\\n\\n
These books synthesize perspectives of renowned scientists from the world’s most prestigious institutions - from Fukushima Renewable Energy Institute in Japan to Stanford University in the United States, including Columbia University (US), University of Sidney (AU), University of Miami (USA), Cardiff University (UK), and many others.
\\n\\nThis collaboration embodied the true essence of Open Access by simplifying the approach to OA publishing for Academic editors and authors who contributed their research and allowed the new research to be made available free and open to anyone anywhere in the world.
\\n\\nTo celebrate the 50 books published, we have gathered them at one location - just one click away, so that you can easily browse the subjects of your interest, download the content directly, share it or read online.
\\n\\n\\n\\n\\n"}]',published:!0,mainMedia:null},components:[{type:"htmlEditorComponent",content:'
IntechOpen and Knowledge Unlatched formed a partnership to support researchers working in engineering sciences by enabling an easier approach to publishing Open Access content. Using the Knowledge Unlatched crowdfunding model to raise the publishing costs through libraries around the world, Open Access Publishing Fee (OAPF) was not required from the authors.
\n\nInitially, the partnership supported engineering research, but it soon grew to include physical and life sciences, attracting more researchers to the advantages of Open Access publishing.
\n\n\n\nThese books synthesize perspectives of renowned scientists from the world’s most prestigious institutions - from Fukushima Renewable Energy Institute in Japan to Stanford University in the United States, including Columbia University (US), University of Sidney (AU), University of Miami (USA), Cardiff University (UK), and many others.
\n\nThis collaboration embodied the true essence of Open Access by simplifying the approach to OA publishing for Academic editors and authors who contributed their research and allowed the new research to be made available free and open to anyone anywhere in the world.
\n\nTo celebrate the 50 books published, we have gathered them at one location - just one click away, so that you can easily browse the subjects of your interest, download the content directly, share it or read online.
\n\n\n\n\n'}],latestNews:[{slug:"webinar-introduction-to-open-science-wednesday-18-may-1-pm-cest-20220518",title:"Webinar: Introduction to Open Science | Wednesday 18 May, 1 PM CEST"},{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"}]},book:{item:{type:"book",id:"3565",leadTitle:null,fullTitle:"International Conference on Applied Life Sciences",title:"International Conference on Applied Life Sciences",subtitle:null,reviewType:"peer-reviewed",abstract:"The International Society for Applied Life Sciences (ISALS) is a worldwide Organization that aims to help scientists and researchers, publish recent findings in its scientific journals, and conferences as well as consultancy services it may provide. 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\r\n\tThe purpose of the book is to provide information on new scientific findings in space exploration and their application to other fields. Space exploration provides a fundamental source of knowledge that will improve our understanding of nature and its influence on our views. Its achievements will be directed to phenomena that require a proper explanation involving the analysis of data in studies of the solar system together with views on the origin of the universe and its evolution. The book should also contain aspects involved in the physical description of new phenomena and determine the manner in which they modify our present views and the techniques that we employ. Such contributions should also be accompanied by studies of their effects on human activity including the development of devices that will improve global communication. The importance of the book will be properly assessed by the value of its contributions.
\r\n\t
During the last decades, the plastic surgery field has made important advances in terms of clinical results and developing new surgical techniques, minimizing complications and reducing the mortality rates. On the other hand, the revolution of new technologies such as medical devices has opened other alternatives in the current clinical practice [1, 2].
\nThere is no secret about the popularity that plastic surgery procedures have gained even in women and men, as a part of a social‐aesthetic revolution that find better bodies and improve personal image. Since its introduction, liposuction has undergone several technical challenges and has improved the clinical outcomes [3, 4].
\nA wide range of technological advancements has been released to replace traditional methods of suctioning fat: ultrasound, power, laser, and radiofrequency. Each surgical alternative has its own benefits and complications. Different medical device companies across the world are continuously working on the safe surgical instruments for this type of surgical procedures [5]. The dreamed liposuction device has to be in the position to offer different functions at the same time: (1) remove excess of fat, (2) keep safe the surrounded soft tissue, (3) devices allowed to be used under local anesthesia, and (4) device results avoid bruising and swelling [6–8].
\nAn innovative and new technique is called High Definition LipoSculture. This is an advanced sculpting technique that creates an athletic and sculpted appearance. The objective of this procedure is to remove both superficial and deep fat that surrounds muscle groups in order to enhance the visibility of underlying toning and musculature. This technique could be applied in multiple body areas such as abdomen, chest, waist, back, buttocks, arms, flanks, and thighs [2, 4].
\nThe aim of this chapter is to review the principal concepts that involve this technique and describe its clinical application.
\nObesity, overweight, and metabolic syndrome are a public health issue nowadays. Countries such as the United States report an estimate of 40% of the adult population suffer from this health problem. This spectrum of diseases is associated with high rates of mortality in comparison with cancer, cardiovascular disease, and violent deaths [9, 10].
\nRecent clinical studies predict that in 2013, more than the 50% of the worldwide population would be facing this reality. Weight loss including strategies such as dietary changes and exercise usually does not achieve the desired weight loss goals. Based on this, bariatric and metabolic surgery has become the treatment of choice for obesity and morbid obesity [11].
\nThe Roux‐En‐Y gastric bypass still remains the gold standard surgical option for obese patients. In the course of achieving massive weight loss and resolution of comorbidities, bariatric surgery creates quality‐of‐life problems that are in the medical field of plastic surgeons. Despite the numerous health advantages of bariatric surgery, disgruntled patients complained of disturbing lax skin and subcutaneous tissue [5, 8, 12].
\nPlastic surgeons learned during the last years that change in body contour with repulsive hanging skin and bizarre rolls of skin and fat. Due to this, High Definition LipoSculture has been presented as a safe and effective option [13].
\nAn electronic literature review was conducted in order to find the most recent medical literature published in this field. Using the keywords such as plastic surgery, liposuction, body contouring, aesthetic medicine, and surgical procedure, the following databases were consulted: Pubmed, Lilacs, Proquest, Cochrane, Ovid, and Google Scholar. With the aim to maximize the number of articles, no date limit in the search was set, and manuscripts in English, Spanish, and Portuguese were considered.
\nInitially, 87 articles were obtained, of which 25 met the inclusion criteria. However, only 23 were referenced in the current work with a focus on high definition liposuction and body contouring or gave important theoretical contributions.
\nInitially, all the patients are exanimated and evaluated in plastic surgery consultation, and complete medical records are reviewed including previous surgical procedures, current medication use, and recent laboratory analysis. Considering that this type of surgical procedure is created to be a sculpting procedure rather than a debulking technique, an appropriate patients’ selection is necessary. A good muscle tone without an excessive amount of fat or skin laxity is expected (body mass index < 30) [3, 14].
\nOnce the physical examination is performed, lipodystrophy throughout the trunk has to be evaluated. Patients are requested to perform various muscle contractions in the clinical assessment to evaluate separately the muscle groups that contribute to the contour of the torso. Finally, skin laxity, elasticity, and quality of tissue are considered [15, 16].
\nFor male patients, there are other aspects to be included in the clinical assessment: the presence of gynecomastia, chest contour, and volume of fat in this area. In the female cases, a comparable estimate is performed: the buttocks, lumbosacral angle, fat disposition in the lateral thighs, and perigluteal area are considered [4, 7, 12].
\nThe physical examination is suggested to include documentation of scars, hernias, and other potential routine findings. Upon completion of the history and physical examination, based on our current clinical guidelines, patients are scheduled for an extra medical examination by the anesthesia department, to have the chance to evaluate other current medical issues ongoing at the same time. Once the patient meets the clinical requirements for this procedure, a final appointment is suggested to show a quick presentation explaining the surgical presentation in details, focused on benefits and potential complications. At the end of this medical visit, patients sign informed consent forms to continue with the medical process of surgery scheduling [17, 18].
\nPatients are requested to be in the ambulatory surgery service 2 h prior to the surgical time. A new medical assessment is conducted to review the general medical status of the patient on the surgery day. Recent laboratory test results, electrocardiograms, and thorax X‐rays are reviewed prior to authorizing the patient to be transferred to the operating room. Based on the patients’ medical conditions and preferences, epidural or general anesthesia is offered by the anesthesia team.
\nPreoperative strategies that involve medication such as thromboembolism prophylaxis included low‐weight heparin, intravenous corticosteroids, analgesics, and antibiotic prophylaxis are administrated with the main goal to keep the patient in the best condition possible and avoid potential clinical complications.
\nPerforming an abdominal ultrasonography, the abdominal muscle groups are evaluated. The median, paramedian, and lateral muscle layer planes in the iliac fossae and flanks are comparatively evaluated and demarcated, the boundaries of the rectus muscles, rectus fascia, especially in the supraumbilical region and the contour of the superior oblique with the superficial fascicule close to the iliac edge and correlated with anterior rectus on each side (Figure 1).
\nInitial ultrasound evaluation.
Once the patients arrive into the operating room, the first step is the surgical marking (Figure 2). This is performed with the patient initially in supine and in the upright standing position. It is essential to identify and understand the superficial anatomy and topography. Erroneous marking will lead to deformities and abnormal appearance and affects clinical outcomes [19].
\nPreoperative marking.
Preoperative marking.
The surface anatomy differs between men and women patients. In women, the transversal lines in the rectus abdominis muscle are not aesthetically desired. In men, the landmarks marked are the pectoralis major, serratus anterior, rectus abdominis, external oblique, iliac crest, and inguinal ligaments and the relationship between those structures. In women, the landmarks are the serratus anterior, rectus abdominis, external oblique, iliac crest, and inguinal ligaments. Other anatomical areas of care comprise the lateral and posterior torso (Figure 3) [19, 20].
\n\nUnder general or epidural anesthesia and previous asepsis and antisepsis, on sterile surgical fields, plastic surgeon initiates the procedure. Infiltration is performed with Klein solution, with tumescence technique. It starts with deep fat liposuction with power‐assisted liposuction (PAL). After obtaining the redundant fat tissue and achieve a uniform surface, ultrasound‐assisted liposuction (UAL) system is used following anatomical landmarks for 3–5 min per zone. Later, a lipoaspiration is performed with PAL system fat tissue surface along anatomical landmarks. Finally, a foam dressing is placed along the lines of the marking.
\nPatients are required for a hospital stay at least 48–72 h postoperatively. Pain control, prophylaxis antibiotic, and antiinflammatory medications are given in order to improve the patients’ comfort and avoid infections in the operative site. In some cases, open drains are placed both in female and male patients in the sacral area and inguinal area, respectively.
\nOther postoperative interventions are the use of mild‐compression garment, stockings to prevent deep vein thrombosis, and an abdominal band for 4 weeks. Supplementary care includes lymphatic drainage massages and adjunctive external ultrasound (1‐h session once a day for 10 days). Patients are scheduled for postoperatively follow‐up at 1, 15, 30, and 90 days, respectively. Alarm signs and general recommendations are given for all the patients in order to reduce postoperative complications. The duration of the cosmetic results will be associated with the patient care in terms of healthy life styles and adequate medical follow‐up. There is no accurate data describing failed procedures in the follow‐up period [21].
\nClinical results: pre‐ vs. postoperative.
There are limited clinical studies published in the current medical literature showing extensive series with appropriate and considerable follow‐up; however, the level of satisfaction in patients is surely high. In 2007, Dr. Hoyos published a study describing the experience in 306 patients using this surgical approach. In 306 subjects enrolled in the trial, 257 (84%) reported satisfactory results. In our clinical experience that include near to 80 patients, our level of patient satisfaction reached 90% (Figures 4 and 5) [3, 7, 12].
\nClinical results: pre‐ vs. postoperative.
As expected in any surgical procedure, based on its nature, patients are exposed to clinical risk, some related with the anesthesia and other associated directly with the surgical technique. In the first group, one could find abnormalities in the cardiac rhythm, obstruction of the airway, allergic reactions, and bronchoaspiration. In the second group, one could find bleedings, low blood pressure, blood clots, pulmonary embolism, deep vein thrombosis, damage in neurovascular structures, hypothermia, and burning with surgical instruments and medical devices [5, 7, 21].
\nResearchers and surgeon scientists devoted to improve the clinical outcomes in this surgical field are exploring new alternatives to develop new techniques and surgical approaches with minimal invasion. On the other hand, minimize tissue morbidity, decrease hospital stay and recovery time, and increase skin contraction/tightening are points to improve [22].
\nThese priorities have led the medical and technical industry to develop new devices focused on noninvasive body contouring and nonsurgical adipose reducing techniques. A new medical approach called “High‐Intensity Focused Ultrasound“(HIFU) is now available, which delivers high‐intensity ultrasonic energy to the deep subcutaneous tissue, producing heat capable of ablating adipose tissue and thermally modifying collagen. Cosmetic outcomes so far are very promising [23].
\nOther alternative that has been used by experts in this field is the cryolipolysis. This technique refers to use cold exposure to induce subcutaneous fat necrosis secondary to inflammatory reaction/cascade that affects the adipose tissue directly. Clinical studies have proven good clinical results in terms of reduction in the subcutaneous fat deposits and minimal complication rates [6, 7, 14].
\nFurthermore, radiofrequency devices are designed to use optical energies to treat directly the dermis and hypodermis. This technology allows to target principally the water located in the dermal layer; however, the target is controlled by thermal stress leading to dermal tightening and contraction. At the same time, in the same physical process, there is an activation of the dermal fibroblast to stimulate the new collagen formation. The utilization of bipolar radiofrequency in the hypodermis maximizes fat cell metabolism; devices such as BodyFxTM, Invasix use this type of principles [8, 17, 23].
\nHigh definition liposuction procedures should be considered revolutionary in the plastic surgery field. They are more complex, difficult, and need a special learning curve. The procedures require surgeons to understand how the anatomical configuration skin‐fat‐muscle‐skeletal structures help equally in the 3D superficial topography either in woman or in male human contouring. New technologies and novel medical devices coming up will lead in the future minimal scar procedures with better clinical outcomes.
\nVortices are common in fluid motion that originates due to the rotation of fluid elements. They occur widely and extensively in a broad range of physical systems from the earth’s surface to interstellar space. A few examples include spiral galaxies in the universe, red spots of Jupiter, tornadoes, hurricanes, airplane trailing vortices, swirling flows in turbines and in different industrial facilities, vortex rings formed by the firing of certain artillery or in the mushroom cloud resulting from a nuclear explosion. The physical quantity that characterizes the rotation of fluid elements is the vorticity ω = ∇ × u where u is the fluid velocity. Qualitatively, it can be said that in the region of vortex formation, the vorticity concentration is high compared with its surrounding fluid elements. Vortices formed behind obstacles to a fluid flow are also an interesting observation in various aspects of daily life. Study on the fluid flow around obstacles dates back to the fifteenth century when Leonardo da Vinci drew some sketches of vortex formation behind obstacles in flowing fluids. It has been an interesting and challenging problem in fluid mechanics and is of basic importance in several areas such as the study of aircraft designing, oceanography, atmospheric dynamics, engineering, human blood circulation. [1, 2, 3, 4]. Analyzing the behavior of flow around such obstacles also provides a medium to study the physical mechanism of transition from laminar to turbulent flow. If a stationary solid boundary lies in the path of a fluid flow, the fluid stops moving on that boundary. Thereby, a boundary layer is formed and its separation from the solid boundary generates various free shear layers that curl into concentrated vortices. These vortices then evolve, interact, become unstable and detach to turbulence. The dynamics of fluids is very diverse and the detail characteristics of transition to turbulence are quite complicated, which also differ from flow to flow. Such understandings can only be realized by experiments and computational models. However, there are a few unifying themes in the theory and a few routes to turbulence that are shared by many flows. One such theme is that when the Reynolds number (the parameter measuring the speed of a class of similar flows with steady configuration) increases, the temporal and spatial complexity of the flows increases eventually leading to turbulence. At a low Reynolds number, a pair of counter-rotating vortices forms behind the cylinder. As the Reynolds number increases, the vortices become unstable and gradually evolve into a von Karman vortex street [5, 6, 7, 8, 9]. The topic of flow past an obstacle is of utmost importance from the experimental point of view also. Its understanding is applicable in the stability of submerged structures, vortex-induced vibrations, etc. [10].
Vortices have been extensively studied and explored in the liquid state of matter. However, scientists have also extended their research to study the formation and behavior of vortices in the fourth state of matter, the plasma. Measurements done in space have shown that plasma vortices appear in the earth’s magnetosphere as well as along the Venus wake. On both planets, the solar wind encounters different obstacles. For earth, it is the earth’s magnetic field and for Venus, the interaction takes place with the ionized components in the upper layer of the planet’s atmosphere. Plasma vortices in earth-based laboratories have also been studied theoretically and experimentally [11, 12, 13, 14, 15]. Plasma is said to cover more than 99% of the matter found in the universe and dust particles are the unavoidable, omnipresent ingredients in it. Hence, in most cases, plasma and dust particles exist together, and these particles are massive (billion times heavier than the protons). Their size ranges from tens of nanometer to as large as hundreds of microns. Foreign particles in the plasma environment get charged up by the inflow of electrons and ions present in the plasma. The presence of these charged and massive particles increases the complexity of the plasma environment, and hence, this class of plasma has been named as ‘complex plasmas’ or ‘dusty plasmas’. They involve in a rich variety of physical and chemical processes and are thus investigated as a model system for various dynamical processes [16, 17]. Phase transition is an important and characteristic feature in dusty plasmas, due to which it is considered as a versatile medium to study all the three different phases (solid, liquid and gas) in just a single phase. They also behave as many particle interacting systems and provide a unique platform to study various organized collective effects prevalent in fluids, clusters, crystals, etc., in greater spatial and temporal resolution. With the help of laser light scattering, it is possible to visualize the micrometer or nanometer-sized dust particles through proper illumination. This allows to study the various phenomena in dusty plasma in greater spatial and temporal resolution since they appear in a slower time scale owing to their heavier mass [18, 19]. Along with a variety of dynamic phenomena that includes waves, shocks, solitons, etc., dusty plasma medium also supports the formation of vortices. Self-generated vortices have been observed in many dusty plasma experiments, which have been dealt with significant attention. The main cause of such vortex formation is the nonzero curl of the various forces acting on the electrically charged dust particles that are commonly found in radiofrequency (RF) discharges, microgravity conditions and subsonic dusty plasma flow with low Reynolds numbers [20, 21]. The nonzero component of the curl induces a rotational motion to the charged dust particles, which leads to the formation of the vortices. Depending on the different plasma production mechanisms and dust levitation (floating of dust particles in the plasma medium), the causes of the rotation of dust particles vary accordingly. Most importantly, the problem of fluid flow around obstacles can be investigated at the most elementary individual particle level in dusty plasmas. The existence of a liquid phase of dusty plasmas provides us the suitable conditions for the study. However, the obstacles used for such study in dusty plasmas are different from the solid obstacles in the hydrodynamic fluid medium.
In this chapter, we will concentrate mainly on dusty plasmas, their characteristics and a model system to study fluid flow around an obstacle at the particle level. After the introductory portion in Section 1, the fundamentals of dusty plasma are discussed in Section 2. In Section 3, the production of a dusty plasma medium by RF discharge will be discussed. Then in Section 4, we will discuss about the type and behavior of the obstacle which is used in dusty plasma flows. In Section 5, we will discuss the dusty plasma flow and the pattern formation behind the obstacle. The final section then summarizes the chapter as a whole.
First, let us start with a very brief explanation of plasma! Basically, plasma is an assembly of a nearly equal number of electrons and ions, and the charge neutrality is sustained on a macroscopic scale. In the absence of any external disturbance, that is, under equilibrium conditions, the resulting total electric charge is zero. The microscopic space-charge fields cancel out inside the plasma and the net charge over a macroscopic region vanishes totally. The quasi-neutrality condition at equilibrium is given by,
where
The ‘plasma’ state of matter differs from ordinary fluids and solids by its natural property of exhibiting collective behavior. These collective effects result in the occurrence of various physical phenomena in the plasma, resulting in the long-range of electromagnetic forces among the charged particles. The very first example of plasma that is obvious to refer is the Sun, the source of existence of life. The protective layer to the earth’s atmosphere, known as the ionosphere, also remains in the form of ionized particles, that is plasma. Moreover, natural plasmas exist in interstellar space, stars, intergalactic space, galaxies, etc. On earth, the common form of natural plasma is lightning, fire and the amazing Aurora Borealis. Artificial plasmas are generated by applying electric or magnetic fields through a gas at low pressures. These are commonly found in street lights, neon lights, etc. Neon light is a gas discharge light, which is actually a sealed glass tube with metal electrodes at both the ends of the tube and filled with one or several gases at low pressure.
As already mentioned before, dust particles in space as well as in earth’s atmosphere, are unavoidable. These particles in plasma form a new field, that is dusty plasma or complex plasma. Dusty plasma is defined as a normal electron-ion plasma with charged dust components added to it. Naturally, dust grains are metallic, conducting, or made of ice particulates. Until and unless these are manufactured in laboratories, their shape and size vary. Depending on the surrounding plasma environments (due to the inflow of electrons and ions), dust particulates are either negatively or positively charged. These charged particles as a whole affect the plasma and result in collective and unusual behavior. When observed from afar, dust particles can be considered as point charges. As they are charged by the plasma species (electrons and ions), the charge neutrality condition is now modified, which is given by,
where
Plasma possesses the fundamental property of shielding any external potential by forming a space charge around it. This particular property provides a measure of the distance over which the influence of the electric field of a charged particle (dust particle in our case) is experienced by other particles (electrons and ions) inside the plasma. Typically, this length is known as the dust Debye length
where
A pictorial representation of a dusty plasma medium is shown in Figure 1.
Schematic of a dusty plasma medium. The pink-shaded portion is the plasma medium. The green ball is the dust particle that is negatively charged.
In a dusty plasma medium, the charged particles interact with each other
where
where
Depending on the coupling parameter, a dusty plasma system remains in a weakly coupled state or a strongly coupled one. When
Thus, we see that by adjusting the dusty plasma parameters, we can obtain a fluid state of the dusty plasma medium experimentally. This provides us a unique model to study vortex formation behind an obstacle in the particle most level.
Laboratory dusty plasmas differ from space and astrophysical dusty plasmas in a significant manner. The discharges done in the laboratory have geometrical boundaries. The composition, structure, conductivity, temperature, etc., of these geometries affect the formation and transport of the dust grains. Also, the external circuit, which produces and sustains the dusty plasma, imposes boundary conditions on the dusty discharge, which vary spatially as well as temporally. Dusty plasmas in the laboratory are generally produced by two main discharge techniques—direct current (DC) discharge and RF discharge. In this chapter, we will mainly focus on the production technique by RF discharge method in a DUPLEX device.
As the name suggests, DUPLEX is an abbreviation for Dusty Plasma Experimental Chamber. It comprises of a cylindrical glass chamber, 100 cm in length and 15 cm in diameter. The glass chamber configuration of the DUPLEX device provides a suitable and great access for optical diagnostics. One end of the cylindrical chamber is connected to the vacuum pump systems and the other end is closed by a stainless steel (SS) flange with Teflon O-ring between the glass chamber and the SS flange. On this closed end, there are ports for pressure gauge fitting, probe insertion and electrical connections. A radio frequency power generator (frequency: 13.56 MHz, power: 0–300 W) and an RF matching network are used for the plasma discharge. The RF antennas used in this setup are aluminum strips of 2.5 cm width and 20 cm length typically placed on the outer surface of the glass chamber. A schematic of the setup is shown in Figure 2. This strip acts as the live electrodes.
Schematic of a DUPLEX setup. The pink-shaded portion is the argon plasma.
Initially, the chamber pressure is reduced to a value of about ∼10−3 mbar with the help of a rotary pump. Argon is used as the discharge gas, by injecting which the desired chamber pressure can be maintained. A grounded base plate is also inserted into the chamber (about ∼30 cm length, 14.5 cm width and 0.2 cm thickness), which acts as the grounded electrode and the region above it is selected as the experimental region. Applying a radiofrequency power (13.56 MHz and 5 W) between the aluminum strips (working as live electrodes) and the grounded base plate, a capacitively coupled RF discharge plasma is produced. Due to the application of the RF field, initially, the stray electrons inside the chamber get energized and in turn ionize the gas molecules present in the chamber. The aluminum strips used as live electrode outside give the flexibility to change the electrode position whenever required. Also, it facilitates in forming a uniform plasma over an extensive area of the grounded plate, that is the experimental region. The plasma parameters can be varied manually by tuning the discharge conditions,
Dust particles used in the experiment are gold-coated silica dust particles (∼ 5 micron diameter). These are initially put inside a buzzer that is fitted to the grounded base plate. After the production of the plasma, a direct current (DC) voltage of ∼ (6–12)V is applied to the buzzer, which ejects the dust particles from it through a hole. When these dust particles enter into the plasma environment, electrons and ions flow towards it and charge up the particles. In the laboratory, the dust particles are usually negatively charged as the electrons are lighter and highly mobile than the ions. These negatively charged dust particles are acted upon by two forces mainly, the upward electric field force (
Photograph of a dust layer levitation in plasma.
The obstacle used in dusty plasma flow experiments is actually a dust void. A void is a dust-free region, which is encountered spontaneously in certain experimental conditions or can be produced externally also [23, 24, 25, 26, 27, 28]. In the past couple of decades, there have been a few studies on the interaction of a dusty plasma medium with dust voids. In 2004, Morfill et al. studied a laminar flow of liquid dusty plasma with a velocity ∼ 0.8 cms−1 around a spontaneously generated lentil-shaped void [29]. They observed the formation of a wake behind the void that is separated from the laminar flow region by a mixing layer. The flow also exhibited stable vortex flows adjacent to the boundary of the mixing layer. Another study was made in 2012 by Saitou et al. where they externally placed a thin conducting wire of 0.2 mm diameter and 2.5 cm length. They made the dust particles flow with velocity in the range ∼ (5–15) cms−1 but did not observe any vortex formation behind the obstacle. What they observed was a bow shock in front of it [30]. In the very next year itself (2013), Meyer et al. also did a similar experiment with a different configuration and dust flow mechanism (velocity ∼ 10–25 cms−1) than Saitou’s [21]. They produced a dust void by placing a 0.5-mm-diameter cylindrical wire transverse to the flow. They too observed a bow shock and a tear-shaped wake in front and behind the obstacle, respectively. Moreover, Charan et al. in 2016 did a molecular dynamics simulation study where they used a square obstacle and observed von Karman vortex street at low Reynolds number (i.e. low velocity) compared with normal hydrodynamic fluids [31]. Then in 2018, Jaiswal et al. investigated dust flow towards a spherical obstacle over a range of flow velocities ∼ (4–15)cms−1 and different obstacle biases [32]. The spherical obstacle also generated a dust-free area in its vicinity. They too observed bow shock formation in front of the obstacle but no vortex formation behind it. In 2020, Bailung et al. also investigated the study of dust flow around a dust void with a unique flow mechanism (dust flow velocity ∼ 3–10 cms−1) in a DUPLEX setup [33]. Dust particles are allowed to flow towards an already existing stationary dust layer. They could observe the formation of a counter-rotating pair of vortices behind the obstacle in a particularly narrow range of velocity ∼ (4–7) cms−1. Above and below this range, their vortices are not observed. Due to the interplay between these two forces, a circular void is generated around the pin. At the void boundary, these two forces equate with each other.
In the next section, we will study the results of Bailung et al. in detail, but before that let us understand the mechanism of the formation of dust void due to the insertion of an external cylindrical wire. A cylindrical pin inside the plasma attains a negative potential for the plasma and a sheath is formed in its vicinity. Due to the negative potential of the pin, ions try to drift towards it giving rise to a force on the dust particles named as ion drag force. This force is directed radially inward with the pin as the centre. Also, the negatively charged dust particles experience a repulsive electrostatic force from the pin which is directed radially outward. The interplay between these two forces generates a circular void around the pin. At the void boundary, these two forces equate with each other. A typical configuration of pin insertion through the grounded plate of a DUPLEX chamber is shown in Figure 4. The pin is externally connected to a DC bias voltage. By varying the bias voltage, the size of the void can be altered according to experimental requirements. Typically, at a RF power of 5 W and chamber pressure ∼ 0.02 mbar, the diameter of the dust void in floating condition (i.e. no external bias) is ∼1.7 cm. A typical example of a dust void is shown in Figure 5. However, unlike the solid obstacles in the case of hydrodynamic fluids, the dust void is not a rigid kind of obstacle. As already seen, the boundary of the void is maintained by a delicate force balance between the outward electrostatic force and inward ion drag force. An incoming dust flow, depending on the velocity of the flow, would cross the void boundary and penetrate into the void.
Snapshot of a dust void formed in DUPLEX chamber. The bright spot in the Centre is the reflection of laser light from the cylindrical pin. The photograph is taken from the top of the chamber.
Due to the non-rigidity of the dust void boundary, the behavior of the flow near the obstacle is somewhat different than conditions of hydrodynamic fluid with a rigid obstacle. Despite this difference, the transition from laminar to turbulence is observed in the wake of the obstacle in the case of dusty plasma flow also. As the flow approaches the void boundary, the middle section of the flow slightly penetrates into the void region and slips through the void boundary layer on both sides. The trajectory of the flow (in the mid-section) is deflected in front of the void due to the repulsive force exerted by the sheath electric field of the void and then flows downstream surrounding the void. The curved dust flow again meets behind the void and continues with the flow. As observed by Bailung et al. at a very narrow range of velocity ∼ (4–7) cms−1, a counter-rotating vortex pair is seen to appear. Below and above this range, the dust particles do not form any vortices. A typical example of three different conditions is shown in Figure 6.
Typical snapshots showing structures formed behind the void at (a) 3.5cms−1, (b) 4.5cms−1, (c) 8 cm−1.
In each of the images, dust particles flow from right to left shown by dashed arrows. The top image (a) depicts a flow with dust flow velocity ∼ 3.5 cms−1 and the snapshot is at time t = 1370 ms from a reference time (t = 0, when dust flow reaches the right edge of the images). The middle image (b) shows dust fluid flow velocity ∼ 4.5 cms−1 at t = 1033 ms showing a vortex pair formation behind the void. The vortices are shown by the two arrow marks. It is observed that vortices are not formed for larger flow velocity ∼ 8 cms−1 (image (c)). For such high velocities, flow trajectories behind the void are elongated and dynamics in the wake is rather complex due to cross-flow at high speed. The bright illuminated point at the centre of each image is the reflection of laser light from the pin. Two horizontal lines that appear in all the images are due to laser reflection from the wall of the glass chamber. It is noted that dust flow with unsteady laminar velocity, which is (4–7)cms−1, and optimum dust density in the experimental region above the grounded plate is required to generate the vortex behind the void.
For a better understanding, a pictorial representation showing the dusty plasma streamlines around dust void at three different velocities are shown in Figure 7(a)–(c) of Figure 7 corresponds to the observation shown in (a), (b) and (c) of Figure 6.
A pictorial illustration of the dusty plasma flow interaction with the dust void at different flow velocities. (a) Laminar flow, (b) unsteady laminar flow with filamentary vortex-type structure in the upstream and vortex pair in the downstream and (c) turbulent flow.
At a lower dust flow velocity, the void in the upstream is slightly compressed and trajectories of the streamlines flowing close to the void (boundary layer) curl behind the void. However, no structure formation in the wake appears here. Dust particles, after meeting behind the void, just continue with the flow smoothly. For critical flow speed (b), flow dynamics in the upstream void boundary is quite different. Streamlines that hit perpendicularly at the void flow some distance into the void region. They reconstruct the boundary during the flow and get ejected backward making the streamline bifurcation to occur much ahead of the void boundary. The curved streamlines, which are ejected backward, again flow along with the incoming dust flow close to the boundary layer. This critical reorientation in the front of the void generates a suitable condition for the formation of the vortex pair behind the void. Particles get slowed down in this region and these slower particles flow close to the boundary layer around the void and contribute in the formation of the vortex pair. At higher velocities (c), that is above the critical range for vortex formation, all the particles that hit the upstream void boundary are flushed away by the flow along with it. The streamlines intersect and crossover at a distance far behind the void and there is no formation of any stable structure. It is well known that in hydrodynamic fluids, at much higher velocities, vortex streets are observed. However, here such streets are not observed to form. This may be due to the restriction of the experimental geometry. The transition from laminar to turbulence is well known in fluid dynamics. But studying it in dusty plasma provides the chance to observe the individual particle-level trajectory. In turn, the dynamics can be studied in greater detail.
To see the dust dynamics in greater detail, let us look at the vortex formation behind the dust void step by step. At the outset of the formation, the slower particles moving along the curved boundary layer interact with the stationary particles behind the void and start to swirl on each side. The flow front then meets in the wake region behind the void (Figure 8(a)) and gradually traverses a swirling circular path. This is evident in the dotted arrow marks in (Figure b). After duration of 966 ms from the start of the flow, two counter-rotating vortices complete their formation (Figure c). Only the slower particles flowing close to the boundary layer participate in this swirling motion due to the nonzero curl of the forces. Those particles away from the boundary layer move faster and do not contribute to the swirling. With increasing time and inflow of more particles, the swirling finally grows into a distinct pair of the vortex with an eye in the middle (Figure (d)). As the flow progresses by maintaining a constant inflow of particle flux, the vortex pair sustains till 1167 ms. The one shot of dust flow in the experiment done by Bailung et al. lasted for about 2 sec.
The parallel arrows depict the direction of the dust flow. (a) when both the oppositely curling flow front meet behind the void. Dotted curve traces in (b) indicate flow trajectories. The arrows in (c) - (g) show the vortex pair. the vortices vanish with time when flow is nearly over (h).
Hence, gradually when the particle flux started decreasing, the vortex pair starts to die out. It is faintly visible till 1233 ms (Figure g). The time for the growth of the vortex pair is ∼200 ms (from the time the particles meet behind the void) and survives for duration of 200 ms (depending on the duration of accelerated dusty plasma fluid flow). Finally, they disappear after 1300 ms. The rotational frequency measured for the vortices is about ∼3 Hz.
It is already mentioned that the advantage of studying vortex dynamics in dusty plasma lies in the fact that particles can be individually tracked. Different particle tracking software and computational models are available, which can generate the velocity vectors of the trajectory of the particles and hence can give a quantitative interpretation of the experimentally observed results. One such particle tracking platform is OpenPIV (Open Particle Image Velocimetry) in MATLAB [34]. This helps to study the evolution of the vortex pair along with its vorticity. But to perform successful PIV from images, the recorded videos of the dust flow dynamics should have a high-quality resolution and must be in high speed. A PIV analysis performed on a video recorded at 100 frames per second is shown in Figure 9.
PIV analysis showing the time evolution of the vortices for a duration of 1 sec. The velocity vectors and vorticity profile drawn from (a) (0.53-0.62) sec (b) (0.63-0.72) sec (c) (0.73-0.82) sec (d) (0.83-0.92) sec (e) (0.93-1.02) sec (f) (1.03-1.12) sec (g) (1.13-1.22) sec (h) (1.23-1.32) sec (i) (1.33-1.42) sec (j) (1.43-1.52) sec are shown. The color bar shows the value of vorticity in 1/s. The dotted circle in (a) shows the original position of the void boundary before the flow and the dot at the center of the circle depicts the pin position.
Each image in the figure is an average PIV result of 10 consecutive image frames. The position of the void and the pin position are drawn by a red-dashed circle and a red dot, respectively. The velocity vectors show the trajectory of the dust particles and the color code gives the value of the vorticity at different times in units of s−1. The slowing down of the particles in front of the void is clearly seen by comparing the velocity vectors’ lengths in Figure 9(a) and (b). The backflow of the incoming dust particles mentioned earlier (due to repulsive sheath electric field force of the pin) is also observed in (b). The curling of dust particles leading to vortex formation is evident from (c) and (d). The vorticity of the fully formed vortex pair is about ∼ (20–25)s−1, which is shown by the color bar in (e) and (f)). This is nearly equal to twice the measured angular frequency. With the decrease of the dust flow influx, the vortex structure deforms (vorticity ∼15 s−1) and breaks away into smaller vortices (vorticity ∼10s−1) as seen from (g) to (i). Vortices finally disappear in (j), evident from the vorticity value which almost tends to 0.
Reynolds number is the characteristic parameter that helps to predict flow patterns. It is the ratio of the inertial forces to the viscous forces and is given by,
where
In case of dusty plasma fluids, the viscosity is estimated from the formula,
where
The viscosity is calculated to be
Thus, the Reynolds number for dust flow velocity ∼ (3–10) cms−1 is estimated to be lying in the range 50–190. The vortex pair formation appears in a critical range of 60–90.
In the case of hydrodynamic fluid, the range of Reynolds number for vortex formation is 5–40, which is much lower compared with that in dusty plasma fluid. This is because the ratio
The study of vortices in the problem of flow past an obstacle is significant as it provides a platform to investigate the transition from laminar to turbulence. Formation of vortices in the wake region behind an obstacle appears in the unsteady laminar regime of flows and has been widely studied in hydrodynamic fluids. However, dusty plasma medium, which is a component of the fourth state of matter, provides a unique stage to study such phenomena at the particle level. A special property of this medium is that it can remain in both fluids (liquid- or gas-like) as well as the crystalline state. By mere adjustment of plasma conditions, the desired state can be obtained. The individual tracking of micron-sized dust particles by methods such as PIV (Particle Image Velocimetry) yields the particle trajectory in form of velocity vector fields. This gives a very clear picture of the behavior of flow near obstacle boundaries. However, the obstacles used in dusty plasma flow experiments differ from those in hydrodynamic fluid experiments in the sense that unlike those in hydrodynamics, the obstacle boundaries in dusty plasma are non-rigid. Any foreign pin or wire inserted into the plasma would possess a negative potential with respect to the plasma. Dust particles in its vicinity are repelled due to electrostatic force and form a dust-free region around it, called the dust void. This dust void, whose boundary is delicately maintained by dusty plasma forces, acts as a non-rigid type of obstacle. Dusty plasma flows also generate counter-rotating vortices in the wake region behind a dust void at a particular range of velocities. Below and above this range, no structure formation is seen to appear. The particle behavior causing the formation of the vortices is better understood by tracking particles in consecutive frames. The estimated Reynolds number value for vortices to appear in the wake of a void in a dusty plasma medium is estimated to lie in the range 60–90. This is quite larger than the Reynolds number range for hydrodynamic fluids which is roughly about 5–40. This higher range in dusty plasma medium is attributed to the higher kinematic viscosity of dusty plasma fluids. However, in dusty plasma experiments, Von Karman vortex streets (observed in the turbulent regime of hydrodynamic fluids) are not yet explored. If such experiments could be successfully performed, then there will be immense scope of understanding turbulence at the particle-most level and with a better perspective. Although to study turbulent dynamics, high-speed cameras with high-quality resolution would be necessary.
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On September, 29th 2006 he has won a post PhD fellowship from the university of Bologna (from October 2006 to October 2008), at the competitive examination he was ranked first in the industrial engineering area. He extensively served as referee for several international journals. He is author/coauthor of more than 100 research papers. He has been involved in some projects supported by MURST and European Community. 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He also obtained an MSc in Molecular and Genetic Medicine, and a Ph.D. in Clinical Immunology and Human Genetics from the University of Sheffield, UK. He also completed a short-term fellowship in Pediatric Clinical Immunology and Bone Marrow Transplantation at Newcastle General Hospital, England. Dr. Rezaei is a Full Professor of Immunology and Vice Dean of International Affairs and Research, at the School of Medicine, Tehran University of Medical Sciences, and the co-founder and head of the Research Center for Immunodeficiencies. He is also the founding president of the Universal Scientific Education and Research Network (USERN). Dr. Rezaei has directed more than 100 research projects and has designed and participated in several international collaborative projects. He is an editor, editorial assistant, or editorial board member of more than forty international journals. He has edited more than 50 international books, presented more than 500 lectures/posters in congresses/meetings, and published more than 1,100 scientific papers in international journals.",institutionString:"Tehran University of Medical Sciences",institution:{name:"Tehran University of Medical Sciences",country:{name:"Iran"}}},{id:"180733",title:"Dr.",name:"Jean",middleName:null,surname:"Engohang-Ndong",slug:"jean-engohang-ndong",fullName:"Jean Engohang-Ndong",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/180733/images/system/180733.png",biography:"Dr. Jean Engohang-Ndong was born and raised in Gabon. After obtaining his Associate Degree of Science at the University of Science and Technology of Masuku, Gabon, he continued his education in France where he obtained his BS, MS, and Ph.D. in Medical Microbiology. He worked as a post-doctoral fellow at the Public Health Research Institute (PHRI), Newark, NJ for four years before accepting a three-year faculty position at Brigham Young University-Hawaii. Dr. Engohang-Ndong is a tenured faculty member with the academic rank of Full Professor at Kent State University, Ohio, where he teaches a wide range of biological science courses and pursues his research in medical and environmental microbiology. Recently, he expanded his research interest to epidemiology and biostatistics of chronic diseases in Gabon.",institutionString:"Kent State University",institution:{name:"Kent State University",country:{name:"United States of America"}}},{id:"188773",title:"Prof.",name:"Emmanuel",middleName:null,surname:"Drouet",slug:"emmanuel-drouet",fullName:"Emmanuel Drouet",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/188773/images/system/188773.png",biography:"Emmanuel Drouet, PharmD, is a Professor of Virology at the Faculty of Pharmacy, the University Grenoble-Alpes, France. As a head scientist at the Institute of Structural Biology in Grenoble, Dr. Drouet’s research investigates persisting viruses in humans (RNA and DNA viruses) and the balance with our host immune system. He focuses on these viruses’ effects on humans (both their impact on pathology and their symbiotic relationships in humans). He has an excellent track record in the herpesvirus field, and his group is engaged in clinical research in the field of Epstein-Barr virus diseases. He is the editor of the online Encyclopedia of Environment and he coordinates the Universal Health Coverage education program for the BioHealth Computing Schools of the European Institute of Science.",institutionString:null,institution:{name:"Grenoble Alpes University",country:{name:"France"}}},{id:"131400",title:"Prof.",name:"Alfonso J.",middleName:null,surname:"Rodriguez-Morales",slug:"alfonso-j.-rodriguez-morales",fullName:"Alfonso J. Rodriguez-Morales",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/131400/images/system/131400.png",biography:"Dr. Rodriguez-Morales is an expert in tropical and emerging diseases, particularly zoonotic and vector-borne diseases (especially arboviral diseases). He is the president of the Travel Medicine Committee of the Pan-American Infectious Diseases Association (API), as well as the president of the Colombian Association of Infectious Diseases (ACIN). He is a member of the Committee on Tropical Medicine, Zoonoses, and Travel Medicine of ACIN. He is a vice-president of the Latin American Society for Travel Medicine (SLAMVI) and a Member of the Council of the International Society for Infectious Diseases (ISID). Since 2014, he has been recognized as a Senior Researcher, at the Ministry of Science of Colombia. He is a professor at the Faculty of Medicine of the Fundacion Universitaria Autonoma de las Americas, in Pereira, Risaralda, Colombia. He is an External Professor, Master in Research on Tropical Medicine and International Health, Universitat de Barcelona, Spain. He is also a professor at the Master in Clinical Epidemiology and Biostatistics, Universidad Científica del Sur, Lima, Peru. In 2021 he has been awarded the “Raul Isturiz Award” Medal of the API. Also, in 2021, he was awarded with the “Jose Felix Patiño” Asclepius Staff Medal of the Colombian Medical College, due to his scientific contributions to COVID-19 during the pandemic. He is currently the Editor in Chief of the journal Travel Medicine and Infectious Diseases. His Scopus H index is 47 (Google Scholar H index, 68).",institutionString:"Institución Universitaria Visión de las Américas, Colombia",institution:null},{id:"332819",title:"Dr.",name:"Chukwudi Michael",middleName:"Michael",surname:"Egbuche",slug:"chukwudi-michael-egbuche",fullName:"Chukwudi Michael Egbuche",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/332819/images/14624_n.jpg",biography:"I an Dr. Chukwudi Michael Egbuche. I am a Senior Lecturer in the Department of Parasitology and Entomology, Nnamdi Azikiwe University, Awka.",institutionString:null,institution:{name:"Nnamdi Azikiwe University",country:{name:"Nigeria"}}},{id:"284232",title:"Mr.",name:"Nikunj",middleName:"U",surname:"Tandel",slug:"nikunj-tandel",fullName:"Nikunj Tandel",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/284232/images/8275_n.jpg",biography:'Mr. Nikunj Tandel has completed his Master\'s degree in Biotechnology from VIT University, India in the year of 2012. He is having 8 years of research experience especially in the field of malaria epidemiology, immunology, and nanoparticle-based drug delivery system against the infectious diseases, autoimmune disorders and cancer. He has worked for the NIH funded-International Center of Excellence in Malaria Research project "Center for the study of complex malaria in India (CSCMi)" in collaboration with New York University. The preliminary objectives of the study are to understand and develop the evidence-based tools and interventions for the control and prevention of malaria in different sites of the INDIA. Alongside, with the help of next-generation genomics study, the team has studied the antimalarial drug resistance in India. Further, he has extended his research in the development of Humanized mice for the study of liver-stage malaria and identification of molecular marker(s) for the Artemisinin resistance. At present, his research focuses on understanding the role of B cells in the activation of CD8+ T cells in malaria. Received the CSIR-SRF (Senior Research Fellow) award-2018, FIMSA (Federation of Immunological Societies of Asia-Oceania) Travel Bursary award to attend the IUIS-IIS-FIMSA Immunology course-2019',institutionString:"Nirma University",institution:{name:"Nirma University",country:{name:"India"}}},{id:"334383",title:"Ph.D.",name:"Simone",middleName:"Ulrich",surname:"Ulrich Picoli",slug:"simone-ulrich-picoli",fullName:"Simone Ulrich Picoli",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/334383/images/15919_n.jpg",biography:"Graduated in Pharmacy from Universidade Luterana do Brasil (1999), Master in Agricultural and Environmental Microbiology from Federal University of Rio Grande do Sul (2002), Specialization in Clinical Microbiology from Universidade de São Paulo, USP (2007) and PhD in Sciences in Gastroenterology and Hepatology (2012). She is currently an Adjunct Professor at Feevale University in Medicine and Biomedicine courses and a permanent professor of the Academic Master\\'s Degree in Virology. She has experience in the field of Microbiology, with an emphasis on Bacteriology, working mainly on the following topics: bacteriophages, bacterial resistance, clinical microbiology and food microbiology.",institutionString:null,institution:{name:"Universidade Feevale",country:{name:"Brazil"}}},{id:"229220",title:"Dr.",name:"Amjad",middleName:"Islam",surname:"Aqib",slug:"amjad-aqib",fullName:"Amjad Aqib",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/229220/images/system/229220.png",biography:"Dr. Amjad Islam Aqib obtained a DVM and MSc (Hons) from University of Agriculture Faisalabad (UAF), Pakistan, and a PhD from the University of Veterinary and Animal Sciences Lahore, Pakistan. Dr. Aqib joined the Department of Clinical Medicine and Surgery at UAF for one year as an assistant professor where he developed a research laboratory designated for pathogenic bacteria. Since 2018, he has been Assistant Professor/Officer in-charge, Department of Medicine, Manager Research Operations and Development-ORIC, and President One Health Club at Cholistan University of Veterinary and Animal Sciences, Bahawalpur, Pakistan. He has nearly 100 publications to his credit. His research interests include epidemiological patterns and molecular analysis of antimicrobial resistance and modulation and vaccine development against animal pathogens of public health concern.",institutionString:"Cholistan University of Veterinary and Animal Sciences",institution:null},{id:"62900",title:"Prof.",name:"Fethi",middleName:null,surname:"Derbel",slug:"fethi-derbel",fullName:"Fethi Derbel",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/62900/images/system/62900.jpeg",biography:"Professor Fethi Derbel was born in 1960 in Tunisia. He received his medical degree from the Sousse Faculty of Medicine at Sousse, University of Sousse, Tunisia. He completed his surgical residency in General Surgery at the University Hospital Farhat Hached of Sousse and was a member of the Unit of Liver Transplantation in the University of Rennes, France. He then worked in the Department of Surgery at the Sahloul University Hospital in Sousse. Professor Derbel is presently working at the Clinique les Oliviers, Sousse, Tunisia. His hospital activities are mostly concerned with laparoscopic, colorectal, pancreatic, hepatobiliary, and gastric surgery. He is also very interested in hernia surgery and performs ventral hernia repairs and inguinal hernia repairs. He has been a member of the GREPA and Tunisian Hernia Society (THS). During his residency, he managed patients suffering from diabetic foot, and he was very interested in this pathology. For this reason, he decided to coordinate a book project dealing with the diabetic foot. Professor Derbel has published many articles in journals and collaborates intensively with IntechOpen Access Publisher as an editor.",institutionString:"Clinique les Oliviers",institution:null},{id:"300144",title:"Dr.",name:"Meriem",middleName:null,surname:"Braiki",slug:"meriem-braiki",fullName:"Meriem Braiki",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/300144/images/system/300144.jpg",biography:"Dr. Meriem Braiki is a specialist in pediatric surgeon from Tunisia. She was born in 1985. She received her medical degree from the University of Medicine at Sousse, Tunisia. She achieved her surgical residency training periods in Pediatric Surgery departments at University Hospitals in Monastir, Tunis and France.\r\nShe is currently working at the Pediatric surgery department, Sidi Bouzid Hospital, Tunisia. Her hospital activities are mostly concerned with laparoscopic, parietal, urological and digestive surgery. She has published several articles in diffrent journals.",institutionString:"Sidi Bouzid Regional Hospital",institution:null},{id:"229481",title:"Dr.",name:"Erika M.",middleName:"Martins",surname:"de Carvalho",slug:"erika-m.-de-carvalho",fullName:"Erika M. de Carvalho",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/229481/images/6397_n.jpg",biography:null,institutionString:null,institution:{name:"Oswaldo Cruz Foundation",country:{name:"Brazil"}}},{id:"186537",title:"Prof.",name:"Tonay",middleName:null,surname:"Inceboz",slug:"tonay-inceboz",fullName:"Tonay Inceboz",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/186537/images/system/186537.jfif",biography:"I was graduated from Ege University of Medical Faculty (Turkey) in 1988 and completed his Med. PhD degree in Medical Parasitology at the same university. I became an Associate Professor in 2008 and Professor in 2014. I am currently working as a Professor at the Department of Medical Parasitology at Dokuz Eylul University, Izmir, Turkey.\n\nI have given many lectures, presentations in different academic meetings. I have more than 60 articles in peer-reviewed journals, 18 book chapters, 1 book editorship.\n\nMy research interests are Echinococcus granulosus, Echinococcus multilocularis (diagnosis, life cycle, in vitro and in vivo cultivation), and Trichomonas vaginalis (diagnosis, PCR, and in vitro cultivation).",institutionString:"Dokuz Eylül University",institution:{name:"Dokuz Eylül University",country:{name:"Turkey"}}},{id:"71812",title:"Prof.",name:"Hanem Fathy",middleName:"Fathy",surname:"Khater",slug:"hanem-fathy-khater",fullName:"Hanem Fathy Khater",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/71812/images/1167_n.jpg",biography:"Prof. Khater is a Professor of Parasitology at Benha University, Egypt. She studied for her doctoral degree, at the Department of Entomology, College of Agriculture, Food and Natural Resources, University of Missouri, Columbia, USA. She has completed her Ph.D. degrees in Parasitology in Egypt, from where she got the award for “the best scientific Ph.D. dissertation”. She worked at the School of Biological Sciences, Bristol, England, the UK in controlling insects of medical and veterinary importance as a grant from Newton Mosharafa, the British Council. Her research is focused on searching of pesticides against mosquitoes, house flies, lice, green bottle fly, camel nasal botfly, soft and hard ticks, mites, and the diamondback moth as well as control of several parasites using safe and natural materials to avoid drug resistances and environmental contamination.",institutionString:null,institution:{name:"Banha University",country:{name:"Egypt"}}},{id:"99780",title:"Prof.",name:"Omolade",middleName:"Olayinka",surname:"Okwa",slug:"omolade-okwa",fullName:"Omolade Okwa",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/99780/images/system/99780.jpg",biography:"Omolade Olayinka Okwa is presently a Professor of Parasitology at Lagos State University, Nigeria. She has a PhD in Parasitology (1997), an MSc in Cellular Parasitology (1992), and a BSc (Hons) Zoology (1990) all from the University of Ibadan, Nigeria. She teaches parasitology at the undergraduate and postgraduate levels. She was a recipient of a Commonwealth fellowship supported by British Council tenable at the Centre for Entomology and Parasitology (CAEP), Keele University, United Kingdom between 2004 and 2005. She was awarded an Honorary Visiting Research Fellow at the same university from 2005 to 2007. \nShe has been an external examiner to the Department of Veterinary Microbiology and Parasitology, University of Ibadan, MSc programme between 2010 and 2012. She is a member of the Nigerian Society of Experimental Biology (NISEB), Parasitology and Public Health Society of Nigeria (PPSN), Science Association of Nigeria (SAN), Zoological Society of Nigeria (ZSN), and is Vice Chairperson of the Organisation of Women in Science (OWSG), LASU chapter. She served as Head of Department of Zoology and Environmental Biology, Lagos State University from 2007 to 2010 and 2014 to 2016. She is a reviewer for several local and international journals such as Unilag Journal of Science, Libyan Journal of Medicine, Journal of Medicine and Medical Sciences, and Annual Research and Review in Science. \nShe has authored 45 scientific research publications in local and international journals, 8 scientific reviews, 4 books, and 3 book chapters, which includes the books “Malaria Parasites” and “Malaria” which are IntechOpen access publications.",institutionString:"Lagos State University",institution:{name:"Lagos State University",country:{name:"Nigeria"}}},{id:"273100",title:"Dr.",name:"Vijay",middleName:null,surname:"Gayam",slug:"vijay-gayam",fullName:"Vijay Gayam",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/273100/images/system/273100.jpeg",biography:"Dr. Vijay Bhaskar Reddy Gayam is currently practicing as an internist at Interfaith Medical Center in Brooklyn, New York, USA. He is also a Clinical Assistant Professor at the SUNY Downstate University Hospital and Adjunct Professor of Medicine at the American University of Antigua. He is a holder of an M.B.B.S. degree bestowed to him by Osmania Medical College and received his M.D. at Interfaith Medical Center. His career goals thus far have heavily focused on direct patient care, medical education, and clinical research. He currently serves in two leadership capacities; Assistant Program Director of Medicine at Interfaith Medical Center and as a Councilor for the American\r\nFederation for Medical Research. As a true academician and researcher, he has more than 50 papers indexed in international peer-reviewed journals. He has also presented numerous papers in multiple national and international scientific conferences. His areas of research interest include general internal medicine, gastroenterology and hepatology. 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In recent years, the application of chemistry to biological molecules has gained significant interest in medicinal and pharmacological studies. This topic will be devoted to understanding the interplay between biomolecules and chemical compounds, their structure and function, and their potential applications in related fields. Being a part of the biochemistry discipline, the ideas and concepts that have emerged from Chemical Biology have affected other related areas. This topic will closely deal with all emerging trends in this discipline.",coverUrl:"https://cdn.intechopen.com/series_topics/covers/15.jpg",keywords:"Phenolic Compounds, Essential Oils, Modification of Biomolecules, Glycobiology, Combinatorial Chemistry, Therapeutic peptides, Enzyme Inhibitors"},{id:"17",title:"Metabolism",scope:"Metabolism is frequently defined in biochemistry textbooks as the overall process that allows living systems to acquire and use the free energy they need for their vital functions or the chemical processes that occur within a living organism to maintain life. Behind these definitions are hidden all the aspects of normal and pathological functioning of all processes that the topic ‘Metabolism’ will cover within the Biochemistry Series. Thus all studies on metabolism will be considered for publication.",coverUrl:"https://cdn.intechopen.com/series_topics/covers/17.jpg",keywords:"Biomolecules Metabolism, Energy Metabolism, Metabolic Pathways, Key Metabolic Enzymes, Metabolic Adaptation"},{id:"18",title:"Proteomics",scope:"With the recognition that the human genome cannot provide answers to the etiology of a disorder, changes in the proteins expressed by a genome became a focus in research. Thus proteomics, an area of research that detects all protein forms expressed in an organism, including splice isoforms and post-translational modifications, is more suitable than genomics for a comprehensive understanding of the biochemical processes that govern life. The most common proteomics applications are currently in the clinical field for the identification, in a variety of biological matrices, of biomarkers for diagnosis and therapeutic intervention of disorders. From the comparison of proteomic profiles of control and disease or different physiological states, which may emerge, changes in protein expression can provide new insights into the roles played by some proteins in human pathologies. Understanding how proteins function and interact with each other is another goal of proteomics that makes this approach even more intriguing. Specialized technology and expertise are required to assess the proteome of any biological sample. Currently, proteomics relies mainly on mass spectrometry (MS) combined with electrophoretic (1 or 2-DE-MS) and/or chromatographic techniques (LC-MS/MS). MS is an excellent tool that has gained popularity in proteomics because of its ability to gather a complex body of information such as cataloging protein expression, identifying protein modification sites, and defining protein interactions. The Proteomics topic aims to attract contributions on all aspects of MS-based proteomics that, by pushing the boundaries of MS capabilities, may address biological problems that have not been resolved yet.",coverUrl:"https://cdn.intechopen.com/series_topics/covers/18.jpg",keywords:"Mono- and Two-Dimensional Gel Electrophoresis (1-and 2-DE), Liquid Chromatography (LC), Mass Spectrometry/Tandem Mass Spectrometry (MS; MS/MS), Proteins"}],annualVolumeBook:{},thematicCollection:[],selectedSeries:null,selectedSubseries:null},seriesLanding:{item:null},libraryRecommendation:{success:null,errors:{},institutions:[]},route:{name:"profile.detail",path:"/profiles/199012",hash:"",query:{},params:{id:"199012"},fullPath:"/profiles/199012",meta:{},from:{name:null,path:"/",hash:"",query:{},params:{},fullPath:"/",meta:{}}}},function(){var e;(e=document.currentScript||document.scripts[document.scripts.length-1]).parentNode.removeChild(e)}()