model used for particle response time than that of a loosely packed granular column. The particle response model given by Eq. (78) performs better than other models; this is possibly because the liquid used in Rondon et al. [40] is much viscous than water.
\nThis chapter presented a brief introduction to the equations and closure models suitable for fluid-solid two-phase flow problems such as sediment transport, submarine landslides, and scour at hydraulic structures. Two averaging operations were performed to derive the governing equations so that the turbulent dispersion, important for geophysical flow problems, can be considered. A new model for the rheological characteristics of sediment phase was used when computing the stresses of the solid phase. The \n
This material presented here is partially based upon work supported by the National Science Foundation under Grant No. 1706938 and the Ministry of Science and Technology, Taiwan [MOST 107-2221-E-032-018-MY3]. Any opinions, findings, and conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the National Science Foundation.
\nNanomaterials (NMs) are the structures fabricated in the nanoscale, i.e. 1 to 100 nm and having at least one dimension in the nanoscale. The fabrication, study, and application of nanostructures are known as nanotechnology. The exhibition of novel physicochemical properties by the nanoscale materials has provided a unique opportunity for researchers to design and develop materials with applications in the diverse fields of science and technology. This has attracted attention towards nanoparticles (NPs) and their fabrication as compared to other sectors of NMs. Some of the nanomaterial productions have reached to the industrial scale due to the high demand for NMs in consumer products and their number is increasing at the moment with their developing applications. Ever-increasing demand for different NPs has generated the need for easy, safe, efficient, rapid, and eco-friendly procedures for their large-scale production.
Nanomaterials can be produced by two general approaches, i.e. top-down approach and bottom-up approach. Another classification includes different methods like physical, chemical, biological, and hybrid methods of nanoparticle production. The physical method requires an expensive setup, is high energy-consuming, and hazardous to health and the environment. Whereas chemical methods are highly efficient as compared to physical methods, but involve a toxic reducing agent, solvent, and stabilizing/capping agents. Recently, the biological method of nanoparticle production has attracted attention because of its ease, eco-friendly nature, high efficiency, and high yield. In this method, a biological agent or a biomolecule plays a significant role in the production of NMs [1]. Production of NMs by a biological method is a promising alternative for physical and chemical methods [2].
Among the different biological systems like bacteria, actinomycetes, fungi, plants, protozoa, and animals, fungi have shown great potential for the production of NPs on large scale. Bacteria normally produced NPs intracellularly, where large-scale production and purification of NPs is complicated and expensive. Unlike bacteria, fungi produce NPs extracellularly and are easy to use and purify NPs for large-scale production [3]. Fungi are easy to handle, versatile, tolerant, and economical biological systems for industrial production of biotechnology products and have been used extensively in large-scale production of different metabolites. The tremendous ability of fungi in the secretion of proteins up to 100 g/L, metabolic diversity, and high production capacity have made them a unique option for industrial biotechnology for decades. Hence, filamentous fungi are the first choice, since they are capable of secreting a large amount of proteins and other metabolites extracellularly. Moreover, the fabrication of NPs by a fungal system is a green process [4]. Among the fungal sources,
Industrial biotechnology processes demonstrate a significant reduction of greenhouse gas emissions using renewable resources. The process is environment friendly and do not result in the accumulation of toxic compounds in the ecosystem. In industrial biotechnology, biomass input is used under the process of biological agents like metabolites and biomolecules to create a wide spectrum of products. There is a worldwide interest to enable the production of different NPs on biotechnological lines because of their eco-friendly nature, less energy-intensive, ease of execution, and ability to modify biological agents, and products [10].
In the present chapter, we are going to focus on the need for large-scale productions of NPs by biological methods in general and by
More than 6400 different biologically active substances have been reported from filamentous fungi which have potential bioactivities and different applications [11]. As these fungi have greater tolerance to high metal ion concentration and have the ability to internalize and bio accumulate metal ions they can be used for metal ion reduction and stabilization in nanomaterial synthesis [12, 13, 14, 15, 16]. A huge range of fungi is shown to have the ability to synthesize NPs. Out of which
Nanomaterial synthesized | Reference | |
---|---|---|
Silver | [18] | |
Silver | [19] | |
Silver | [20] | |
Silver | [21] | |
Silver | [22] | |
Silver | [23] | |
Silver | [24] | |
Silver | [25, 26] | |
Silver | [27, 28] | |
Silver | [14, 15] | |
Silver | [29] | |
Silver | [30] | |
Silver | [31, 32] | |
Silver | [33] | |
Silver | [34] | |
Silver | [35] | |
Silver | [36] | |
Silver | [37] | |
Silver | [17] | |
Silver | [38] | |
Silver | [39] | |
Silver | [40] | |
Silver | [41] | |
Silver | [42] | |
Silver | [43] | |
Silver | [44] | |
Silver and Gold | [45] | |
Gold | [46] | |
Gold | [47] | |
Gold | [48] | |
Gold | [49] | |
Gold | [50] | |
Gold | [51] | |
TiO2 | [52] | |
TiO2 | [53] | |
ZnO | [54] | |
ZnO | [55, 56] | |
FeCl3 | [57] | |
Ca3P2O8 | [58] | |
Hg | [59] | |
CuO | [60] | |
CuO | [60] | |
Fennell AUMC 13012 | CuO | [60] |
CuO | [60] | |
CuO | [60] | |
CuO | [60] |
Various
The cell-free extracts of
All these various types of NPs synthesized using different isolates and strains of
The green chemistry approach highlights the usage of microorganisms which offers a cheaper, lighter, reliable, nontoxic, and eco-friendly process [68, 69]. Fungi secrete a higher amount of proteins owing to significantly higher productivity of NPs [70] which effectively proved a potential source for the extracellular synthesis of different NPs without using harmful toxic chemicals. The advantages made fungi more suitable for large-scale production and easy downstream processing, also economic [70, 71]. Besides, enzyme nitrate reductase is found to be responsible for the synthesis of NPs in fungi [68, 69]. Biofabrication of NPs using fungi (eukaryotic organism) has several advantages over the prokaryotic mediated approach for reproducibility of nanosized materials. Also include ease to multiplication, grow, handling, and rest of downstream process for this top-down approach of nanobiosynthesis through nano factories [72, 73]. Tarafdar et al., [74] observed rapid, low cost, and eco-friendly iron nanoparticle fabrication by using the fungi
Zielonka et al., [75] demonstrated fungi are almost ideal biocatalysts for NPs biosynthesis. In contrast to bacteria, as they are well-known for producing greater amounts of biologically active substances that make the fungus more appropriate for large-scale production [31, 32]. Moreover, fungal biomass can resist flow pressure, agitation, and harsh conditions in chambers such as bioreactors. Also, they exude extracellular reductive proteins which can be used in subsequent process steps. However, the fungal cell is deprived of unessential cellular components since NPs are accelerated outside the cell and can be immediately used in manifold ways without pre-treatment [76]. There are a large number of fungi, which can efficiently synthesize silver NPs, such as
Here we highlighted the advantages of NMs produced by using
Advantages of nanoparticles produced by
AgNPs released silver ions in the fungal cell, which increased its antifungal function. AgNPs synthesized by using
El-Desouky et al., [79] demonstrated the synthesis AgNPs by an eco-friendly and low-cost method using the fungi
It is well-identified that biological systems can fabricate the number of metallic and non-metallic nanoparticles. Synthesis of nanoparticles can be achieved at low cost by biological system especially from the fungal system at low pH, temperature, and salt concentration. Various studies have been proved that fungus-like
Even though, various studies have been initiated to understand the mechanism for the synthesis of nanoparticles from
Possible mechanism for the biosynthesis of Co3O4 nanoparticles in
The numerous NMs have been synthesized by
Graphical representation of different applications of NMs synthesized using
NMs synthesized by
In recent years, the nanotechnological advances in the field of agriculture have been increasing as the application of various NMs in the development of nano-based products like nanofertilizers for increasing crop yield and soil improvement, for plant growth promotion, nanopesticides, nanofungicides, nanoencapsulation for slow release of agrochemicals, and more in which NMs plays a vital role. The application of NPs as agrochemicals has become more common as technological advances make their production more economical for employment in the agriculture sector. For the potential application of NPs in plant disease control primarily included the information about the antimicrobial activity of different nano-size compounds against phytopathogens and the development of better application strategies to enhance the efficacy of disease suppression [100]. The antimicrobial activity of
Nanoformulations of copper-chitosan (Cu/Ch) has been prepared as an antifungal agent against
The application of NMs in the food security and animal industry is attending the great interest of the scientific community in recent years. Food security is usually the preparation, treatment, and storage of food products in which the food-borne pathogens or illness will not going to cause any damage or spoilage to the product [96, 97, 111]. Food insecurity, like illegal additives, pathogens, pesticide residues, allergens, and other unsafe factors, those are not only seriously affects human health, but also limit the rapid development of food industries to a certain extent [112, 113, 114]. The identification and quantitative analysis of bacteria is a very important and crucial issue in food safety. Conventional practices require long culture time, highly skilled operators, or specific recognition elements of each type of bacteria [113]. For this purpose, the analytical methods or equipments that meet the requirement of modern detection of various hazardous substances present in the foods for example packaging materials, sensors, and food containers coated with NPs are develop using NMs. The novel nano-based food packaging materials have the unique characteristics involving oxygen scavengers, antimicrobial potential, and barriers to gas or moisture, and many other. In view of these multiple benefits of nanopackaging, its application in the pathogens detection, antimicrobials, allergens and contaminants, UV-protecting activity, high gas barrier plastics, etc. are some important areas of research [115]. The use of such NMs in food packaging enhances the shelf life of food devoid of undesirable alteration in its quality.
The application of smart packaging systems has increased tremendously in animal industries the muscle-based food products such as meat, chicken, etc. that are prone to contamination. The packaging of meat and muscle products suppress the spoilage, enhance the tenderness by allowing enzymatic activity, avoid contamination, retain the cherry red color in red meats and reduce the loss in its weight [116]. Plastic food packaging is one of the most important areas of research that employ nanotechnology to make stronger and lighter packaging materials and also enhances its performance. Besides this, NMs with strong antimicrobial properties such as Ag and TiO2 NPs could be used in the packaging of foods to prevent spoilage [117]. Additionally, the application of NPs of clay in food packaging helps to control the entry of carbon dioxide, oxygen, and moisture towards food materials, thus preventing food spoilage.
Nowadays, more researchers have been paying attention to the development of nanosensors, which are being added in plastic packaging to spot the gases released from spoiled food. In the food spoilage or contamination condition, the packaging material will alert the consumer by detecting toxins, microbial contamination, and pesticides in food products, based on flavor production and color changing [118]. Moreover, plastic films entrenched with silicate NPs are being developed to maintain food fresh for a longer period. In this case, NPs play a vital role in dropping the oxygen flow and also facilitate to impede the moisture seeping out from the package. In animal industries,
In medicine and pharmacy, NMs have been successfully applied due to their high surface area that is able to adsorbed or conjugate with an extensive variety of therapeutic and diagnostic agents such as drugs, vaccines, genes, antibodies, and biosensors. In recent years, antibiotic resistance is an emerging major global health problem and novel antimicrobial formulations are essentially needed to fight against these drug-resistant microbes, therefore nano-based medicine as antimicrobial agents have gained considerable attention in the field of microbial drug resistance [119, 120]. Hence, the NPs synthesized by Mousa et al., [119] using the endophytic fungus
There are several reports on the synthesis and antimicrobial applications of
NMs offer a unique platform for the purification of water contaminated with pollutants namely organics, metal ions, biological contaminants, and arsenic from the water because of the high surface area of nanosorbents and their ability of chemical modification as well as easier regeneration [127, 128, 129, 130]. Chatterjee et al., [91] reported the synthesis of superparamagnetic iron oxide NPs (IONPs) (Fe3O4) of 20-40 nm size by manglicolous (mangrove) fungus
In another study, the Au NPs was synthesized by
Other than this, nowadays NMs could be applied in antimicrobial surface coatings, environmental sensing, renewable energy, and many other environmental applications.
Assessment of toxicity of synthesized NPs is the critical step for ensuring their safe and sustainable applications. Hence, toxicity evaluation of all the newly synthesized nanoparticle must be considered before their industrial applications. As far as the comparison of biosynthesized NPs with NMs synthesized by other methods especially the chemical method is concerned, the biosynthesized NPs seems to be biocompatible [133]. For instance, the green synthesized NPs were found to enhance the plant seedling growth, yield and quality, suggesting the biocompatibility of biosynthesized NPs as compared to the chemical synthesis NPs [134]. In cont