Chemical composition of corn leaf.
\r\n\tThis book intends to provide the reader with a comprehensive overview of the current state-of-the-art on Theileriosis, Babesiosis, and Anaplasmosis, both in humans and domestic animals. Particularly this book aims to permit the researchers to enter into a critical focus on the biology of the parasites, eco-epidemiology of the diseases, clinical manifestations, risk factors, immunology, surveillance, diagnosis, identification, and management of risks as well as the potential economic impact on animal production.
",isbn:"978-1-80356-384-8",printIsbn:"978-1-80356-383-1",pdfIsbn:"978-1-80356-385-5",doi:null,price:0,priceEur:0,priceUsd:0,slug:null,numberOfPages:0,isOpenForSubmission:!0,isSalesforceBook:!1,hash:"3d72ae651ee2a04b2368bf798a3183ca",bookSignature:"Prof. Elisa Pieragostini",publishedDate:null,coverURL:"https://cdn.intechopen.com/books/images_new/11577.jpg",keywords:"Zoonosis, Global Climate Change, Epidemiology, Risk Factors, Haemoparasites, Prevention & Control, Piroplasmosis, Anaplasmosis, Babesiosis, Theileriosis, Tick-Borne Diseases, Ticks",numberOfDownloads:null,numberOfWosCitations:0,numberOfCrossrefCitations:null,numberOfDimensionsCitations:null,numberOfTotalCitations:null,isAvailableForWebshopOrdering:!0,dateEndFirstStepPublish:"February 23rd 2022",dateEndSecondStepPublish:"April 29th 2022",dateEndThirdStepPublish:"June 28th 2022",dateEndFourthStepPublish:"September 16th 2022",dateEndFifthStepPublish:"November 15th 2022",remainingDaysToSecondStep:"21 days",secondStepPassed:!0,currentStepOfPublishingProcess:3,editedByType:null,kuFlag:!1,biosketch:"Professor of Animal genetics and breeding at Bari University, a researcher in animal genetics related to the resilience of Apulian livestock to enzootic tick-borne haemoparasites and to the involved functional effect of hemoglobin variants. She is a member of national and international scientific associations.",coeditorOneBiosketch:null,coeditorTwoBiosketch:null,coeditorThreeBiosketch:null,coeditorFourBiosketch:null,coeditorFiveBiosketch:null,editors:[{id:"51521",title:"Prof.",name:"Elisa",middleName:null,surname:"Pieragostini",slug:"elisa-pieragostini",fullName:"Elisa Pieragostini",profilePictureURL:"https://mts.intechopen.com/storage/users/51521/images/system/51521.jpg",biography:"Dr. Pieragostini has a Degree in Biological Sciences, DPhil in Biochemistry received from Bologna University, Italy.\r\nShe was an Assistant professor of “Genetics” at the Faculty of Science of Bologna University, a Full professor of “Animal genetics and breeding” Bari University, Italy, and Elected President of course on “Agricultural Science and Technology” (2001-2010) Bari University.\r\nShe retired in 2015.\r\nFrom 1977 to 1984 she carried out intensive work on Drosophila investigating quantitative characters associated with biochemical markers. From the1985 onwards, she had been studying Apulian farm animals focusing on blood-based markers as well as on the structure-function relationship of the different hemoglobin variants come across and their relationship with the Apulian livestock resilience to the enzootic tick-borne diseases. \r\nShe was Project Director\r\nShe is a member of national and international scientific associations.",institutionString:"Independent Researcher",position:null,outsideEditionCount:0,totalCites:0,totalAuthoredChapters:"1",totalChapterViews:"0",totalEditedBooks:"0",institution:{name:"University of Bari Aldo Moro",institutionURL:null,country:{name:"Italy"}}}],coeditorOne:null,coeditorTwo:null,coeditorThree:null,coeditorFour:null,coeditorFive:null,topics:[{id:"16",title:"Medicine",slug:"medicine"}],chapters:null,productType:{id:"1",title:"Edited Volume",chapterContentType:"chapter",authoredCaption:"Edited by"},personalPublishingAssistant:{id:"280415",firstName:"Josip",lastName:"Knapic",middleName:null,title:"Mr.",imageUrl:"https://mts.intechopen.com/storage/users/280415/images/8050_n.jpg",email:"josip@intechopen.com",biography:"As an Author Service Manager my responsibilities include monitoring and facilitating all publishing activities for authors and editors. From chapter submission and review, to approval and revision, copy-editing and design, until final publication, I work closely with authors and editors to ensure a simple and easy publishing process. I maintain constant and effective communication with authors, editors and reviewers, which allows for a level of personal support that enables contributors to fully commit and concentrate on the chapters they are writing, editing, or reviewing. I assist authors in the preparation of their full chapter submissions and track important deadlines and ensure they are met. I help to coordinate internal processes such as linguistic review, and monitor the technical aspects of the process. As an ASM I am also involved in the acquisition of editors. 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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:"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:"314",title:"Regenerative Medicine and Tissue Engineering",subtitle:"Cells and Biomaterials",isOpenForSubmission:!1,hash:"bb67e80e480c86bb8315458012d65686",slug:"regenerative-medicine-and-tissue-engineering-cells-and-biomaterials",bookSignature:"Daniel Eberli",coverURL:"https://cdn.intechopen.com/books/images_new/314.jpg",editedByType:"Edited by",editors:[{id:"6495",title:"Dr.",name:"Daniel",surname:"Eberli",slug:"daniel-eberli",fullName:"Daniel Eberli"}],productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"57",title:"Physics and Applications of Graphene",subtitle:"Experiments",isOpenForSubmission:!1,hash:"0e6622a71cf4f02f45bfdd5691e1189a",slug:"physics-and-applications-of-graphene-experiments",bookSignature:"Sergey Mikhailov",coverURL:"https://cdn.intechopen.com/books/images_new/57.jpg",editedByType:"Edited by",editors:[{id:"16042",title:"Dr.",name:"Sergey",surname:"Mikhailov",slug:"sergey-mikhailov",fullName:"Sergey Mikhailov"}],productType:{id:"1",chapterContentType:"chapter",authoredCaption:"Edited by"}},{type:"book",id:"1373",title:"Ionic Liquids",subtitle:"Applications and Perspectives",isOpenForSubmission:!1,hash:"5e9ae5ae9167cde4b344e499a792c41c",slug:"ionic-liquids-applications-and-perspectives",bookSignature:"Alexander Kokorin",coverURL:"https://cdn.intechopen.com/books/images_new/1373.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"}}]},chapter:{item:{type:"chapter",id:"79700",title:"Functional Application for the Corn Leaf Fibre to Make Reinforced Polymer Composites Sheet",doi:"10.5772/intechopen.101656",slug:"functional-application-for-the-corn-leaf-fibre-to-make-reinforced-polymer-composites-sheet",body:'Nowadays, most developed countries are paying special attention to environmental issues, and some of the most important actions to protect the environment are focused on the optimum use of natural resource, the reduction of air pollution, loss of soil moisture, upgrading industrial and agroforestry wastes, etc. [1, 2, 3]. All these are with main aim of reducing and utilizing agricultural waste, which may be profitable, pollution free and economically viable for the farmer and industries. The most suitable way is to solve environmental related issues and increase the income of farmers [4, 5, 6]. Corn leaf fibre is nowadays exploited as reinforcements material owing to their low cost, fairly good mechanical properties, high specific strength, availability, eco-friendly and biodegradability characteristics Application of high-performance composites using natural fibres is increasing in various engineering fields. This not only reduces the cost but also saves from environmental pollution [7, 8, 9, 10]. These composites are also used in panel for partition and false ceiling, wall sheet, floor, window and door frame. The mainly fibre-reinforced composite is handled to have material properties in all directions and material properties are different in all performances with control of the fibre orientation [11, 12, 13, 14].
The corn leaf agricultural waste material was collected from local corn farm. The chemical constituent of corn leaves was found to be cellulose of 43%, lignin of 22%, hemicelluloses of 31% and Ash of 1.9% (Figure 1).
Corn leaf.
The corn leaves are cut into 5 to 6 cm length and 1 kg dried leaves are placed in the cooking pot. Make a solution of sodium hydroxide and soda AQ, pour the solution in the pot with leaves and boil for 2 to 3 hour After that, it will become pulp and we will wait for it to cool down and wash it with water three or four times, and then, we will blend with the help of blending machine and squeeze them the help of cotton fabric (Table 1) [15, 16].
S. No | Properties | Range (%) |
---|---|---|
1. | Cellulose | 43 |
2. | Lignin | 22 |
3. | Hemicelluloses | 31 |
4. | Ash | 1.9 |
Chemical composition of corn leaf.
The polyester resin with hardener is mixed in a container and then continuously stirred for 2 to 5 minutes. Then, corn leaf fibre was added with continuous stirring and uniform mixture. Afterwards, this prepared liquid material is placed on the mould, and after 3 hour, mould is removed as composite sheet. This final composite sheet is properly placed in contact with sunlight for 5 to 7 days (Figure 2).
(a) Resin and hardener. (b) Mould.
There are severe environmental problems such as air pollution, smoke formation and loss of soil moisture. The main aim to choose corn leaf is utilization of agricultural waste that may be profitably pollution free and economically viable for the farmer (Figure 3 and Table 2).
All natural fibre images.
S. No | Thickness(mm) | Pulp ratio (%) | Epoxy (%) | Hardener (%) |
---|---|---|---|---|
1. | 4 | 35 | 50 | 15 |
2. | 4 | 45 | 40 | 15 |
3. | 4 | 55 | 30 | 15 |
4. | 8 | 35 | 50 | 15 |
5. | 8 | 45 | 40 | 15 |
6. | 8 | 55 | 30 | 15 |
Specimen composition.
Thickness measurement instruments are used as per standard performance ASTM D-1777.
Tensile measurement instrument is used as per ASTMD–-638 standards. This instrument is of very good quality and has properly accurate measurement material sheet with tensile result and easily operating system (Figures 4 and 5, Table 3).
Tensile strength testing instrument.
Tensile specimen shape.
Sr.no. | Symbol | Description | Dimension (mm) |
---|---|---|---|
1. | I0 | Gauge length | 145 |
2. | I1 | Grip distance | 160 |
3. | I2 | Overall length | 240 |
4. | b | Width of narrow parallel portion | 15 |
5. | b1 | Width ends | 30 |
6. | T | Thickness | 4, 8 |
Tensile specimen dimensions.
The specimen was exposed to a large amount of power for a small intermission of stage. A measurable with more impact energy will have more roughness. This impact measurement instrument is used for as per ASTMD-256 standards (Figures 6 and 7; Tables 4–6).
Impact strength testing instruments.
Impact specimen of IZOD shape.
Sr. no. | Description | Dimension (mm) |
---|---|---|
1. | Length of specimen | 63.5 |
2. | Centring of notch | 2.54 |
3. | Radius of notch type V | 0.25 |
4. | Angle of notch | 45′ |
5. | Width | 12.70 |
6. | Thickness | 4, 8 |
Impact specimen dimensions.
Sr.no. | Pulp ratio (%) | Various thickness (mm) | Mean thickness (mm) |
---|---|---|---|
1. | 35 | 4.16, 4.22, 4.28, 4.26, 4.33, 4.48, 4.56, 4.87, 4.10, 4.21 | 4.347 |
2. | 45 | 4.33, 4.42, 4.37, 4.56, 4.68, 4.77, 4.87, 4.66, 5.02, 5.13 | 4.681 |
3. | 55 | 4.56, 4.68, 4.72, 4.26, 4.32, 4.37, 4.76, 5.12, 5.33, 5.22 | 4.734 |
4. | 35 | 7.66, 7.90, 7.88, 7.97, 8.10, 8.34, 8.44, 8.56, 8.69, 8.78 | 8.232 |
5. | 45 | 8.24, 8.33, 8.54, 8.56, 8.76, 8.87, 8.42, 8.19, 9.09, 9.18 | 9.681 |
6. | 55 | 8.16, 8.23, 8.36, 8.40, 8.27, 8.26, 8.41, 8.43, 8.53, 8.66 | 8.371 |
Sheet thickness results.
Sr.no. | Thickness(mm) | Pulp ratio (%) | Weight (gm) | GSM(g/m2) |
---|---|---|---|---|
1. | 4 | 35 | 142 | 142gm/0.03 = 4733 |
2. | 4 | 45 | 136 | 136gm/0.03 = 4533 |
3. | 4 | 55 | 124 | 124gm/0.03 = 4133 |
4. | 8 | 35 | 237 | 237gm/0.03 = 7900 |
5. | 8 | 45 | 223 | 223gm/0.03 = 7433 |
6. | 8 | 55 | 210 | 210gm/0.03 = 7000 |
Sample GSM.
Mechanical properties of corn leaf fibre and epoxy resin composites are explained here.
It can be observed from Table 7 and Figure 8 that with pulp ratio (35%) and thickness of 4 mm and 8 mm, density values are 1.183 g/m3 and 0.987 g/m3, respectively. Further, it is observed that at low pulp ratio (%), density (g/m3) for composite sheet materials is higher. With pulp ratio of 55% in composite sheet and for both thickness levels 4 mm and 8 mm, lower density is observed. Increase in pulp ratio % in sample results in decrease in density for composite material sheet. This may be due to the presence of some voids. It can be seen from the images that void is there between fibre and matrix, which shows less compatibility of corn leaf fibre with epoxy resin at higher pulp ratio (Figures 9–11).
Sr.no. | Thickness (mm) | Pulp ratio (%) | Density (g/m3) |
---|---|---|---|
1. | 4 | 35 | 142gm/120 = 1.1833 |
2. | 4 | 45 | 136gm/120 = 1.1333 |
3. | 4 | 55 | 124gm/120 = 1.0333 |
4. | 8 | 35 | 237gm/240 = 0.9875 |
5. | 8 | 45 | 223gm/240 = 0.9291 |
6. | 8 | 55 | 210gm/240 = 0.8750 |
Sample density.
Effect of the pulp ratio and thickness on density properties.
Image for composite sheet material.
Specimen size for composite sheet material.
Specimen break after tensile strength test for composite material.
Samples are tested on DAK series 7200 machine (a universal testing machine) and tensile strength is recorded. The values are depicted in Table 8.
Sr.no. | Pulp ratio (%) | Thickness (mm) | Tensile strength 1 (Mpa)ASTMD-638 | Tensile strength 2(Mpa)ASTMD-638 | Mean tensile strength |
---|---|---|---|---|---|
1. | 35 | 4 | 5.47 | 4.43 | 4.950 |
2. | 45 | 4 | 2.10 | 4.17 | 3.135 |
3. | 55 | 4 | 1.98 | 3.15 | 2.565 |
4. | 35 | 8 | 7.61 | 7.58 | 7.595 |
5. | 45 | 8 | 4.47 | 5.10 | 4.785 |
6. | 55 | 8 | 3.88 | 4.02 | 3.950 |
Tensile strength result.
It can be observed from Table 8 and Figure 12 that at pulp ratio of 35%, a thickness level of 4 mm and 8 mm gives the highest tensile strength value 4.95 Mpa and 7.58 Mpa, respectively. It may be due to the higher density for composite sheet according to Table 7. The maximum tensile strength obtained for corn leaf fibre ratio (35%) may also be due to good bonding between epoxy and fibre pulp ratio, and approximately hexagonal structure of cellulose present in the sugarcane leaves fibre gives high flexibility to the fibre. Further, higher tensile strength may be attributed to the more energy transfer to the fibres by the matrix [17, 18].
Effect of the pulp ratio and thickness on tensile properties.
With pulp ratio (55%) in composite sheet and for both 4 mm and 8 mm thickness, low tensile strength has been observed. It may be due to increase in pulp ratio % decreases density as reported earlier. The decrease in tensile strength with increase in pulp ratio (%) may be due to increase in voids created by air entrapment due to small-size particles. The tensile strength for neat epoxy is very less, which shows that there is decrease in strength in composite and less density that may be due to weak adhesion between fibre pulp and matrix, which causes no proper transfer of energy to the fibres by matrix.
In order to find the impact capability of sample, impact test is carried out using IZOD – CHARPY digital impact tester machine. Absorbed energy obtained for six different (samples) composite sheets from the IZOD – CHARPY machine has been shown in figure. It has been observed from Table 9 that maximum impact strength of 2.40 Kj/m2 is obtained for 55% pulp ratio sheet.
Sr.no. | Pulp ratio% | Thickness (mm) | Impact strength 1(kg. /m2)ASTMD-256 | Impact strength 2(kg. /m2) ASTMD-256 | Impact strength |
---|---|---|---|---|---|
1. | 35 | 4 | 1.77 | 1.35 | 1.11 |
2. | 45 | 4 | 1.25 | 1.49 | 1.55 |
3. | 55 | 4 | 1.22 | 1.37 | 1.79 |
4. | 35 | 8 | 2.39 | 2.10 | 1.89 |
5. | 45 | 8 | 1.35 | 1.67 | 1.99 |
6. | 55 | 8 | 2.43 | 1.72 | 2.40 |
Impact test results.
Further, pulp ratio of (55%) with 4 mm and 8 mm thickness has highest impact strength for 1.79 Kj/m2 and 2.4 Kj/m2 respectively. The impact strength of the composites increases with increase in fibre content (pulp ratio %). It may be due to during impact force, fibre pulls out and fibre breakage occurs at lower fibre loading of the polymer composites. At high fibre loading, the fibre crowding leads to easy debonding, which in turn increases the impact resistance, when compared with the impact energy of neat epoxy which is very less. It is observed that the impact strength increases.
Pulp ratio (35%) in composite sheet for both thickness levels of 4 and 8 mm, lower impact strength has been observed with decrease in pulp ratio % and epoxy resin concentration level. The optimum combination for the impact strength of the composites is pulp ratio of 55% and for both thickness levels as seen in Figures 13 and 14, respectively.
(a). Impact specimen (b). Broken specimen after impact strength testing.
Effect of the pulp ratio and thickness on impact strength properties.
Scanning electron microscope (SEM) is basically measurement the material surface by scanning through high wavelength beams with different wavelengths. The different composite materials are shown in SEM imageFigures 15–17.
FESEM image for pulp ratio and epoxy resin for composite sheet.
FESEM image for pulp ratio and epoxy resin for composite sheet.
FESEM image for pulp ratio and epoxy resin for composite sheet.
Field emission scanning electron microscope image for sugarcane leaf fibre pulp-reinforced composites is taken to understand microstructure. From the images, the fibre dispersion, matrix without fibres and fibre agglomeration are clearly visible. The images indicate that the failure is due to matrix failure, fibre pull-out and also due to the presence of some voids. The FESEM image of coir fibre-reinforced samples clearly shows the broken sugarcane leaf fibres. It is seen from the images that void is there between fibre and matrix, which shows less compatibility of corn leaf fibre with epoxy resin. Uniform mixing are pulp ratios and other particles leads to less air voids.
This study on the natural corn leaf fibre-reinforced epoxy composites uses pulp ratio (%), thickness level of 4 mm and 8 mm and constant hardness as filler material for the following conclusions: From the present work, it is concluded that the natural corn leaf fibre along with pulp ratio (%), thickness level of 4 mm and 8 mm and constant hardness can be successfully used with epoxy resin to prepare polymer matrix composites with good mechanical properties.
For composite sheet, it is found that pulp ratio is of 35% and thickness of 4 mm to highest tensile strength 4.95. According to figure, it is found that for pulp ratio of 35% and thickness of 8 mm to the highest tensile strength 7.59. It is observed that the maximum value of tensile strength is obtained for corn leaf fibre ratio (35%) composite sheet. Increasing pulp ration (%) and low density reduce tensile strength due to non-bonding of pulp particles with sugarcane leaf fibre.
It is found that pulp ratio is of 55% and thickness of 4 mm to highest impact strength for about 1.79. According to figure, it is found that pulp ratio of 55% and thickness of 8 mm give the highest impact strength 2.4. The impact strength of the composites increases with increase in fibre content (pulp ratio %), and this is because on the application of the impact force, fibre pulls out and fibre breakage occurs at lower fibre loading of the polymer composites. The pulp ratio (35%) in composite sheet and both levels of thickness have lower impact strength.
The FESEM image shows good bonding between fibre, pulp ration (%) and matrix. Also, breakage of fibres shows the load transferred from matrix to the fibres.
The use of natural sugarcane leaf fibres is to prepare eco-friendly composites. It is utilized as agricultural waste, which may be profitable, pollution free and economically viable for the farmer and industries. These composites are also used in panel for partition and false ceiling, wall sheet, floor, window and door frame.
In recent years, wireless communication systems have had a significant impact on the daily life of human beings, therefore nowadays more and more users are connecting their devices to existing networks causing a constant increase in data traffic and the need for high speed networks will continue to increase over the years [1, 2, 3]. To cope with this rise the new 5G communication systems would have to dramatically improve the communication capacity by exploiting enormous unlicensed bandwidth in particular, in the millimeter waveband. It should also be prepared to provide and support very high data rates which in turn therefore requires the design of antennas and amplifiers satisfying the expected data rate [4, 5, 6]. Research in 5G Millimeter Band wireless communication shows that as mobile industries developed to use the millimeter wave spectrum, carriers are likely to use the 28, 38 and 73GHz bands which will become available in future technologies [7]. The requirements imposed by 5G technology on the antennas are: lightweight antenna, low profile, low cost mass production, ease of installation, Despite its narrow band the microstrip patch antenna may prove to be an ideal candidate to meet these requirements and the design of a microwave amplifier becomes very interesting in view of the operation of 5G technology in millimeter band. This chapter proposes the design of a microstrip patch antenna and an amplifier for 5G application then a PA-Antenna Unit operating in the 28 GHz band. In the following lines we will respectively present the architecture of our Co-Design then the mathematical model of the antenna and the amplifier as well as their modeling then the interpretation and analysis of the results and finally the conclusion.
The principle of the Co-Design of a PA-Antenna block is based on the fact that the junction of the antenna and the amplifier must be done with as little loss as possible, which is why it is very objective for us to work on each one. Equipment with a reference impedance which will facilitate the junction of the two because the option of designing a matching network no longer becomes a necessity. So let us say the stages of Co-design illustrated in the figure below (Figure 1).
PA-antenna block Co-design principle.
In the chain of transmission of wireless communication systems, the proposed Co-Design Block is of capital importance because the amplifier will have the role of taking a weak signal as input and producing a high intensity signal at the output. This signal will be recovered at the output by the antenna and radiates by it in the free space.
In this section we will notify the different formulas used to obtain the dimensions of the rectangular patch:
where C is the speed and εr the dielectric constant of the substrate.
where the effective dielectric constant is expressed by the formula
Where h is the height of the dielectric substrate, the extension of length
The dimensions of the ground plane are expressed by the following formulas:
The feeding technique used for our antennas is the microstrip feeding technique because of its ease of manufacture and its better reliability according to [8].
The choice of the feeding technique chosen therefore imposes a choice of adaptation technique in our work we have chosen the insed feed adaptation technique. This technique involves inserting notches to bring the impedance of the antenna down to that of the power line [9]. Each notch is equivalent to a parallel admittance Y with a conductance G and a subceptance B. The following formulas on the conductance of a slot, the mutual conductance and the resistance of the antenna are expressed as follows
The mutual conductance is expressed as follows:
Where
After having developed all the theoretical analysis which allows us to find, using mathematical formulas, the various parameters important for the design of the antenna, we will now proceed to the modeling of the antenna.
The previous section allowed us to show how to obtain the different antenna dimensions of a rectangular patch antenna. Table 1 below illustrates these dimensions.
Dimension | Value (mm) |
---|---|
Wp | 4.23 |
Lp | 3.52 |
Wg | 11.84 |
Lg | 10.3 |
Wf | 0.3912 |
Lf | 1.95 |
Fi | 0.93 |
gap | 0.26 |
Antenna dimension.
When modeling the antenna several initiatives were taken first with the proposal of several antenna shapes departing from the known classical shape. The Figures 2 and 3 below represent the different forms of modeled antennas.
Rectangular patch modeled: a) with dimension, b) without dimension.
Proposed patch antenna shape.
The Other forms of antennas modeled in terms of contribution are illustrated below.
An Amplifier is an electronic device whose role is to increase the power of a signal introduced at its input. To simplify our study we will admit that our amplifier is a quadrupole whose matrix is [S] and connected to a voltage source E with an internal impedance and it is loaded by an impedance (Figure 4).
Distribution waves and reflection coefficients at the entry and exit of the quadrupole.
The matrix [S] of distribution of this linear quadrupole is such that [9]:
When making the amplifier, we try to have maximum gain. In other words, it is necessary to perform the adaptation at the input of the transistor and the source simultaneously with the adaptation between the transistor output and the load.
The transistor amplifier are very recurrent microwave amplifiers their characteristics depend on the properties of the Transistor for the design in our work we looked at the FET transistor sp_aiiAF035P1_00–19941209 manufactured by Alpha Industries so we will first illustrate the characteristics of our transistor namely the input and output reflection coefficients S11, S22 the transmission coefficient S21 which represents the transmission from the input to the output or the own gain of the transistor and of the future amplifier S12, represents the isolation or the reverse transmission from the output to the input the drain source voltage Vds = 5 V and the current Ids = 70 mA. We will therefore present and illustrate the S-parameters listed below in Figure 5.
Schematic of the transistor and simulation of S-parameters.
The S-parameters of the transistor obtained are as follows: S11 = −1.067 dB, S22 = −0.219 dB, S21 = −11.164 dB, S12 = − 35.289 dB. We realize that the inherent gain of the transistor is very low, it is imperative for us to improve this gain as well as the characteristics of the amplifier in order to produce an amplifier that meets the constraints imposed by 5G technology.
Considering K as the stability factor, the expression of the stability factor is given by the following formula:
and if
The Stability constant K of the transistor and mod_delta
The architecture of a Microwave Amplifier is shown as follows (Figure 6).
Microwave amplifier.
For the design of the amplifier, we will first start with impedance matching. The adaptation with Stub has been opted for by this document. The structure of the stub is shown in Figure 7 below.
Stub structure.
Figure 8 below shows the S-parameters of the Stub.
Stub S-parameters.
The validation of our Stub is confirmed by an impedance adaptation to 50 ohms at the input and at the output the table below summarizes the result obtained (Table 2).
Parameters | Value |
---|---|
S11 (dB) | −15.062 |
S22 (dB) | −15.062 |
S12 (dB) | −0.637 |
S21 (dB) | −0.637 |
Summary of the Sparameters of the stub.
The above table presents the results of synthesis of the S-parameters of the stub at the resonant frequency of the transistor. From these results, it can be seen that: S11 = S22, S12 = S21 Hence, the matching of the impedance is good, because the waves leaving the source and passing through the line are not partly reflected when they arrive on the load.
The design of the transistor amplifier is shown in the Figures 9 and 10 above.
Microwave amplifier without stage of transistor.
Microwave amplifier with stage of transistor.
The Antenna Parameters shown below are: Reflection Coefficient S11, Voltage Standing Wave Ratio (VSWR), Antenna Gain in (dB), and Antenna Input Impedance in Ohms The S11 reflection coefficient is the parameter demonstrating whether the antenna adaptation is good or not, the criterion for defining good adaptation through this parameter is S11 < −10 dB. The Figure 11 below illustrate the S11 parameter of the antennas.
Antennas parameter S11.
The Voltage Standing Wave Ratio (VSWR) is the parameter demonstrating if the adaptation of the antenna is good the characteristic value is VSWR ≤2 the Figure 12 illustrates the voltage standing wave ratio obtained by the antennas.
Stationary wave ratio of antennas.
The gain of the antenna characterizes the capacity of the antenna to radiate the maximum power that is ingested at its input. The Figure 13 illustrate the gain of antennas.
Antennas gain.
The input impedance of the antenna obviously shows whether we have suitably adapted the antenna or not, it is also clear that this is one of the conditions to be satisfied in order to be able to make our Co-Design Block PA-Antenna the Figure 14 below illustrates the impedance of our antennas.
Antenna input impedance.
In the summary of the Figures 2 and 3 presented above we have proposed 04 antenna shapes the first shape (Figure 2) is the classic rectangular patch template then the other shapes offered are patch templates excluding classic models (Figure 3). We can obviously note that the antennas have a good adaptation and an input impedance at 50 ohms but the gain proposed by these antennas are quite low because the strongest gain proposed here is 7.25 dB to improve these gains so we have model antenna arrays. An antenna array: is the combination of several antenna of the same type in order to form a single antenna the assembly of the different radiating elements must respect a certain distance between radiating element the standard pitch most used in most cases is not worth = 0.5λ for our work we will be interested in linear networks and we will model this one with 4 elements so the distance between will be worth 0.5λ Figure 15 below presents the modeling of the two antenna arrays the step of value 0.5 λ is 5.36 mm. The Figure 15 below illustrates the configuration of these antenna networks.
Linear antenna arrays modeled with different shape.
The reflection coefficients observed in each of the antenna networks below are illustrated in the Figure 16 below.
S11 reflection coefficient of antenna arrays.
Figure 17 shows the gains obtained by these different antennas network.
Gain of different antenna network.
We are now going to explore the gain of the antenna arrays in the E plane in order to observe the side lobes generated; the Figure 18 below illustrates it.
Representation of gain in plan E of antenna network.
To confirm the validity of our results, the representation of the impedances of the antenna networks are illustrated in Figure 19 below.
Input impedance of antenna networks.
It is clear that the impedance presented by our input antenna arrays is 50 ohms at the resonant frequency. We will summarize our work on Antennas in the table below (Table 3).
The results obtained must be compared with those which have already been the subject of research and accepted in the scientific research community (Table 4).
Antenna Parameters | Values | |
---|---|---|
S11 (dB) | −15.6 | Single antenna with different shape offered |
−13.05 | ||
−24.345 | ||
−23.277 | ||
−15.515 | Antenna has 4 elements with different proposed shape | |
−13.31 | ||
−11.066 | ||
Gain (dB) | 7.25 | Single antenna with different shape offered |
6.24 | ||
5.94 | ||
6 | ||
13 | Antenna has 4 elements with different proposed shape | |
11.7 | ||
12.16 | ||
Bandwidth(MHz) | 550 | Single antenna with different shape offered |
361.3 | ||
416 | ||
473.88 | ||
504.59 | Antenna has 4 elements with different proposed shape | |
344.91 | ||
360.66 | ||
Efficiency (%) | 76.82 | Single antenna with different shape offered |
64.313 | ||
71.9 | ||
72.15 | ||
75.3 | Antenna has 4 elements with different proposed shape | |
69.81 | ||
63.99 | ||
Impédance (ohms) | 50 ohms |
Summary of antenna parameters.
Ref | S11 (dB) | Gain (dB) | VSWR | Bandwidth(GHz) | Efficiency (%) |
---|---|---|---|---|---|
[10] | −15.35 | — | 1.79 | — | 87.8 |
[11] | −20.35 | 6.21 | 1.02 | 0.4 | 65.6 |
[12] | −17.34 | 6.72 | 1.28 | — | — |
[13] | −23.67 | 6.7 | — | 1.15 | 81.2 |
[14] | −39.37 | 6.37 | 1.022 | 2.48 | 86.73 |
[15] | −39.7 | 5.23 | — | 4.1 | — |
[16] | −14.151 | 6.06 | 1.488 | 0.8 | — |
[17] | −22.2 | 6.85 | 1.34 | — | — |
[18] | −27.7 | 6.72 | 1.22 | 0.463 | 75.875 |
Comparative analysis at the antenna level.
Comparing our works to those listed, it is clear that our obtained gain is greater than the proposed works, the bandwidth obtained is better compared to the works [11, 18]. The reflection coefficients obtained are better compared to works [16, 15] but the bandwidth obtained in these works is better than ours. We can therefore deduce from these works that our antennas comply with and meet the requirements imposed by 5G technology.
After modeling the amplifier, it is therefore important to observe the parameters obtained by the amplification after simulation. The S-parameters of the amplifier are summarized in Figure 20 below.
S-parameters of the amplifier without stage transistor.
The S-Parameters of the amplifier with stage transistor are shown in Figure 21 below.
S-parameters of amplifier with stage transistor.
As we notice in our figures above the amplifier presents 04 parameters namely S11, S22, S12, S21 the parameters S11, S22 respectively represent the reflection coefficients at the input and at the output of the amplifier and the parameter S12 represents isolation, the parameter S21 represents the amplifier transmission gain. The goal of making a transistor stage is therefore to improve the transmission gain of the amplifier. The Table 5 below illustrates the characteristics of the amplifier.
Co-Design Block PA-Antenna.
The following table establishes a comparison between our work and the work carried out by [19] (Table 6).
Amplifier Parameters | Values | |
---|---|---|
Amplifier without stages | Amplifier with stage | |
S11 (dB) | −30.784 | −29.645 |
S22 (dB) | −16.978 | −16.779 |
S12 (dB) | −16.445 | −32.941 |
S21 (dB) | 7.68 | 15.31 |
Impédance d’entrée ou de sortie | 50 ohms | |
Bandwidth (GHz) | Greater than 2GHz |
Summary of amplifier parameters.
Parameters | This Work | [19] |
---|---|---|
Frequency (GHz) | 28 | |
S11 (dB) | −13.124 | |
S22 (dB) | −15.455 | |
S12 (dB) | — | |
S21 (dB) | 10.803 | |
Application | 5G |
Comparative analysis at the amplifier level.
Our results obtained in simulation are much better than that obtained in [19]. Our amplifier has a gain of 15 dB which shows that our amplifier meets the requirements imposed by 5G technology.
The Co-Design Block PA-Antenna can be done with the greatest serenity because the impedances of the two equipment’s comply with the principles listed above. The figure below therefore illustrates the proposed PA-Antenna Co-Design (Figure 22).
Co-Design PA-Antenna Parameter S11.
The results obtained after simulation show us the following characteristics illustrated in the Figure 23 below.
The S11 parameter clearly shows us that our Co-Design is functional and well suited to the resonant frequency. In this chapter we enumerate a method of designing a transmitter block namely the antenna and the amplifier it is important to note that the design of the block requires the partial design of each of the transmitters in order to consider the design of the block. The design of the block takes into account the impedance adaptation parameters this as well as in this chapter we have arranged such that the amplifier and the antenna present at input as at output an impedance of 50 ohms thus facilitating the junction of the two block the proof Figure 23 illustrates clearly and clearly that the block is functioning correctly and the impedances of the various equipment are in conformity with the fixed reference impedance.
Having reached the end of this chapter, the objective of which is to propose a PA-Antenna Co-Design block for 5G applications, it is clear that the design of such a device requires fairly strict requirements and methodology. Therefore, we looked at the design on the one hand of the antenna and on the other hand of the amplifier by setting 50 ohms as the working impedance guaranteeing the adaptation of the impedance of the device. After design of the two equipment’s separately. We therefore proposed and simulated said device. This has characteristics that meet the requirements imposed by 5G technology, which should be noted that the antennas and amplifier proposed in this chapter offer very good characteristics compared to some existing equipment and presented in this chapter. It is also necessary to note the double resonance of our antenna in the 46.06 GHz band and presenting in this one an impedance of 50 ohms and a good bandwidth.
All my thanks go to my teachers at the National Polytechnic School of Douala Cameroon for their teachings and advice. My thanks go to the Intech-Open author community who will shed some light on this work to make it even better.
In this chapter, it is clear that we have only had the possibility of simulating our project with the reference software, namely CST microwave and ADS. In this declaration we ask the community to offer us the possibility of being able to design our project indeed we are engineers in Telecommunications and the means to develop such technologies in our country Cameroon is extremely difficult so it will be a huge pleasure for us to have the chance to be able to realize our project thanks to your help.
The Internet has irrevocably changed the dynamics of scholarly communication and publishing. Consequently, we find it necessary to indicate, unambiguously, our definition of what we consider to be a published scientific work.
",metaTitle:"Prior Publication Policy",metaDescription:"Prior Publication Policy",metaKeywords:null,canonicalURL:"/page/prior-publication-policy",contentRaw:'[{"type":"htmlEditorComponent","content":"A significant number of working papers, early drafts, and similar work in progress are openly shared online between members of the scientific community. It has become common to announce one’s own research on a personal website or a blog to gather comments and suggestions from other researchers. Such works and online postings are, indeed, published in the sense that they are made publicly available. However, this does not mean that if submitted for publication by IntechOpen they are not original works. We differentiate between reviewed and non-reviewed works when determining whether a work is original and has been published in a scholarly sense or not.
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\\n"}]'},components:[{type:"htmlEditorComponent",content:'A significant number of working papers, early drafts, and similar work in progress are openly shared online between members of the scientific community. It has become common to announce one’s own research on a personal website or a blog to gather comments and suggestions from other researchers. Such works and online postings are, indeed, published in the sense that they are made publicly available. However, this does not mean that if submitted for publication by IntechOpen they are not original works. We differentiate between reviewed and non-reviewed works when determining whether a work is original and has been published in a scholarly sense or not.
\n\nThe significance of Peer Review cannot be overstated when it comes to defining, in our terms, what constitutes a published scientific work. Peer Review is widely considered to be the cornerstone of modern publishing processes and the key value-adding contribution to a scholarly manuscript that a publisher can make.
\n\nOther than the issue of originality, research misconduct is another major issue that all publishers have to address. IntechOpen’s Retraction & Correction Policy and various publication ethics guidelines identify both redundant publication and (self)plagiarism to fall within the definition of research misconduct, thus constituting grounds for rejection or the issue of a Retraction if the work has already been published.
\n\nIn order to facilitate the tracking of a manuscript’s publishing history and its development from its earliest draft to the manuscript submitted, we encourage Authors to disclose any instances of a manuscript’s prior publication, whether it be through a conference presentation, a newspaper article, a working paper publicly available in a repository or a blog post.
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\n\nSome basic information about the editorial treatment of different varieties of prior publication is laid out below:
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\n\nGiven that conference papers and presentations generally pass through some sort of peer or editorial review, we consider them to be published in the accepted scholarly sense, particularly if they are published as a part of conference proceedings.
\n\nAll submitted manuscripts originating from a previously published conference paper must contain at least 50% of new original content to be accepted for review and considered for publication.
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\n\nAs with the conference papers and presentations, Authors should obtain any necessary permissions from the newspaper or magazine that published the work, and indicate that they have done so in a note to the External Editor.
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