Released this past November, the list is based on data collected from the Web of Science and highlights some of the world’s most influential scientific minds by naming the researchers whose publications over the previous decade have included a high number of Highly Cited Papers placing them among the top 1% most-cited.
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We wish to congratulate all of the researchers named and especially our authors on this amazing accomplishment! We are happy and proud to share in their success!
IntechOpen is proud to announce that 191 of our authors have made the Clarivate™ Highly Cited Researchers List for 2020, ranking them among the top 1% most-cited.
\n\n
Throughout the years, the list has named a total of 261 IntechOpen authors as Highly Cited. Of those researchers, 69 have been featured on the list multiple times.
\n\n\n\n
Released this past November, the list is based on data collected from the Web of Science and highlights some of the world’s most influential scientific minds by naming the researchers whose publications over the previous decade have included a high number of Highly Cited Papers placing them among the top 1% most-cited.
\n\n
We wish to congratulate all of the researchers named and especially our authors on this amazing accomplishment! We are happy and proud to share in their success!
Note: Edited in March 2021
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This book has been designed to incorporate a wide range of new ideas and unique works from all authors from topics like Forensic Engineering, Forensic Entomology and Crime Scene Investigation. I hope that it will be useful to practitioners of forensic medicine, experts, pathologists, law makers, investigating authorities, undergraduate and postgraduate medical school graduates of medicine.",isbn:"978-953-51-2633-1",printIsbn:"978-953-51-2632-4",pdfIsbn:"978-953-51-7306-9",doi:"10.5772/61701",price:119,priceEur:129,priceUsd:155,slug:"forensic-analysis-from-death-to-justice",numberOfPages:128,isOpenForSubmission:!1,isInWos:1,isInBkci:!1,hash:"8e44125aafaaf6e8adb73d733f34fae9",bookSignature:"B. 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Suresh Kumar Shetty is a Professor in the Department of Forensic Medicine at Kasturba Medical College, Mangalore, MAHE, Manipal. He received his Master’s degree at KMC, Manipal, and joined as faculty at KMC, Mangalore, where he has been teaching since 2005.\nHe is presently appointed as the Honorary State Medico-Legal Consultant for three districts [Dakshina Kannada, Udupi and Coorg], Government of Karnataka. He has received his certificate in “Analytical Toxicology & Forensic DNA Typing” awarded by the Department of Analytical Toxicology, Amrita Institute of Medical Sciences, Cochin in November 2006, as well as his PG certificate in Torture Medicine [IMA AKN Sinha Institute, Patna] in 2011. He completed his MBA [Hospital Administration] from Sikkim Manipal University in 2016. He completed his FAIMER fellowship from MAHE, Manipal in 2018.\nHe has co-authored chapters in 3 books and peer-reviewed papers for 15 reputed national and international journals, contributed articles in local and national newspapers, guided postgraduates in Forensic Medicine and undergraduates in ICMR student projects. He has published more than 80 papers, all national and international research papers in scientific journals. He has organized a number of continued medical education [CME] programs, police training programs, seminars and conferences in the capacity of Organizing Secretary from 2009-2019. He hosted the IAFM National conference in 2013. He was the Organizing Secretary of the 1st Indo-French Forensic International Congress in 2018 and also successfully conducted the 2nd Indo-French Congress in Lyon France as Co-Organizing Secretary in 2019. He has successfully completed international collaborations with Mekelle University and Lyon University, France. He is the advisor for the Centre of Forensic Odontology and Head of the Students wing of Bio-Ethics, KMC, Mangalore. He has attended scientific sessions in India as well as abroad like Malaysia, Singapore, Vietnam, Thailand, United States of America, Hong Kong, Australia, China, Russia, and France. \nHe is the author of “Atlas Book on Forensic Pathology” published by Jayeepe Publisher. Forensic Analysis – Death to Justice by IntechOpen publisher, as well as chapters in books from Nova publisher and IntechOpen publisher. He was nominated by the International Bibliographical Centre, Cambridge, England, Selection Committee and earned a position of TOP 100 Health Professionals in 2009, who have made a significant contribution in their field to engender influence on a local, national and international issue and Individual Member of Sydney Forensic Medicine & Science Network, Australia and Asia Pacific Association of Medical Toxicology. 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Forensic analysis involves tasks of scene information mining as well as its reconstruction in order to extract elements for explanatory police test or to show forensic evidence in legal proceedings. Currently, the combination of sensors and technologies allows the integration of spatial data and the generation of virtual infographic products (orthoimages, solid images, point clouds, cross‐sections, etc.) which are extremely attractive. These products, which successfully retain accurate 3D metric information, are revolutionizing dimensional reconstruction of objects and crime scenes. Thus, it can be said that the reconstruction and 3D visualization of complex scenes are one of the main challenges for the international scientific community. To overcome this challenge, techniques related with computer vision, computer graphics and geomatics work closely. This chapter reviews a set of geomatic techniques, applied to improve infographic forensic products, and its evolution. 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The influence of this case on scientific research was not small in such a way that papers related to PTSD, disaster medical, copycats, chemical analysis, unwanted chemicals in food, terrorism, and so on were published. The forensic analyses on Wakayama arsenic poisoning incidence have characteristic that SPring-8, a largest synchrotron radiation facility, was used, as well as many other analytical techniques, but now most of the forensic analyses submitted from the prosecutor have been revealed to be fabrication, hiding the truth by logarithmic calculations, and therefore not scientific. Most of the testimonies at the court by the analysts were also lies. 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In particular, the application of these concepts to case of floods looks immediate, but other applications such as drought analysis can be addressed too. In the case of flooding events causing material damages and even loss of human lives, forensic analysis can provide results that help to clarify responsibilities but specially to prevent that future disasters happen again. This chapter will provide important information for the new forensic hydrologists, a discipline with great future, especially in the context of climate change, which will increase the magnitude, and frequency of extremes.",signatures:"Aldo I. 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Necrophagous Diptera are regarded as the most important forensic indicator species, largely because they colonize a corpse within minutes of death. Other types of carrion-inhabiting insects also offer value, although more limited than flies, to forensic investigations. Perhaps, the most neglected of these groups is the parasitic Hymenoptera, a group comprising several species that utilize necrophagous flies as natural hosts. Parasitic wasps extend the PMI window to include the period of time after necrophagous flies have emerged to when a corpse is discovered. Wasp host preferences and seasonal occurrences can reveal if a body was moved from another location prior to discovery. Foraging behavior of adults can be used to locate concealed bodies and potentially aid in combating entomological terrorism agents. Presently, the full potential of parasitic Hymenoptera as alternate forensic indicator species has not been explored. 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Its wavelength is between 750 nm and 1 mm. The amount of thermal IR radiation emitted by an object is associated with the temperature of the object, the surface area of the object and the spreading of light. 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\r\n\tCandidiasis is an infection caused by Candida spp., mostly Candida albicans. Although, Candida, a yeast, normally exists in human body; on the skin and in the mouth, throat, gut and vagina, it does not normally cause infection. However, sometimes, yeast proliferation occurs, and Candida spp. cause several infections, such as oral infection affecting the mouth and throat, called oropharyngeal candidiasis (thrush), as well as vulvovaginal, oesophageal, intestinal and invasive candidiasis. Oesophageal candidiasis is a common infection in HIV/AIDS patients. Besides this, the pathogenesis of candidiasis in humans is not completely understood. Infection caused by Candida spp. presents a serious problem because of its drug resistance. Investigation of new and effective active substances against pathogenic Candida spp. and a better understanding of the role of molecular mechanisms involved in the formation of antifungal resistance will help prevent Candida infection among individuals with immunological deficiency and will make the antifungal therapy much more effective and improved. This book is intended to provide a comprehensive overview of the latest information on Candida spp. and Candidiasis.
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\n\t\t\t
1. Introduction
\n\t\t\t
Ceramic laser media fabricated by vacuum sintering (Ikesue et al., 1995), (Ikesue et al., 1996), and nanocrystalline (Lu et al., 2000) technology are very attractive materials because they have several remarkable advantages compared with single crystal laser materials. Ceramic samples with a large size can be easily fabricated, whereas this is extremely difficult for single crystals; multiplayer and multifunctional ceramic laser materials are possible because of the polycrystallinity of ceramics (Taira, 2007). Potentially, because of their short fabrication period and because they can be mass-produced, the cost of ceramic laser materials could be much lower than that of single crystals. Furthermore, no complex facilities and critical techniques are required for the growth of ceramics. Since 1995, Ikesue and coworkers have been developing several types of ceramic laser material (Ikesue et al., 1995), (Ikesue et al., 1996), and they found in 2000 that the output power from a 3.4 at.% Nd:YAG ceramic microchip laser is twice that from a Nd:YAG crystal microchip laser of the same size (Shoji et al., 2000). At a low doping concentration, it was found that the efficiency of a diode-end-pumped Nd:YAG ceramic laser is even higher than that of a Nd:YAG single crystal laser. Since 1998, Yanagitani and coworkers have been developing several types of ceramic lasers, and Lu et al. reported the Nd:YAG ceramic laser as one of them in 2001 (Lu et al., 2001). The mechanical properties of YAG ceramics were reported by Kaminskii et al. in ref. (Kaminskii et al., 2003). YAG ceramics had a 10% higher hardness than a YAG single crystal, and the fracture toughness of the YAG ceramics was more than threefold that of the YAG single crystal. Therefore, the ceramics had a higher resistance to thermal shock than the single crystal. Ytterbium (Yb3+)-doped materials are very attractive for diode-pumped solid-state lasers (DPSSLs) (Krupke, 2000). The Yb3+-doped materials have high quantum efficiency and exhibit no concentration quenching simply because the Yb3+ ion has only two manifolds, namely, the ground state 2F7/2 and the upper level 2F5/2. Thus far, many articles about Yb:YAG crystal lasers have been published (Lacovara et al., 1991), (Hönninger et al., 1995), (Sumida et al., 1998). Yb:YAG has broad absorption and emission bands. The broad absorption band in the near-IR region is suitable for laser-diode (LD) pumping, and the broad emission band enables the generation of ultrashort pulses (Hönninger et al., 1995). However, an Yb:YAG laser is known as a quasi-three-level laser or a quasi-four-level laser, and a finite population exists at the Stark level of the lower manifold 2F7/2, where laser transition terminates, which requires high-intensity pumping, a high-brightness pump source, and an efficient heat removal technique (Matsubara et al., 2007), (Sato & Taira, 2004), (Shoji et al., 2004) to prevent reabsorption from the lower level of the laser. Takaichi et al. reported the absorption and emission spectra of a Yb:YAG ceramic (CYb = 1 at.%) and demonstrated laser oscillation, which was the first diode-end-pumped Yb:YAG ceramic laser (not Nd:YAG) with a 345 mW cw output power and a slope efficiency of 26% (Takaichi et al., 2003). Recently, Tsunekane and Taira have demonstrated a high-power diode-edge-pumped single-crystal Yb:YAG / ceramic undoped YAG composite microchip laser (Tsunekane&Taira, 2005), (Tsunekane&Taira, 2006). Early in 2007, a diode-edge-pumped, composite all-ceramic Yb:YAG (CYb = 10 at.%) microchip laser was demonstrated by Tsunekane and Taira, and a 414 W cw output power was obtained with a slope efficiency of 47% (Tsunekane & Taira, 2007). Very recently, Dong et al. have demonstrated a 2.7 W heavily doped (20 at.%) Yb:YAG ceramic laser with a slope efficiency of 52% (Dong et al., 2007) ; however, its two-pass-pumping miniature laser configuration was more complex than a simple conventional end-pumping configuration and its output power was not markedly high. Nakamura et al. demonstrated a 5.5 W cw Yb:YAG (9.8 at.%) ceramic laser with a slope efficiency of 52% using a simple end-pumping scheme (Nakamura et al., 2008a) with a 400 μm fiber-coupled LD. Dong et al. demonstrated a highly efficient (a slope efficiency of 79%) Yb:YAG ceramic laser (Dong et al., 2006) with a 100 μm fiber-coupled LD using an end-pumping scheme, but its output power was 1.7 W.
\n\t\t\t
In section 2, we report a high-power (6.8 W) and high-efficiency tunable Yb:YAG ceramic laser demonstrated using an end-pumping scheme with a slope efficiency of 72% (Nakamura et al., 2008b) at room temperature (20 C).
\n\t\t\t
Additionally, the tunability of the Yb:YAG ceramic laser for spectroscopy and femtosecond laser application. The broadest tunability is demonstrated in section 3. Finally, A diode-pumped passively mode-locked Yb:YAG ceramic laser is demonstrated in section 4. 417 and 286 fs pulses with average powers of 250 and 25 mW were obtained at 1030 nm using 1 and 0.1% output couplers, respectively. 233 fs pulses with an average power of 20 mW were also obtained at a center wavelength of 1048.3 nm using a 0.1% output coupler. To the best of our knowledge, this is the first demonstration of a diode-pumped mode-locked Yb:YAG ceramic laser.
\n\t\t\t
Figure 1.
Experimental setup for the high-power Yb:YAG ceramic laser (Nakamura et al., 2008a).
\n\t\t
\n\t\t
\n\t\t\t
2. High-power and high efficiency Yb:YAG
\n\t\t\t
\n\t\t\t\t
2.1. Experimental setup of linear cavity
\n\t\t\t\t
The experimental setup for the Yb:YAG ceramic laser is shown in Fig. 1. A 940 nm fiber-coupled LD (JENOPTIK Laserdiode, JOLD-30-FC-12) was used as a pumping source, the core diameter of the fiber was 200 μm, and the numerical aperture (NA) of the fiber was 0.22. The pumping beam was focused onto the ceramic with a ratio of 1:1 using the lenses L1 (f = 25 mm) and L2 (f = 25 mm). The diameter of the focused spot on the ceramic was ~200 μm. To obtain high efficiency and high power, a laser cavity consisting of a flat dichroic mirror (DM) and a flat output coupler (OC) as a linear resonator was used. The DM was antireflection (AR)-coated at 940 nm and had a high reflectivity at 1030 nm. The OC was partially-reflection-coated with a transmittance of T = 1, 5, and 10% at 1030 nm. An AR-coated ceramic Yb:YAG (CYb = 9.8 at.%, Konoshima Chemical) with dimensions of 5x10x1 mm3 was used. A 1-mm-thick Yb:YAG ceramic plate was wrapped with indium foil and mounted in a water-cooled copper block that acted as a heat sink. Water was maintained at a room temperature of 20ºC during laser oscillation. The cavity length was 20 mm, which was optimized, as shown in the later part of this section.
\n\t\t\t\t
Figure 2.
Input-output power dependence of efficient Yb:YAG (CYb = 9.8 at%) ceramic laser: (a) with output couplers of T = 1, 5, and 10%, and (b) only T = 10% (Nakamura et al., 2008b).
\n\t\t\t
\n\t\t\t
\n\t\t\t\t
2.2. Experimental results of linear cavity
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\n\t\t\t\t\tFigure 2(a) shows the output power as function of the absorbed pump power in the cases for the three transmittances of the output couplers T = 1, 5, and 10%, (Nakamura et al., 2008b) and Fig. 2(b) shows the output power as function of the absorbed pump power only for the case of T = 10%(Nakamura et al., 2008b). The absorbed pump powers at the lasing threshold were 1.2, 2.0, and 2.3 W, and the maximum output powers of 6.9, 6.9, and 6.8 W for T = 1, 5, and 10%, respectively, were obtained at the absorbed pump power of 13.8 W. The round trip loss L in the resonator was estimated to be 0.09 by the lasing thresholds and the reflectivity of the output couplers (Koechner, 1992), which resulted in a small signal gain g0 of 2.0 cm-1, and a single pass gain G of 1.2 with the 1 mm thick gain medium. Each linear line was fit in Fig. 2(a) for T = 1, 5, and 10%. The slope efficiencies ηslope were 60, 64, and 72% for T = 1, 5, and 10%, respectively. Since we considered that T = 10% is best for obtaining the highest slope efficiency of 72%, we filled the data for the T = 10% case to Fig. 2(b). The maximum output power of 6.8 W for T = 10% was obtained at the absorbed pump power of 13.8 W, indicating that the efficiency of converting pumping optical power to output optical power, ηopt-opt, was 49%. The line of the best fit is shown in Fig. 2(b). The slope efficiency ηslope was 72% for T = 10%. The maximum output power of 6.8 W was determined to be fourfold higher than 1.7 W and the slope efficiency was determined to be 7% lower than 79% using the 100 μm fiber-coupled LD reported by Dong et al. (Dong et al., 2006). Our 6.8 W laser with the slope efficiency of 72% is expected to have a higher slope efficiency than the present result if the pumping source is replaced with a 100 μm fiber-coupled 25 W LD, for example, LIMO25-F100-DL940 (Lissotschenko Mikrooptick) while maintaining the high output power, because the pumping intensity would increase to a value of fourfold higher than that of a 200 μm fiber-coupled LD. In comparing our laser with the edge-pumped composite Yb:YAG ceramic laser (Tsunekane & Taira, 2007) developed by Tsunekane and Taira, we limit our discussion to the cw case; the laser power of 414 W obtained by Tsunekane and Taira is much higher than our result, but their slope and optical-optical conversion efficiency were 47 and 44%, which were 25 and 5% lower than our slope and optical-optical conversion efficiency of 72 and 49%, respectively. The transverse intensity profile of the Yb:YAG ceramic laser beam is shown in Fig. 3. The intensity distribution indicates that the beam is a Gaussian beam (a TEM00 mode beam). The beam image in Fig. 3 was as stable as the pumping LD and we found no amplitude instability.
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Figure 3.
Transverse intensity profile of the Yb:YAG ceramic laser beam (Nakamura et al., 2008b). The intensity distribution indicates that the beam is a Gaussian beam (a TEM00 mode beam).
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These results of high output power, high efficiency, and good beam quality were obtained after the optimization of the cavity length. The cavity length was varied to obtain an optimum value for the highest efficiency and highest output power, and the focal length of the thermal lens for designing a tunable laser cavity configuration. Figure 4 shows the maximum output power as a function of the cavity length. Figure 4 shows that the optimum cavity length is less than 20 mm. This value is the appropriate cavity length for our laser, because there is no space to reduce the cavity length less than 20 mm. When we used the 400 μm fiber-coupled LD (Nakamura et al., 2008a), the optimum cavity length with the highest output power and highest slope efficiency was 25 mm, and reducing the length less than 25 mm yielded a worse result.
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Figure 4.
Maximum output power as function of cavity length of efficient Yb:YAG ceramic laser (Nakamura et al., 2008b).
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The focal length of the thermal lens in the ceramic Yb:YAG plate was considered for designing a tunable laser cavity configuration. Figure 4 also shows that the focal length of the thermal lens is 109 mm [120 mm (the cavity length) minus 11 mm (the distance of the ceramic Yb:YAG and the DM)], because the cavity becomes unstable, terminating the laser oscillation when the Fabry-Perot cavity length exceeds the thermal lens focal length. By considering this thermal lens, a tunable laser with a v-shape cavity including a concave mirror M (radius of curvature, ROC = 250 mm) and an SF10 dispersive prism was obtained, as shown in Fig. 5 in section 3.
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2.3. Summary of linear cavity
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A diode-end-pumped high-efficiency high-power Yb:YAG ceramic laser was demonstrated at a room temperature of 20ºC with an Yb concentration of 9.8 at.%, a gain medium thickness of 1 mm, a pumping power of 13.8 W, an output coupler of T = 10%, and a cavity length of 20 mm. A 6.8 W cw output power was obtained with a slope efficiency of 72%. This is the relatively high efficiency of ceramic Yb:YAG lasers at room temperature. The beam quality was shown as a transverse intensity distribution indicating a Gaussian beam (a TEM00 mode beam).
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3. Tunability of Yb:YAG ceramic laser
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3.1. Tunable Yb:YAG laser
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In previous reports on Yb:YAG ceramic lasers, no descriptions of the tunability of the lasers are given. However, there are some reports on the tunability of Yb:YAG crystal lasers. (Brauch et al., 1995), (Saikawa et al., 2000), (Saikawa et al., 2002) In 2000, the widest tunability range from 1024.1 to 1108.6 nm was demonstrated for a 160 mW Yb:YAG crystal laser using a 0.1% output coupler and a birefringent filter by Saikawa et al. (Saikawa et al., 2000) Subsequently, Saikawa et al. reported a 180 mW Yb:YAG crystal laser with a tunability in the spectral range of 59 nm from 1021.9 to 1081.2 nm in 2002. (Saikawa et al., 2002) Very recently, we have reported the first study of a tunable Yb:YAG ceramic laser (Nakamura et al, 2008b) that exhibits continuous tunability with a spectral range of 63.5 nm from 1020.1 to 1083.6 nm for T = 1% at a maximum output power of 1.6 W. In this section, we investigated the broader tunability range of a 1.4 W Yb:YAG ceramic laser using a 1% output coupler and a prism; this range was twofold broader than that in our previous work. (Nakamura et al, 2008b)
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Comparing the emission spectra of a Yb:YAG crystal (Dong et al., 2003) doped with 10 at.% Yb3+ and the ceramic Yb:YAG (Dong et al., 2006) with 9.8 at.% Yb3+ reported by Dong et al., we found that the ceramic Yb:YAG had a slightly higher emission intensity and the possibility of producing shorter-wavelength oscillation than the crystal Yb:YAG. To consider the difference in the emission spectra in the short-wavelength region, we employed a dichroic mirror (DM; Layertec No. 102927) with a high-reflectivity (HR) wavelength range from 1010 to 1200 nm and an antireflective range from 800 to 970 nm as a replacement for the previously used DM (Layertec No. 103542) (Nakamura et al, 2008b) with an HR range from 1020 to 1200 nm and an antireflective range from 808 to 980 nm. To the best of our knowledge, we obtained the broadest reported tunable range of 118.31 nm from 992.52 to 1110.83 nm for a Yb:YAG laser owing to this modification.
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Figure 5.
Experimental setup for tunable Yb:YAG ceramic laser (Nakamura et al., 2008b). LD: fiber-coupled diode laser; L1, L2: focusing lenses; DM: flat dichroic mirror; M; a concave mirror (ROC = 250 mm); OC: output coupler.
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3.2. Experimental setup of tunable Yb:YAG ceramic laser
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The experimental setup for the Yb:YAG ceramic laser is shown in Fig. 5. A 940 nm fiber-coupled LD (JENOPTIK Laserdiode JOLD-30-FC-12) was used as a pumping source; the fiber has a core diameter of 200 μm and a numerical aperture (NA) of 0.22. The pumping beam was focused onto the ceramic at a ratio of 1:1 using the lenses L1 (f = 25 mm) and L2 (f = 25 mm). The diameter of the spot focused on the ceramic was ~200 μm. A laser cavity consisting of a flat DM and a flat output coupler (OC) with a mirror M and an SF10 prism was used. The DM was antireflection (AR)-coated at 940 nm and had an HR at 1030 nm. In detail, we employed a DM (Layertec No. 102927) with an HR wavelength range from 1010 to 1200 nm and an AR range from 800 to 970 nm, which was a replacement for the previously used DM (Layertec, No. 103542) (Nakamura et al, 2008b) with an HR range from 1020 to 1200 nm and an AR range from 808 to 980 nm. The OC was partially reflection-coated with transmittances of T = 0.1, 1, 5, and 10% at 1030 nm. An AR-coated ceramic Yb:YAG (CYb = 9.8 at.%, Konoshima Chemical) with dimensions of 5x10x1 mm3 was used. The dimensions of the ceramics were selected to enable Brewster angled alignment for a mode-locked laser performance in future to reduce cost. A 1-mm-thick Yb:YAG ceramic plate was wrapped with indium foil and mounted in a water-cooled copper block that acted as a heat sink. The water was maintained at room temperature (20 ºC) during laser oscillation. By considering the thermal lens effect (Nakamura et al, 2008b), a tunable laser with a V-shape cavity including a concave mirror M (radius of curvature, ROC = 250 mm) and an SF10 dispersive prism was obtained, as shown in Fig. 5. The SF10 dispersive prism was inserted into a V-shape resonator as the tuning element between the folded mirror M and the output coupler OC at the Brewster angle. The cavity length was 315 mm.
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Figure 6.
Output power of ceramic Yb:YAG tunable laser as a function of oscillation wavelength for various output couplers (Nakamura et al., 2009).
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3.3. Experimental results of tunable Yb:YAG ceramic laser
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\n\t\t\t\t\tFigure 6 shows the dependence of output power on laser oscillation wavelength for output couplers of T = 0.1, 1, 5, and 10% when the absorbed pump power was 13.8 W. The averaged spectral linewidth of the output was 3.1 nm in these measurements. We achieved smoothly continuous tunability. A tunable range of 52.64 nm from 999.48 to 1052.12 nm was obtained with a maximum output power of 4.41 W at 1031.78 nm for T = 10%. A tunable range of 77.83 nm from 996.75 to 1074.58 nm and a maximum power of 3.63 W at 1034.14 nm were obtained for T = 5%. A maximum power of 1.40 W was obtained at 1033.42 nm and a tunable range of 104.52 nm from 994.35 to 1098.87 nm was obtained for T = 1%, which is broader than the tunability of 84.5 nm reported by Saikawa et al. (Saikawa et al., 2000). Finally, as shown in Fig. 6, T = 0.1% results in the largest tunable range of 118.31 nm from 992.52 to 1110.83 nm, which is broader than the tunability for T =1%, with a maximum output power of 163 mW at 1033.42 nm. To the best of our knowledge, this is the broadest tunability (Nakamura et al, 2009) reported for an Yb:YAG ceramic laser. The shortest wavelength of the tuning range in Fig. 6 is not limited to 1020 nm (Nakamura et al, 2008b) because of the broad dichroic coating range of the pumping mirror (Layertec No. 102927) with an HR wavelength range from 1010 to 1200 nm and an AR range from 800 to 970 nm. This tuning range of 118.31 nm for the Yb:YAG ceramic laser at 20 ºC or 293 K is 3.29-fold broader than the 36.0 nm tuning range, from 1018 to 1054 nm, which was produced from a Yb:YAG crystal laser with a three-plate birefringent filter at 218 and 245 K. (Brauch et al., 1995). Furthermore, our tuning range of 118.31 nm from 992.52 to 1110.83 nm for the high-power ceramic Yb:YAG laser at 20 ºC is twofold broader than that for the crystal Yb:YAG laser reported by Saikawa et al. (Saikawa et al., 2002), which has a tuning range of 59 nm from 1022 to 1081 nm at 18 ºC. The widely tunable Yb:YAG crystal laser with birefringent filters reported by Saikawa et al. (Saikawa et al., 2000) had a tuning range of 84.5 nm from 1024.1 to 1108.6 nm; however, the highest output power was 180 mW, which is much lower than the maximum output power of 1.4 W of our ceramic laser with an SF10 prism for T = 1%, and our tuning range of 104.52 nm for T = 1% is 1.24-fold broader than their 84.5 nm tunable range.
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Figure 7.
Expected transform limited pulses numerically obtained by inverse Fourier transformation of Fig. 6 for T = (a) 10, (b) 5, (c) 1, and (d) 0.1% (Nakamura et al., 2009).
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\n\t\t\t\t\tFigure 7 shows the expected transform-limited pulses obtained by an inverse Fourier transformation of Fig. 6 for T = (a) 10, (b) 5, (c) 1, and (d) 0.1%. The full width at half maximum (FWHM) of the numerically obtained pulse duration was tp = 65.0, 46.9, 35.3, and 31.2 fs for Figs. 7(a)-7(d), respectively. These numerical results suggest that the ceramic Yb:YAG laser medium has the potential for a laser performance of less than 65 fs.
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3.4. Summary of tunable Yb:YAG ceramic laser
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A diode-end-pumped broadly tunable Yb:YAG ceramic laser was demonstrated at room temperature (20 ºC) with Yb concentration of 9.8 at.%, a gain medium thickness of 1 mm, a pumping power of 13.8 W. Continuous tunability with a spectral range of 104.52 nm from 994.35 to 1098.87 nm for T = 1% at a maximum output power of 1.4 W and with a spectral range of 118.31 nm from 992.52 to 1110.83 nm for T = 0.1% at a maximum output power of 0.16 W was also obtained at room temperature. To the best of our knowledge, this is the broadest tunability reported for a Yb:YAG laser. This tunability is expected to be very attractive for femtosecond laser applications. Numerical results suggest that the ceramic Yb:YAG laser medium has the potential for a laser performance of less than 65 fs. The cost of Yb:YAG ceramic laser materials is much lower than that of single crystals because of their high-speed, large production, and mass production potential, is making them tremendously attractive for industrial applications.
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4. Mode-locked Yb:YAG ceramic laser
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4.1. Mode-locked Yb-doped lasers
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Femtosecond mode-locked lasers are applied in various fields of physics, engineering, chemistry, biology and medicine, with applications including ultrafast spectroscopy, metrology, superfine material processing and microscopy. Specific and interesting properties of the femtosecond laser pulses have been used in these applications. For example, femtosecond pulses have a very precise time resolution, and their strong electric field induces important and unusual nonlinear effects. For those applications, high-power, high-efficiency and compact femtosecond lasers are required. Ceramic materials are attractive for satisfying these requirements. YAG ceramics have 10% higher hardness than a YAG single crystal, and the fracture toughness of YAG ceramics is more than threefold that of the YAG single crystal. Therefore, the ceramics have a higher resistance to thermal shock than the single crystal. Ytterbium (Yb3+) also has interesting properties satisfying the above requirements. Its broad absorption and emission spectra allow the realization of a directly laser-diode (LD)-pumped femtosecond laser. Moreover, its small quantum defect, absence of excited-state absorption, upconversion and cross-relaxation reduce the thermal load and enable highly efficient operation. The emission and absorption spectra and thermal conductivity strongly depend on the host material.
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Recently, various ceramic materials have been progressively investigated for use in ultrashort-pulse lasers (Shirakawa et al., 2003), (Tokurakawa et al., 2006), (Shirakawa et al., 2003), (Tokurakawa et al., 2007), (Tokurakawa et al., 2008). A diode-pumped femtosecond Yb:Y2O3 ceramic laser was demonstrated, and 615 fs pulses at a center wavelength of 1076.5 nm were obtained with a 420 mW average power (Shirakawa et al., 2003). A diode-pumped passively mode-locked Yb:Lu2O3 ceramic laser was demonstrated, for which 357 fs pulses at a center wavelength of 1033.5 nm with a 352 mW average power were obtained (Tokurakawa et al., 2006). A passively mode-locked femtosecond Yb3+-doped Y3(Sc0.5Al0.5)2O12 (Yb:YSAG) ceramic laser pumped by a Ti:sapphire laser was also demonstrated, and 280 fs pulses at a center wavelength of 1035.8 nm with a 62 mW average power were obtained (Saikawa et al., 2007), but the laser was not diode-pumped. A diode-pumped Kerr lens mode-locked laser of Yb3+:Sc2O3 ceramics was demonstrated with 92 fs pulses at a center wavelength of 1042 nm and an 850 mW average power, and 90 fs pulses at a center wavelength of 1092 nm and a 160 mW average power (Tokurakawa et al., 2007). A diode-pumped Kerr lens mode-locked laser with Yb3+:Lu2O3 and undoped Y2O3 combined ceramics was demonstrated, and 65 fs pulses at a center wavelength of 1032 nm with a 320 mW average power were obtained (Tokurakawa et al., 2008). In previous reports on Yb:YAG ceramic lasers, there is no description of the mode locking of lasers. However, in some reports the femtosecond mode locking of Yb:YAG crystal lasers is discussed (Hönninger et al., 1999), (Aus der Au et al., 2000), (Neuhaus et al., 2008a), (Neuhaus et al., 2008b), (Uemura&Torizuka, 2008). The average power and pulse energy have been scaled up to 76 W and 25.9 μJ using a mode-locked thin-disk Yb:YAG laser (Neuhaus, 2008b). A Kerr lens mode-locked Yb:YAG crystal laser has been demonstrated, for which the pulse duration was as short as 100 fs at a center wavelength of 1051 nm (Uemura&Torizuka, 2008). The shortest pulse obtained using a diode-pumped ceramic laser without the Kerr lens effect was 357 fs (Tokurakawa et al., 2006).
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In this section, we report a diode-pumped passively mode-locked Yb:YAG ceramic laser generating 286 fs pulses with an average power of 25 mW at a wavelength of 1033.5 nm using a 0.1% output coupler. 233 fs pulses with an average power of 20 mW were also obtained at a center wavelength of 1048.3 nm using a 0.1% output coupler. To the best of our knowledge, this is the first demonstration of a diode-pumped mode-locked Yb:YAG ceramic laser and the shortest pulse using diode-pumped ceramic lasers without Kerr lens mode locking. In our previous studies as shown in section 3, we measured the broadest tunability of Yb:YAG ceramics at room temperature (RT) (Nakamura et al., 2008b), (Nakamura et al., 2009). This broad tunability indicates the possibility of sub-100-fs pulse generation using Yb:YAG ceramics.
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Figure 8.
Experimental setup of the mode-locked Yb:YAG ceramic laser (Yoshioka et al., 2009). LD: fiber-coupled diode laser. L1, L2: focusing lenses. M1-M4: high-reflectivity mirrors. OC1, OC2: output couplers. P1-P2: SF10 Brewster prisms. SESAM: semiconductor saturable absorber mirror. Dashed lines indicate the beam lines in cw operation. Solid lines indicate the beam lines in mode-locked operation.
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4.2. Experimental setup of mode-locked Yb:YAG ceramic laser
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The experimental setup for the mode-locked Yb:YAG ceramic laser is shown in Fig. 8. An x-fold cavity configuration was used. A 940 nm fiber-coupled LD was used as a pumping source. The core diameter of the fiber was 200 μm. The numerical aperture (NA) of the fiber was 0.22. The maximum pump power was 26.6 W. The pumping beam was imaged by relay to the ceramics using lens L1 (f = 50 mm) and lens L2 (f = 70 mm). The 1-mm-thick Yb:YAG (CYb = 9.8 at.%) ceramic plate was arranged at the Brewster’s angle. The Yb:YAG plate was wrapped with indium foil and mounted in a water-cooled copper heat sink block. The copper block was cooled by flowing water at 20 C. The ceramic was placed between two high-reflectivity mirrors (M1, M2) that were anti-reflection (AR)-coated at 940 nm and had high reflectivity at 1030 nm with a 100 mm radius of curvature (ROC). The reference laser operated in cw mode with a 10% output coupler (OC1) and a high-reflectance end mirror (M3) along the dashed lines in Fig. 8. For passive mode locking, a 1 or 0.1% output coupler (OC2) and a semiconductor saturable absorber mirror (SESAM, BATOP) with 2% saturable absorption at 1030 nm, 70 μJ/cm2 saturation fluence and 500 fs relaxation time constant were used in the respective arms. The total cavity length was 1620 mm. The laser beam was focused onto the SESAM by a concave mirror (M4, ROC = 250 mm). The distance among the mirrors and the folded angle of the mirrors are shown in Fig. 8. The astigmatism compensation was not considered. The spot sizes of laser mode in the laser crystal and on SESAM were estimated ~ 61 × 53 μm and ~ 450 × 330 μm, respectively. An SF10 Brewster prism pair (P1, P2) with 465 mm separation was inserted in the other arm to compensate for the dispersion. The total negative GDD of this cavity was about –2670 fs2 per a round trip.
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4.3. Experimental results of mode-locked Yb:YAG ceramic laser
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We demonstrated mode locking for three cases. The first case was mode locking at 1030 nm using a 1% output coupler. The second case was mode locking at 1030 nm using a 0.1% output coupler. The third case was mode locking at 1050 nm region with cw oscillation at 1030 nm region using a 0.1% output coupler.
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Figure 9.
a) Measured autocorrelation trace and the sech2 fitting, and (b) spectrum of the mode-locked pulses using a 1% output coupler (Yoshioka et al., 2009).
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4.3.1. Mode locking at 1030 nm region using a 1% output coupler
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\n\t\t\t\t\t\tFigure 9 shows the intensity autocorrelation trace and the spectrum of mode-locked pulses using a 1% output coupler. The average output power was 250 mW at a pump power of 26.6 W. The sech2-fitted pulse width was 417 fs and the spectral width was 3.02 nm at the center wavelength of 1033.3 nm, which results in a time-bandwidth product of 0.353, slightly above the Fourier limit for a sech2 pulse (0.315). The repetition rate was 91 MHz. The pulse energy and peak power were 2.75 nJ and 6.60 kW, respectively. When the 1% output coupler was used, mode locking at 1050 nm region was not observed but cw oscillation at 1050 nm region or simultaneous cw dual-wavelength oscillation at 1030 and 1050 nm was observed.
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4.3.2. Mode locking at 1030 nm region using a 0.1% output coupler
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\n\t\t\t\t\t\tFigure 10 shows the intensity autocorrelation trace and the spectrum of mode-locked pulses using a 0.1% output coupler. The average output power was 25 mW at a pump power of 26.6 W. The sech2-fitted pulse width was 286 fs and the spectral width was 4.51 nm, and centered at 1033.5 nm. This results in a time-bandwidth product of 0.363, which is 15% above the Fourier limit for a sech2 pulse (0.315). This indicates that the pulse has potential to be further shortened by extracavity compression. The repetition rate was 91 MHz. The pulse energy and peak power were 0.275 nJ and 0.960 kW, respectively. The pulse width of 286 fs obtained using a 0.1% output coupler (Fig. 10) was shorter than that of 417 fs obtained using a 1% output coupler (Fig. 9) because the intracavity power is increased using a 0.1% output coupler, which makes it possible for the laser to oscillate with a broad spectral range. However, the average output power decreased to 25 mW owing to the low transmission of the 0.1% output coupler.
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Figure 10.
a) Measured autocorrelation trace and the sech2 fitting, and (b) spectrum of the mode-locked pulses at 1030 nm region using a 0.1% output coupler (Yoshioka et al., 2009).
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4.3.3. Mode locking at 1050 nm region using a 0.1% output coupler
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When the SESAM angle was changed slightly from the conditions described in Sec. 4.3.2, mode locking at 1033.5 nm suddenly stopped and simultaneous cw dual-wavelength oscillation at 1030 and 1050 nm occurred. When the intensity of the cw spectral component at 1050 nm was increased and the laser mode radius focused on the SESAM was optimized, mode-locked pulses were generated again. Figure 11 shows (a) the intensity autocorrelation trace, (b) the spectrum of mode-locked pulses. The output spectrum in Fig. 11(b) was measured by injection into the fiber-coupled spectrometer directly from OC2. The average output power was 20 mW at a pump power of 26.6 W. The sech2-fitted pulse width was 233 fs and the spectral width was 5.20 nm and centered at 1048.3 nm, which results in a time-bandwidth product of 0.330, slightly above the Fourier limit for a sech2 pulse (0.315). The repetition rate was 91 MHz. The pulse energy and peak power were 0.220 nJ and 0.946 kW, respectively. Figure 12 shows a pulse train of cw mode-locking in millisecond time scale. This indicates that the mode-locked pulses had a long-term stability. The pulse width of 233 fs at 1048.3 nm in Fig. 11 obtained using a 0.1% output coupler was the shortest among these results. This indicates that the laser has the potential to generate shorter pulses at 1050 nm region rather than 1030 nm region. However, the cw spectral component at 1032.4 nm was not quenched in our cavity during mode locking at 1048.3 nm. This occurred owing to the strong emission at 1030 nm.
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Figure 11.
a) Measured autocorrelation trace and the sech2 fitting, (b) spectrum of the mode-locked pulses at 1050 nm region using a 0.1% output coupler (Yoshioka et al., 2009).
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Figure 12.
Pulse train of cw mode-locking in millisecond time scale (Yoshioka et al., 2009).
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4.4. Summary of mode-locked Yb:YAG ceramic laser
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A diode-pumped femtosecond ytterbium laser with a host material of YAG ceramic was demonstrated. We successfully achieved passive mode locking at wavelengths of 1033.5 and 1048.3 nm. At 1033.5 nm, passive mode locking by a semiconductor saturable absorber mirror generated 286 fs pulses with an average power of 25 mW using a 0.1% output coupler. This is the shortest pulse width in the 1030 nm region. At 1048.3 nm, the shortest pulse of 233 fs with an average output power of 20 mW was generated using a 0.1% output coupler. To the best of our knowledge, this is the first mode-locked Yb:YAG ceramic laser, and the shortest pulse for diode-pumped ceramic lasers without Kerr lens mode locking was obtained.
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5. Summary
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A high-power efficient ceramic Yb:YAG laser was demonstrated at a room temperature of 20 C with an Yb concentration of 9.8 at.%, a gain medium of 1 mm, a pumping power of 13.8 W, an output coupler of T = 10%, and a cavity length of 20 mm. A 6.8 W cw output power was obtained with a slope efficiency of 72%.
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A diode-end-pumped Yb:YAG ceramic laser with a broad tunability was demonstrated. The continuous tunability in the spectral range of 104.52 nm from 994.35 to 1098.87 nm for T = 1% at a maximum output power of 1.4 W and in the spectral range of 118.31 nm from 992.52 to 1110.83 nm for T = 0.1% at a maximum output power of 0.16 W was also obtained at room temperature. To the best of our knowledge, this is the broadest tunability of Yb:YAG lasers.
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A diode-pumped passively mode-locked Yb:YAG ceramic laser was demonstrated. 417 and 286 fs pulses with average powers of 250 and 25 mW were obtained at 1030 nm using 1 and 0.1% output couplers, respectively. 233 fs pulses with an average power of 20 mW were also obtained at a center wavelength of 1048.3 nm using a 0.1% output coupler. To the best of our knowledge, this is the first demonstration of a diode-pumped mode-locked Yb:YAG ceramic laser.
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\n\t\n',keywords:null,chapterPDFUrl:"https://cdn.intechopen.com/pdfs/8448.pdf",chapterXML:"https://mts.intechopen.com/source/xml/8448.xml",downloadPdfUrl:"/chapter/pdf-download/8448",previewPdfUrl:"/chapter/pdf-preview/8448",totalDownloads:4653,totalViews:349,totalCrossrefCites:2,totalDimensionsCites:5,totalAltmetricsMentions:0,impactScore:2,impactScorePercentile:73,impactScoreQuartile:3,hasAltmetrics:0,dateSubmitted:null,dateReviewed:null,datePrePublished:null,datePublished:"February 1st 2010",dateFinished:null,readingETA:"0",abstract:null,reviewType:"peer-reviewed",bibtexUrl:"/chapter/bibtex/8448",risUrl:"/chapter/ris/8448",book:{id:"3161",slug:"frontiers-in-guided-wave-optics-and-optoelectronics"},signatures:"Shinki Nakamura",authors:[{id:"4143",title:"Dr.",name:"Shinki",middleName:null,surname:"Nakamura",fullName:"Shinki Nakamura",slug:"shinki-nakamura",email:"shinki.nakamura.laser@vc.ibaraki.ac.jp",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",institution:{name:"Ibaraki University",institutionURL:null,country:{name:"Japan"}}}],sections:[{id:"sec_1",title:"1. Introduction",level:"1"},{id:"sec_2",title:"2. High-power and high efficiency Yb:YAG",level:"1"},{id:"sec_2_2",title:"2.1. Experimental setup of linear cavity",level:"2"},{id:"sec_3_2",title:"2.2. Experimental results of linear cavity",level:"2"},{id:"sec_4_2",title:"2.3. Summary of linear cavity",level:"2"},{id:"sec_6",title:"3. Tunability of Yb:YAG ceramic laser ",level:"1"},{id:"sec_6_2",title:"3.1. Tunable Yb:YAG laser",level:"2"},{id:"sec_7_2",title:"3.2. Experimental setup of tunable Yb:YAG ceramic laser",level:"2"},{id:"sec_8_2",title:"3.3. Experimental results of tunable Yb:YAG ceramic laser",level:"2"},{id:"sec_9_2",title:"3.4. Summary of tunable Yb:YAG ceramic laser ",level:"2"},{id:"sec_11",title:"4. Mode-locked Yb:YAG ceramic laser",level:"1"},{id:"sec_11_2",title:"4.1. Mode-locked Yb-doped lasers",level:"2"},{id:"sec_12_2",title:"4.2. Experimental setup of mode-locked Yb:YAG ceramic laser",level:"2"},{id:"sec_13_2",title:"4.3. Experimental results of mode-locked Yb:YAG ceramic laser",level:"2"},{id:"sec_13_3",title:"4.3.1. Mode locking at 1030 nm region using a 1% output coupler",level:"3"},{id:"sec_14_3",title:"4.3.2. Mode locking at 1030 nm region using a 0.1% output coupler ",level:"3"},{id:"sec_15_3",title:"4.3.3. Mode locking at 1050 nm region using a 0.1% output coupler",level:"3"},{id:"sec_17_2",title:"4.4. Summary of mode-locked Yb:YAG ceramic laser",level:"2"},{id:"sec_19",title:"5. Summary",level:"1"}],chapterReferences:[{id:"B1",body:'\n\t\t\t\t\n\t\t\t\t\t\n\t\t\t\t\t\t\n\t\t\t\t\t\t\tAus der\n\t\t\t\t\t\t\tAu. J.\n\t\t\t\t\t\t\n\t\t\t\t\t\t\n\t\t\t\t\t\t\tSpühler\n\t\t\t\t\t\t\tG. 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Express, 1\n\t\t\t\t\t1 Jan. 2008) id. 012007 (3 pages) 0021-4922\n\t\t\t\t\n\t\t\t'},{id:"B39",body:'\n\t\t\t\t\n\t\t\t\t\t\n\t\t\t\t\t\t\n\t\t\t\t\t\t\tYoshioka\n\t\t\t\t\t\t\tH.\n\t\t\t\t\t\t\n\t\t\t\t\t\t\n\t\t\t\t\t\t\tNakamura\n\t\t\t\t\t\t\tS.\n\t\t\t\t\t\t\n\t\t\t\t\t\t\n\t\t\t\t\t\t\tOgawa\n\t\t\t\t\t\t\tT.\n\t\t\t\t\t\t\n\t\t\t\t\t\t\n\t\t\t\t\t\t\tWada\n\t\t\t\t\t\t\tS.\n\t\t\t\t\t\t\n\t\t\t\t\t\n\t\t\t\t\t2009\n\t\t\t\t\tDiode-pumped mode-locked Yb:YAG ceramic laser.\n\t\t\t\t\tOpt. Express, 17\n\t\t\t\t\t11 Jun., 2009) 8919\n\t\t\t\t\t25 , 1094-4087\n\t\t\t\t\n\t\t\t'}],footnotes:[],contributors:[{corresp:"yes",contributorFullName:"Shinki Nakamura",address:null,affiliation:'
Ibaraki University, Japan
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1. Introduction
Porous media are defined as “materials containing very large numbers of pores with various sizes.” Owing to their characteristic large surface area, the porous media are used in various fields such as chemical plants, architecture, agriculture, environment, medical care, biology etc. In heat transfer engineering, which is one of this book’s topics, heat pipes [1] and vapor chambers [2] that utilize independent liquid supply based on the capillarity in a porous wick play an active part in the thermal management of electronic devices. For instance, thin heat pipes of <1 mm in thickness are even used in smartphones whose usage has witnessed an exponential increase [3]. In addition, in recent years, to cool electronic devices, two-phase immersion cooling with saturated pool boiling heat transfer has attracted attention for increasing the heat generation density and reducing the costs of thermal management. In particular, great numbers of studies have focused on improving the critical heat flux by loading a porous medium with a functional shape and structure onto the cooling surface, in addition to enhance the boiling heat transfer. It is recommended to refer to the review studies of Yuki [4], Mori [5, 6], and Kandlikar et al. [7]; however, there have been multiple studies that attempted to separate liquid supply and vapor discharge, such as the honeycomb porous plate of Mori et al. [8], the porous layers having a non-uniform spatial structure [9, 10, 11], and porous meshes provided with hydrophilic and hydrophobic functions [12, 13]. Note that the results of Bai et al. [14] and Yuki et al. [15] in which the critical heat flux of the saturated pool boiling of water in an atmospheric pressure environment exceeded 5 MW/m2, thus demonstrating the high potential of the porous media as a latent heat transport promoter. On the other hand, also for a single-phase flow, there have been a large number of attempts to utilize the porous media as a heat transfer promoter. The examples include heat transfer enhancement by metal foams [16, 17], utilization as a radiation converter [18, 19], and promotion of heat transfer using sphere-packed tubes [20, 21].
Focusing on high potential of the porous media as the heat transfer promoter as mentioned above, multiple studies have introduced porous metals for heat removal from high-heat flux equipment of a level of 10 MW/m2. For example, the divertor of a nuclear fusion reactor currently under research and development is exposed to a steady heat load of approximately 10 MW/m2 due to the inflow of α particles generated by nuclear fusion reaction. Sharafat et al. [22, 23] introduced metal foams as a heat transfer promoter of He gas flow pressurized to 40 MPa and demonstrated high cooling performance of >10 MW/m2. Furthermore, Joshi et al. proposed a cooling technology that makes use of the phase change of coolant in a pin-fins microchannel for high heat generation density electronic devices exceeding 10 MW/m2 [24, 25, 26]. Moreover, he attempted a technology that assists heat transfer in the promotion of evaporation in a nanoporous film via a gas impinging jet [27]. Regarding additional applications of the porous media under high heat flux conditions, refer to the review article by Smakulski et al. [28]. Obviously, in the thermal management of these high heat flux devices, in addition to securing the cooling performance, it is necessary to consider both economical efficiency and maintainability; therefore, thermal management with low flow rate and low pumping power is indispensable.
As an efficient heat removal technology at a level of 10 MW/m2, Toda and Yuki proposed a cooling device known as EVAPORON (Evaporated Fluid Porous-Thermodevice) to take maximum advantage of the latent heat of vaporization of the coolant [29, 30]. EVAPORON can remove extremely high heat flux by evaporating the cooling liquid that is fed inside the porous medium jointed to the heat transfer surface against a heat flow, using the vast surface area with microchannels of the porous media. Because rather than relying on capillarity such as in the heat pipes, a minimum amount of liquid corresponding to the heat flux level is gently pumped into the porous medium for cooling, a significant reduction in pumping power can then be expected. Furthermore, we verified that the important factor of this technological breakthrough is the quick discharge of considerable amounts of vapor generated in the porous medium [31]. Subsequently, the authors proposed EVAPORON-2 [32, 33] loaded with subchannels for vapor discharge within sintered copper particles and succeeded in the heat removal of over 20 MW/m2. Targeting at a cooling performance exceeding 10 MW/m2 under much lower pumping power conditions, furthermore, the EVAPORON-3 equipped with a vapor–liquid separator on the upper part of the porous medium was also proposed [34].
Figure 1.
Various kinds of porous media.
To summarize, when applying the porous media in the two-phase cooling technology for high heat flux environment, the most important factor is to actively promote the vapor discharge that was generated in the porous medium. Moreover, it is necessary to optimize the porous structure to maximize the advantage of the latent heat of vaporization of the coolant. On the other hand, there are various porous media such as foams, open cells, sintered particle/fiber, meshes etc. (see Figure 1), even if all of these are simply called porous metals. Generally, it is impossible to generalize the thermophysical properties and mechanical properties of the porous media with these different structures, thus referring only on their porosity and pore size. However, to promote phase change heat transfer in the porous medium, it is an undisputed fact that a porous medium with high permeability, which enables rapid discharge of the vapor generated, should be introduced in which its thermal conductivity is also increased to expand the effective heat transfer area. In general, there is a trade-off relationship between increasing the effective thermal conductivity and reducing the flow resistance of the vapor flow (increasing the permeability). Thus, the porous media to be introduced should be selected based on the heat flux level and coolant used. In this chapter, the effective thermal conductivity and absolute permeability for various porous media are first discussed. Subsequently, the effectiveness of unidirectional porous coppers [35] proposed by the author is quantitatively evaluated as a cooling technique on a level of 10 MW/m2. Finally, two our innovative cooling technologies are introduced; “EVAPORON-4”, which is the newest EVAPORON that combines the unidirectional porous copper and a grooved heat transfer surface and “Lotus’ Breathing”, which makes use of two-phase immersion cooling in a saturated pool boiling environment, based on spontaneous liquid supply effect called “Breathing phenomenon” proposed by the author for the first time all over the world.
2. Thermal conductivity and permeability of various porous media
Figure 2 shows the porosity and pore size distributions of sintered-metal-particles/fibers and foamed metals the author used to date. For example, regarding the thermal conductivity and the permeability of isotropic porous media with a simple structure, their modeling is frequently performed based on the porosity and the pore size for each porous medium. As shown in Figure 2, each porous medium has its characteristic porosity and pore diameter. For instance, most foamed metals and open cells have a high porosity of >90%. As far as the author knows, although those with a microscale pore diameter are not commercially available, Unno et al. developed the porous media with high porosity and micropores and demonstrated that it is effective for promoting evaporative heat transfer as per the capillary limit theory [36]. Multiple sintered-metal-particles have a porosity of 30%–50% because of the producing process and the packing structure; moreover, the pore diameter varies from the order of micron to millimeter. For sintered-metal-fibers (a kind of fibrous porous media), the porosity can be regulated over a wide range by the extent of pressing; however, it is difficult to control the orientation of the fiber. We will now discuss the effective thermal conductivity and permeability of these typical porous media from the view point of phase-change enhancement of coolant.
Figure 2.
Porosity and pore size of porous media.
2.1 Effective thermal conductivity of porous media
To discuss the effective heat transfer area, it is important to examine the effective thermal conductivity of the porous media. The prediction formulae for various porous structures have been developed to date; however, in general, the effective thermal conductivity keff of the porous media can be discussed based on the following parallel model weighted by the porosity.
keff=εkf+1−εksE1
where kf and ks are the thermal conductivity of the fluid phase in the pore and that of the porous solid phase, respectively. Note that both kf and ks do not express the thermal conductivity of the material itself but must be taken into account the tortuosity, which expresses the porous structure, and the thermal resistance affected by the degree of sintering, if speaking of a sintered metal. However, Eq. (1) clearly shows that the effective thermal conductivity of the porous media mostly depends on the porosity. For example, for copper-foamed metal with high porosity, if the fluid in the pore is air and the porosity is 0.9, the effective thermal conductivity is estimated to be somewhat <40 W/m/K; however, when estimated from the formula of Boomsma et al. [37], it is ~1 W/m/K. In fact, because the effective thermal conductivity decreases further, depending on the manufacturing method of foamed metals, the expansion of the heat transfer area by the fin effect cannot be expected, particularly for liquid cooling or two-phase immersion cooling. Therefore, the foamed metals and the open cells are often used for gas flows as mechanical dispersion promoters and turbulent promoters. On the other hand, in terms of sintered-metal-particles with a comparatively low porosity, the porous media with the porosity of <0.3 can be produced depending on the degree of sintering and pressing, so that high effective thermal conductivity can be expected. Furthermore, depending on the extent of sintering, the neck structure formed between the particles considerably affects the effective thermal conductivity. As for the fibrous porous media, although the sintered-metal-fibers have high thermal conductivity in the fiber direction, the effective thermal conductivity is assumed to be almost the same as that of the sintered-metal-particles in the direction perpendicularly to the fiber direction.
Herein, as shown in Figure 3, we performed heat conduction simulation to estimate the effective thermal conductivity of the sintered-copper-particle, in which a cubic sintered-copper-particle with a side length of 5 mm is sandwiched between copper square rods of 5 × 5 × 50 mm3. At the lower end surface, the heat flux of 0.5 MW/m2 is exposed and a constant temperature of 100 °C is given to the upper end surface. Adiabatic conditions are attributed to the side surfaces of the rods and sintered-particles. The effective thermal conductivity of the sintered-copper-particle is evaluated using the Fourier law from the difference in the average temperature at the two interfaces between the copper square rod and the sintered particle. The particle size is 1.0 mm and packed structure of particles is a simple cubic structure. To reproduce the neck structure formed between the particles during sintering, a cylinder with a diameter of d is virtually installed around the contact point between the particles, i.e., the diameter of the cylinder is the neck structure at the time of sintering in a pseudo presentation, and d is determined with the contact angle θ as a parameter. In this calculation, contact angles are 5°, 10°, and 20°. The same is valid for contact between the particles and the end surface of the rods. The porosity at a contact angle of 0° is 0.48. Assuming pure copper, the solid phase has a thermal conductivity of 398 W/m/K; moreover, the air in the pore has a thermal conductivity of 0.026 W/m/K. The heat conduction simulation is performed using Stream v13 developed by Cradle, which adopts the finite volume method (FVM); for comparison, the calculation using the finite element method (FEM) is performed at the same time. Because these simulations do not apply any special model for the discretization of the equation of heat conduction, the effective thermal conductivity of the sintered-particle can be evaluated with a higher accuracy than with experiments. Figure 4 shows the results of the simulation. The effective thermal conductivity at contact angles of 5°, 10°, and 20°is 7.8, 19.2, and 45.9 W/m/K, respectively. Obviously, a higher degree of sintering involves higher effective thermal conductivity. However, compared with the bulk thermal conductivity of pure copper, it is reduced to 2% – 4% of the thermal conductivity of the Cu material at a contact angle of 5°; even if the contact angle is 20°, which is the highest degree of sintering, the effective thermal conductivity is reduced to ~12% of the Cu material. The difference from the effective thermal conductivity represented by the parallel model of Eq. (1) is apparent. The abovementioned results verify the necessity to carefully consider the fin effect even when utilizing the sintered-copper-particles due to its low thermal conductivity.
Figure 3.
Calculation of effective thermal conductivity for particle-sintered porous medium.
Figure 4.
Effective thermal conductivity of particle-sintered porous medium.
On the other hand, to maximize the effective thermal conductivity of the porous media, a porous medium to which the parallel model of Eq. (1) can be applied is desirable. This indicates that the introduction of a porous medium with unidirectional pore structure is ideal. Its thermal conductivity differs between the direction of the pores (keff||) and the direction perpendicular thereto (keff⊥); they can be predicted from the following equations by Ogushi et al. [38].
keff∥=1−εksE2
keff⊥=β+1+εβ−1β+1−εβ−1ksE3
The abovementioned equation is driven by adapting the Behrens’ thermal conductivity model for composite material to the unidirectional porous media. Because the fluid in the pore is assumed to be a gas and its thermal conductivity can be ignored, Eq. (2) corresponds to the parallel model. β is the thermal conductivity ratio. At the same porosity of 0.48 as in the sintered-particle, the effective thermal conductivity in the pore direction is 220 W/m/K, which is more than five times higher than that of the sintered-particle. When developing cooling devices for a high heat flux equipment, if the pore direction of the unidirectional porous media agrees with the heat flow direction, the effective heat transfer area potential of the porous media can be maximized. With regard to the effective thermal conductivity in the direction perpendicular to the pores, the thermal conductivity simulation as shown in Figure 3 is also performed on the unidirectional porous media as shown in Figure 5 whereby the effective thermal conductivity is predicted more accurately. In this simulation, the pores are arranged in two patterns, i.e., a square array and a staggered array, and the porosity is adjusted while changing the pore diameter from 0.1 to 1.9 mm without changing the pore position. As understood from Figure 6, the unidirectional porous media exhibits a similarly high thermal conductivity even in the direction perpendicular to the pores because the effective thermal conductivity with the porosity of 0.5 exceeds 100 W/m/K. Moreover, the higher the porosity, the larger the deviation of the effective thermal conductivity from the model of Chiba et al. For example, if the porosity is 0.7, the error is ~35% for the square array and ~ 42% for the staggered array. By grasping the effective thermal conductivity, it becomes possible to discuss the fin efficiency of the porous media. Chiba et al. developed a highly accurate model formula [39], which enables the easy evaluation of the criteria for introducing the unidirectional porous media.
Figure 5.
Square array model and staggered array model for uni-directional porous media.
Figure 6.
Effective thermal conductivity keff⊥ of uni-directional porous media.
2.2 Permeability of porous media
As mentioned above, to effectively use the latent heat of vaporization in a high heat flux environment, a large amount of vapor generated in the porous medium must be quickly discharged to the outside. In other words, it is indispensable to take a mean, including introducing the porous media with high permeability or modifying the spatial structure while considering the improvement in effective thermal conductivity discussed in the previous section. Here, for reference, a simple comparison of the absolute permeability K of the sintered-particle and the foamed metal from the Kozeny–Carman Eq. K = d2ε3/180/(1-ε)2 demonstrates that the permeability of the foamed metals is by two orders of magnitude higher than that of the sintered-particles, which clearly shows outstanding fluid fluidity and vapor discharge performance. However, as we have already understood from the discussion on the effective thermal conductivity, if the foamed metal is used as the phase change promoter, the phase change within the porous medium cannot be expected because of the low effective thermal conductivity, i.e., boiling/evaporation is expected to occur only on the heat transfer surface or in its immediate neighborhood. As for the sintered-particles, complicated microchannels with repeated expanded and contracted portions can be considered particularly suitable for the phase change because a thin liquid film can be formed at the contracted portion. Because of an extremely large pressure loss for the sintered-particles compared to that for the foamed metals, however, it is difficult to smoothly discharge large amounts of vapor from the porous medium, particularly under high heat flux conditions of 10 MW/m2 level. If the upstream pressure of high-speed vapor flow exceeds a pumping pressure/an inlet pressure shortly before the porous medium, the vapor phase near the heat transfer surface particularly starts to excessively grow and form a thermal resistance layer that quickly deteriorates the heat transfer performance. In fact, in the heat transfer tests by the author in which the sintered-metal-particles and the sintered-metal-fibers were used, such phenomena have been confirmed that the heat transfer performance of the porous media with higher permeability is reversed under high heat flux conditions exceeding several MW/m2 [31, 40]. It is effective to yield a multiple structure to the porous medium (e.g., biporous structure at the lower right of Figure 1) to provide a path for vapor discharge, however, it is extremely important to reduce the flow resistance in the porous medium because the vapor is first generated within the porous medium. In fact, the use of microchannels is also important in this technology as we want to promote evaporative heat transfer [41]. Therefore, effecting compromise with curved flow paths such as in the sintered-particles and introducing unidirectional porous media provide powerful means to improve the permeability. Here, to evaluate the permeability of the unidirectional porous media, the absolute permeability is modeled based on the Darcy–Weithbach equation, which gives the pressure loss of a circular pipe flow (the inflow resistance to the porous medium and the outflow resistance are ignored).
K=εdp2/32E4
Figure 7 shows the permeability of the sintered-particles and the unidirectional porous media. The horizontal axis is the porosity with a characteristic length dp of 100 μm (corresponding to the particle diameter for the sintered-particles and the pore diameter for the unidirectional porous media). Indeed, with increase in porosity, the permeability increases; however, for example, if the porosity is 0.3, 0.4, and 0.5, the permeability ratios of the unidirectional porous media and the sintered-particles are 30.6, 12.7, and 5.6 times, respectively. This ratio does not depend on the characteristic length. In other words, when focusing on the porous structure, the unidirectional porous media can be considered as the one that offers the best compromise between the improvement of the thermal conductivity and the improvement of the permeability. An example of application is a fibrous wick manufactured by sintering fibers, which considerably reduces the flow resistance in the fiber direction to contribute to the improvement in the maximum heat transport capacity of small heat pipes [3].
Figure 7.
Permeability of unidirectional porous.
2.3 Other heat transfer-related issues for introducing porous media
An important issue when introducing the porous media as a heat transfer promoter is the contact thermal resistance generated at the contact interface between the porous medium and the heat transfer surface. In general, with increasing heat flux, the temperature gap increases due to the increase in contact thermal resistance generated at the interface, so that the heat transfer coefficient is directly affected. For instance, when a sintered-particle is mechanically pressed to the heat transfer surface, a large contact thermal resistance is generated because of the point contact state between the heat transfer surface and the particles. In the point contact state, the heat conduction to the first particle is considerably deteriorated, so that boiling and evaporation occur mainly on the heat transfer surface or the first several layers of the particle, and thus, effective utilization of latent heat of vaporization inside the porous medium cannot be expected. The best measure is sintering the sintered-particle to the heat transfer surface. Remarkable research results are reported by Kibushi et al. [42] regarding the contact thermal resistance in a high heat flux environment exceeding 1 MW/m2 (for the experimental details refer to the reference). Figure 8 shows the temperature gap that occurs at the contact interface of two flat surfaces. The loads on a jointing surface of ϕ10 mm are 0.33, 1.71, and 3.03 MPa, and there are the two patterns of mechanical and solder joints. Focusing on the heat flux of 2 MW/m2, in the mechanical joint case, a temperature difference of ~40 K occurs under a load of 3.03 MPa, and a temperature gap exceeding 100 K takes place at the load of 0.33 MPa. However, it can also be confirmed that the contact thermal resistance is significantly improved by solder bonding. At the heat flux of 5 MW/m2, the temperature gap is ~10 K, and it is ~20 K upon linear extrapolation to 10 MW/m2. Accordingly, it is evident that when the porous medium is loaded on the heat transfer surface, the contact thermal resistance should be reduced by solder bonding or the like. Our heat transfer tests regarding a gas impinging jet flow into a sintered-particle verified that the heat transfer coefficient is spectacularly increased by soldering the porous medium to the heat transfer surface [43]. Further, the pool boiling results by Peterson et al. [44] have also demonstrated that boiling heat transfer is dramatically enhanced by HIP bonding of the porous medium to the heat transfer surface.
Figure 8.
Temperature gap due to contact thermal resistance.
For introducing the unidirectional porous media proposed this time, if the pores that serve as the flow path are parallel to the heat transfer surface, a perfect surface contact state can be achieved over the entire heat transfer surface. Furthermore, even if the pores are perpendicular to the heat transfer surface, the surface contact state can be maintained in the solid phase portion, which can maximally reduce the contact thermal resistance between the porous medium and the heat transfer surface.
2.4 Introduction of unidirectional porous copper
A majority of unidirectional porous media proposed in this study is generally fabricated by electric discharge machining or MEMS. As the production with these techniques is very expensive, it is desirable to introduce the unidirectional porous media with excellent mass productivity. Here, three unidirectional porous media are presented, which are currently introduced to the author’s laboratory. The first is the lotus copper shown in Figure 9(a), in which pores are formed utilizing different saturation degree of dissolved hydrogen existing in molten copper with temperature gradient [45]. Chiba et al. already demonstrated its superiority in single-phase flow heat transfer [46]. The boiling heat transfer enhancement technology that the author is currently developing in cooperation with Lotus Thermal Solutions Co., Ltd. will be introduced in the next section. Hokamoto et al. also proposed a technique for forming a group of thin metal tubes into a unidirectional porous tube by exploded welding technique (Figure 9(b) [47]). To date, the author has introduced unidirectional porous copper tubes as a heat transfer promoter of a gas flow in a joint research with Hokamoto et al. of Kumamoto University. Based on single-phase flow heat transfer tests, the unidirectional porous tubes of 21 mm in outer diameter shows a heat transfer performance that is up to approximately eight times higher than that of a smooth tube at the maximum as shown in Figure 9(c) [48]. The pore size and the porosity of this porous tube can be adjusted by varying the inner diameter and wall thickness of the thin tube. The lastly introduced unidirectional porous copper is the one molded by a metal 3D printing technique [49]. Recent advances in 3D printing technology enabled the molding of even porous media composed of copper and having microchannels. The adjustment of the pore diameter and the pore structure matching the heat transfer mechanism are possible, which is the greatest attraction of this technology.
Figure 9.
Unidirectional porous media ((a) lotus copper, (b) exploded welded porous pipe) and (c) heat transfer performance of a gas flow in exploded welded porous pipes & its CFD simulation.
On the other hand, when this type of unidirectional porous copper is applied as a promoter of boiling/evaporation heat transfer, particularly if the pores are perpendicular to the heat transfer surface, one of the advantages is that the coolant can surely be supplied to the heat transfer surface. The major limitation is how to rapidly discharge a large amount of vapor generated in the porous medium to the outside. As a solution, we propose to joint the unidirectional porous copper to the grooved heat transfer surface; thus, as shown in Figure 10, two cooling structures are enabled. The first structure on the left shows the liquid supply direction is opposite to the vapor discharge direction, whereas the second structure on the right shows a method of directly discharging the vapor outside the porous medium via these grooves. In the next section, we will focus on the cooling performance related to flow boiling heat transfer and pool boiling heat transfer using these cooling structures.
Figure 10.
Two heat removal devices proposed.
3. Enhancement of flow boiling and pool boiling heat transfers using unidirectional porous copper
3.1 Enhancement of flow boiling/evaporative heat transfer with EVAPORON-4
As mentioned in the Introduction, the author proposed EVAPORON, EVAPORON-2, and EVAPORON-3, cooling devices using porous metals [29, 30, 31, 32, 33, 34]. The porous metal is connected to the cooling surface as shown in Figure 11, the cooling liquid is supplied into the porous medium in a countercurrent to the heat flow, and the heat is removed by the vigorous phase change of the cooling liquid within. To smoothly discharge the large amount of vapor outside the porous medium, EVAPORON-2 has several subchannels inside the porous medium, and EVAPORON-3 has a liquid–vapor-separator on the porous medium. Here, the concept of cooling device EVAPORON-4, using a unidirectional porous media is realized as shown in Figure 12(a). As shown in Figure 12(b), 9 × 5 grooves for the vapor discharge are formed on the heat transfer surface, and the unidirectional porous copper shown in Figure 12(c) is joined by soldering. The groove is 1.0 mm in width and 0.5 mm in depth. The unidirectional porous copper with a diameter of 20 mm and a thickness of 10 mm is produced by machining and has 248 small pores of ϕ0.5 mm in diameter. In addition, the porous medium has large five ϕ2.6 mm holes for the vapor discharge. EVAPORON-4 is a once-through type cooling device in which the cooling liquid supplied from the upper part of the unidirectional porous copper through the small pores undergoes phase change in the pores and the grooves to be then discharged through the grooves and the vapor discharging large holes. Figure 13 shows some of the results in two cases that the unidirectional porous copper is jointed onto the heat transfer surface with/without soldering (“Without TIM (Thermal Interface Material)” shows the data of mechanical joint without bonding). For details of the experimental apparatus and various results, please refer to Reference [50]. The inlet liquid subcooling of distilled water is 40 K, whereas the x mark on the plot shows that the obtained data represent the critical heat flux. From this figure, the data with soldering move to the lower wall-superheat side under each flow rate condition, which verifies that the phase change heat transfer is enhanced by solder bonding the porous copper to the grooved heat transfer surface. Focusing on the data obtained at the flow rate of 0.5 L/min, while the critical heat flux without solder bonding is ~3 MW/m2, the critical heat flux is improved to exceed 6 MW/m2 by solder bonding (1.8-fold enhancement). For the flow rate of 2.0 L/min, as the maximum heat flux (not the critical heat flux) without solder bonding is approximately 9 MW/m2, the critical heat flux by solder bonding is expected to exceed 10 MW/m2, though the experiment was stopped due to the temperature limit of the cartridge heaters we used. For reference, the measured critical heat flux of the impinging jet at the flow rate of 2.0 L/min is approximately 4 MW/m2 (the same flow rate is ejected from a hole of ϕ2 mm), so that the cooling performance of EVAPORON-4 is much higher compared with other cooling technologies. These results are attributed to the effective functioning of the phase change within and the vapor discharge outside the porous medium, because the heat transfer is remarkably improved under high heat flux conditions.
Figure 11.
From the left: EVAPORON, EVAPORON-2, and EVAPORON-3.
Figure 12.
Outline of EVAPORON-4.
Figure 13.
Boiling curves of EVAPORON-4.
Currently, we are examining the flow rate distribution and the phase change in porous media by CFD and visualization experiments. From now onward, we intend to push forward discussions and optimization by introducing the porous copper fabricated by a 3D metal printer, as shown in Figure 14, thus comprising the un-uniform unidirectional pore and groove structures that can make maximum use of the latent heat of vaporization [49]. Moreover, we are examining a small-sized cold plate having in mind an application to electronic devices, a theme to be referred to in Reference [51].
Figure 14.
Unidirectional porous copper fabricated by 3D printing technique.
3.2 Enhancement of critical heat flux of saturated pool boiling using lotus coppers by “breathing phenomenon”
In the past heat transfer experiments using EVAPORONs, the author noticed that the inlet pressure of the fluid rapidly decreases when the phase change in the porous medium is considerable and the vapor is vigorously ejected to the outside, i.e., there must be spontaneous liquid supply phenomenon associated with the discharge of vapor (henceforth referred to as “Breathing Phenomenon”). As shown in Figure 15, the author has proposed to attach a porous plate called “lotus copper” with a unidirectional pore structure to the grooved heat transfer surface (Figure 9(a)), whereby the critical heat flux of saturated pool boiling is spectacularly increased [15, 52, 53, 54]. This two-phase immersion cooling technique we usually call “Lotus’ Breathing” offers the following features.
Spontaneous liquid supply phenomenon due to vapor blowout (Breathing Phenomenon)
No requirement of capillarity induced in the porous medium
Once-through type liquid supply and vapor discharge (Figure 15). Liquid supply and vapor discharge are separated and formation of coalesced bubbles is retarded.
Use of a unidirectional porous copper with high permeability and high thermal conductivity to enhance the breathing phenomenon and the heat transfer in the porous medium.
Figure 15.
Breathing phenomenon spontaneously induced by lotus copper on a grooved heat transfer surface ((a) mode-G, (b) mode-L).
There are two possible breathing modes “Mode-G” and “Mode-L”, as in Figure 15(a) and (b), i.e., the Mode-G on the left in which the vapor is discharged from the groove and accordingly the liquid is supplied from the upper part of the porous medium as well as the inverse mode-L.
To demonstrate the increase in CHF by the breathing phenomenon, saturated pool boiling experiments have been conducted in an atmospheric pressure environment. For details of the experiment, please refer to Reference [15]. The Lotus copper plate (10 mm x 10 mm, thickness = 2 mm, porosity = 65.9%, and average pore diameter = 0.49 mm) is attached to a 10 mm × 10 mm heat transfer surface provided with 0.5 mm-square or 1.0 mm-square unidirectional grooves as a boiling heat transfer surface. The results for water and FC72 are shown in Figure 16. In the case of water, the critical heat flux for the smooth surface in this device is 1.4 MW/m2, which is an adequate value for a boiling heat transfer experiment using the heat transfer block. The results also verify that the critical heat flux when utilizing the lotus copper jointed on the grooved heat transfer surface considerably improves by providing wider grooves. The 0.5 mm-square groove achieves the critical heat flux of 4.6 MW/m2 at the wall superheat of 58.9 K, and the one of 1.0 mm-square groove achieves the critical heat flux of 5.3 MW/m2 at the wall superheat of 111 K, which indicates that the groove size is an important factor for improving the critical heat flux by the breathing phenomenon. The boiling heat transfer is also remarkably enhanced even if compared to that for the smooth surface; this technology has proven to achieve both the enhancement of the boiling heat transfer and the critical heat flux. By visualizing the boiling phenomenon shortly before the critical heat flux, a large amount of vapor is discharged from the grooves. Thus, the breathing phenomenon in these experiments conceivably corresponds to the Mode-G of Figure 15(a). On the other hand, in the FC72 case, the maximum heat flux, which is not the critical heat flux, is 0.83 (MW/m2) that is 5.5 times higher than CHF of the smooth surface. This result verifies that the breathing phenomenon can work for dielectric fluid and increases the critical heat flux.
Figure 16.
CHF improvement by breathing phenomenon (left: Water, right: FC72).
Currently, the mechanism of critical heat flux enhancing and the factors that further entails the breathing phenomenon are being discussed based on the visualization experiment and CFD simulation as shown in Figure 17. In addition, the effects of varying the porosity, the pore size of the lotus copper, and the groove structure have been evaluated [55, 56].
Figure 17.
Example of CFD simulation and visualization experiment of breathing phenomenon.
4. Conclusion
In this chapter, the thermal conductivity and permeability of various porous media were quantitatively evaluated; as one of the porous media appropriate for high heat flux heat removal, targeted by the author, the introduction of “porous metal with unidirectional pores” was strongly suggested. Furthermore, as an application of using unidirectional porous coppers, we demonstrated the cooling performance of the flow boiling/evaporation cooling device EVAPORON-4, and that of the pool boiling enhancing technology “Lotus Cooler” based on “Breathing Phenomenon”. From now onward, we intend to optimize the structure of the unidirectional porous media and the grooved heat transfer surface, thus aiming at improving and controlling the performance of these cooling technologies.
\n',keywords:"unidirectional porous metal, cooling, high heat flux, permeability, effective thermal conductivity, heat transfer, phase change, EVAPORON, lotus’ breathing",chapterPDFUrl:"https://cdn.intechopen.com/pdfs/76260.pdf",chapterXML:"https://mts.intechopen.com/source/xml/76260.xml",downloadPdfUrl:"/chapter/pdf-download/76260",previewPdfUrl:"/chapter/pdf-preview/76260",totalDownloads:274,totalViews:0,totalCrossrefCites:1,dateSubmitted:"September 18th 2020",dateReviewed:"February 12th 2021",datePrePublished:"April 13th 2021",datePublished:"August 18th 2021",dateFinished:"April 13th 2021",readingETA:"0",abstract:"In this chapter, new heat transfer enhancement technologies with unidirectional porous metal called “EVAPORON” and “Lotus’ Breathing” are introduced to remove and manage heat from high heat flux equipment. The unidirectional porous metals introduced here can be easily fabricated by unique techniques such as mold casting technique, explosive welding technique, and 3D printing technique. First of all, many kinds of porous media, which have been introduced by the author so far as a heat transfer promoter, are compared each other to clarify what kind of porous metal is more suitable for high heat flux removal and cooling by focusing on the permeability and the effective thermal conductivity. For the practical use of the unidirectional porous copper with high permeability and high thermal conductivity, at first, heat transfer performance of two-phase flow cooling using a heat removal device called “EVAPORON” is reviewed aiming at extremely high heat flux removal beyond 10 MW/m2. We have been proposing this device with the unidirectional porous copper fabricated by 3D printing technique as the heat sink of a nuclear fusion divertor and a continuous casting mold. Second, two-phase immersion cooling technique called “Lotus’ Breathing” utilizing “Breathing Phenomenon” is introduced targeting at thermal management of various electronics such as power electronics and high performance computers. The level of the heat flux is 0.1 MW/m2 to 5 MW/m2. In addition, as the other heat transfer enhancing technology with unidirectional porous metals, unidirectional porous copper pipes fabricated by explosive welding technique are also introduced for heat transfer enhancement of single-phase flow.",reviewType:"peer-reviewed",bibtexUrl:"/chapter/bibtex/76260",risUrl:"/chapter/ris/76260",signatures:"Kazuhisa Yuki",book:{id:"10284",type:"book",title:"Porous Fluids",subtitle:"Advances in Fluid Flow and Transport Phenomena in Porous Media",fullTitle:"Porous Fluids - Advances in Fluid Flow and Transport Phenomena in Porous Media",slug:"porous-fluids-advances-in-fluid-flow-and-transport-phenomena-in-porous-media",publishedDate:"August 18th 2021",bookSignature:"Vallampati Ramachandra Prasad",coverURL:"https://cdn.intechopen.com/books/images_new/10284.jpg",licenceType:"CC BY 3.0",editedByType:"Edited by",isbn:"978-1-83962-712-5",printIsbn:"978-1-83962-711-8",pdfIsbn:"978-1-83962-722-4",isAvailableForWebshopOrdering:!0,editors:[{id:"146601",title:"Dr.",name:"Vallampati",middleName:null,surname:"Ramachandra Prasad",slug:"vallampati-ramachandra-prasad",fullName:"Vallampati Ramachandra Prasad"}],productType:{id:"1",title:"Edited Volume",chapterContentType:"chapter",authoredCaption:"Edited by"}},authors:[{id:"331620",title:"Prof.",name:"Kazuhisa",middleName:null,surname:"Yuki",fullName:"Kazuhisa Yuki",slug:"kazuhisa-yuki",email:"kyuki@rs.socu.ac.jp",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",institution:null}],sections:[{id:"sec_1",title:"1. Introduction",level:"1"},{id:"sec_2",title:"2. Thermal conductivity and permeability of various porous media",level:"1"},{id:"sec_2_2",title:"2.1 Effective thermal conductivity of porous media",level:"2"},{id:"sec_3_2",title:"2.2 Permeability of porous media",level:"2"},{id:"sec_4_2",title:"2.3 Other heat transfer-related issues for introducing porous media",level:"2"},{id:"sec_5_2",title:"2.4 Introduction of unidirectional porous copper",level:"2"},{id:"sec_7",title:"3. Enhancement of flow boiling and pool boiling heat transfers using unidirectional porous copper",level:"1"},{id:"sec_7_2",title:"3.1 Enhancement of flow boiling/evaporative heat transfer with EVAPORON-4",level:"2"},{id:"sec_8_2",title:"3.2 Enhancement of critical heat flux of saturated pool boiling using lotus coppers by “breathing phenomenon”",level:"2"},{id:"sec_10",title:"4. 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Kandlikar, Review of the manufacturing techniques for porous surfaces used in enhanced pool boiling, Heat Transfer Engineering, 35, No. 10, pp.887-902 (2014)'},{id:"B8",body:'Shoji Mori, Kunito Okuyama, Enhancement of the critical heat flux in saturated pool boiling using honeycomb porous media, International Journal of Multiphase Flow, 35, 10, pp. 946-951 (2009)'},{id:"B9",body:'Md Mahamudur Rahman, Emre Ölçeroğlu, and Matthew McCarthy, Role of wickability on the critical heat flux of structured superhydrophilic surfaces, Langmuir, 30, 37, pp. 11225-11234 (2014)'},{id:"B10",body:'Calvin H. Li, T. Li, Paul Hodgins, Chad N. Hunter, Andrey A. Voevodin, John G. Jones, G.P. Peterson, Comparison study of liquid replenishing impacts on critical heat flux and heat transfer coefficient of nucleate pool boiling on multiscale modulated porous structures, International Journal of Heat and Mass Transfer, 54, 15-16, pp. 3146-3155 (2011)'},{id:"B11",body:'Scott G Liter, Massoud Kaviany, Pool-boiling CHF enhancement by modulated porous-layer coating: theory and experiment, International Journal of Heat and Mass Transfer, 44, 22, pp. 4287-4311 (2001)'},{id:"B12",body:'Xianming Dai, Xinyu Huang, Fanghao Yang, Xiaodong Li, Joshua Sightler, Yingchao Yang, and Chen Li, Enhanced nucleate boiling on horizontal hydrophobic-hydrophilic carbon nanotube coatings, Applied Physics Letters 102 (16), 161605 (2013)'},{id:"B13",body:'Xianming Dai, Pengtao Wang, Fanghao Yang, Xiaochuan Li, and Chen Li, Decoupling the influence of surface structure and intrinsic wettability on boiling heat transfer, Applied Physics Letters, 112, 253901 (2018)'},{id:"B14",body:'Lizhan Bai, Lianpei Zhang, Guiping Lin, and G. P. Peterson, Pool boiling with high heat flux enabled by a porous artery structure, Applied Physics Letters, 108, 233901 (2016)'},{id:"B15",body:'Kazuhisa Yuki, Risako Kibushi, Rikako Tsuji, Kio Takai, Noriyuki Unno, Tetsuro Ogushi, Masaaki Murakami, Tomiyuki Numata, Hikaru Nomura, Takuya Ide, Thermal management of auto motive SiC-based on-board inverter with 500 W/cm2 in heat flux, and Two-phase immersion cooling by breathing phenomenon spontaneously induced by lotus porous copper jointed onto a grooved heat transfer surface, Journal of Thermal Science and Technology, Vol.15, No.1, Paper No.20-00051 (2020)'},{id:"B16",body:'Shadi Mahjoob, KambizVafai, A synthesis of fluid and thermal transport models for metal foam heat exchangers, International Journal of Heat and Mass Transfer, 51, 15-16, pp. 3701-3711 (2008)'},{id:"B17",body:'Z.F. Huang, A. Nakayama, K. Yang, C. Yang, W. Liu, Enhancing heat transfer in the core flow by using porous medium insert in a tube, International Journal of Heat and Mass Transfer, 53, 5-6, pp. 1164-1174 (2010)'},{id:"B18",body:'Kouichi Kamiuto, San San Yee, Heat transfer correlations for open-cellular porous materials, International Communications in Heat and Mass Transfer, 32, 7, pp. 947-953 (2005)'},{id:"B19",body:'T. Takeda, D. Sampei, R. Miura, Heat transfer and fluid flow characteristics of a heat exchanger with highly porous thin copper wire inserted, Proceedings of the 30th International Symposium on Transport Phenomena (ISTP30), ISTP080 (2019)'},{id:"B20",body:'R. M. Fand, M. Varahasamy, L.S. Greer, Empirical correlation equations for heat transfer by forced convection from cylinders embedded in porous media that account for the wall effect and dispersion, International Journal of Heat and Mass Transfer, 36, 18, pp. 4407-4418 (1993)'},{id:"B21",body:'Kazuhisa Yuki, Masumi Okumura, Hidetoshi Hashizume, Saburo Toda, Neil B. Morley, Akio Sagara, Flow visualization and heat transfer characteristics for sphere-packed pipes, Journal of Thermophysics and Heat Transfer, 22, 4, pp. 632-648 (2008)'},{id:"B22",body:'S. Sharafat, A. Mills, D. Youchison, R. Nygren, B. Williams & N. Ghoniem, Ultra low pressure-drop helium-cooled porous-tungsten PFC, Journal Fusion Science and Technology, 52, 3, pp. 559-565 (2007)'},{id:"B23",body:'S. Sharafat, N. Ghoniem, M. Sawan, A. Ying, B. Williams, Breeder foam: an innovative low porosity solid breeder material, Fusion Engineering and Design, 81(1), pp. 455-460 (2006)'},{id:"B24",body:'Mohamed H. Nasr, Craig E. Green, Peter A. Kottke, Xuchen Zhang, Thomas E. Sarvey, Yogendra K. Joshi, Muhannad S. Bakir, Andrei G. Fedorov, Hotspot thermal management with flow boiling of refrigerant in ultrasmall microgaps, Journal of Electronic Packaging, 139/011006 (2017)'},{id:"B25",body:'Mohamed H. Nasr, Craig E. Green, Peter A.Kottke, Xuchen Zhang, Thomas E. Sarvey, Yogendra K. Joshi, Muhannad S. Bakir, Andrei G. Fedorov, Flow regimes and convective heat transfer of refrigerant flow boiling in ultra-small clearance microgaps, International Journal of Heat and Mass Transfer, 108, pp. 1702-1713 (2017)'},{id:"B26",body:'Pouya Asrar, Xuchen Zhang, Craig E. Green, Muhannad Bakir, Yogendra K. Joshi, Flow boiling of R245fa in a microgap with staggered circular cylindrical pin fins, International Journal of Heat and Mass Transfer, 121, pp. 329-342 (2018)'},{id:"B27",body:'Shankar Narayanan, Andrei G. Fedorov, Yogendra K. Joshi, Heat and mass transfer during evaporation of thin liquid films confined by nanoporous membranes subjected to air jet impingement, International Journal of Heat and Mass Transfer, 58, pp. 300-311 (2013)'},{id:"B28",body:'Przemysław Smakulski, Sławomir Pietrowicz, A review of the capabilities of high heat flux removal by porous materials, microchannels and spray cooling techniques, Applied Thermal Engineering, 104, pp. 636-646 (2016)'},{id:"B29",body:'S. Toda, K. Yuki, S. Ebara, Y. Kunikata, J. abei, H. Hashizume, Development of an advanced cooling device using porous media with active boiling flow counter to high heat flux, Proceedings of the 13th International Heat Transfer Conferences (IHTC13), BOI-58 (2006)'},{id:"B30",body:'Kazuhisa Yuki, Jun Abei, Hidetoshi Hashizume and Saburo Toda, Super-high heat flux removal using sintered metal porous media, Journal of Thermal Science, 14, 3, pp. 272-280 (2005)'},{id:"B31",body:'K. Yuki, K. Suzuki , H. Hashizume, S. Toda, Key issues to enable heat flux removal exceeding 10MW/m2 by use of metal porous media as latent-heat transfer device, Special Topics & Reviews in Porous Media — An International Journal, vol. 1, no. 1, pp. 1-13 (2010)'},{id:"B32",body:'Kazuhisa Yuki, Hidetoshi Hashizume, Saburo Toda, Sub-channels-inserted porous evaporator for efficient divertor cooling, Fusion Science and Technology, 60, pp. 238-242 (2011)'},{id:"B33",body:'Kazuhisa Yuki, Hidetoshi Hashizume, Saburo Toda, Akio Sagara, Divertor cooling with sub-channels-inserted metal porous media (Effects of the sub-channel volume and location on heat transfer characteristics), Fusion Science and Technology, 64, 2, pp. 325-330 (2013)'},{id:"B34",body:'Kio Takai, Kazuhisa Yuki, Akio Sagara, Heat transfer performance of EVAPORON-3 developed for an enlarged heat transfer surface of Divertor, Plasma and Fusion Research, 12, 1405015 (2017)'},{id:"B35",body:'Kazuhisa Yuki, Kio Takai, Yoshiki Indo and Koichi Suzuki, Proposal of utilizing uni-directional porous metal for extremely high heat flux removal, Proceedings of the 6th International Conference on Porous Media and Its Applications in Science and Engineering (ICPM6), (2016)'},{id:"B36",body:'Noriyuki Unno, Kazuhisa Yuki, Ryo Inoue, Yasuo Kogo, Jun Taniguchi, Shin-ichi Satake, Enhanced evaporation of porous materials with micropores and high porosity, Journal of Thermal Science and Technology, 15, 1, Paper No.19-00654 (2020)'},{id:"B37",body:'K. Boomsma, D. Poulikakos, On the effective thermal conductivity of a three-dimensionally structured fluid-saturated metal foam, International Journal of Heat and Mass Transfer, 44, 4, pp. 827-836 (2001)'},{id:"B38",body:'T. Ogushi and H. Chiba, H. Nakajima and T. Ikeda, Measurement and analysis of effective thermal conductivities of lotus-type porous copper, Journal of Applied Physics, 95, 10, pp. 5843-5847 (2004)'},{id:"B39",body:'Hiroshi Chiba, Tetsuro Ogushi, Hideo Nakajima, Teruyuki Ikeda, Heat transfer capacity of lotus-type porous copper heat sink, JSME International Journal, Series B Fluids and Thermal Engineering, 47, 3, pp. 516-521 (2004)'},{id:"B40",body:'Kazuhisa Yuki, Performance improvement and heat countermeasure technology for high temperature resistant and high heat dissipation members, Technical Information association, (2017) (in Japanese)'},{id:"B41",body:'Shu Soma, Tomoaki Kunugi, Phenomenological model for non-isothermal capillary evaporation in narrow channel, International Journal of Multiphase Flow, 122, 103154 (2020)'},{id:"B42",body:'R. Kibushi, K. Yuki, N. Unno, K. Yuki, T. Tomimura, T. Hatakeyama, M. Ishizuka, Thermal resistance evaluation in high heat flux electronics, Proceedings of 2018 International Conference on Electronics Packaging and iMAPS All Asia Conference (ICEP-IAAC2018), FE2-3 (2018)'},{id:"B43",body:'K. Yuki, M. Kawamoto, S. Nagano, K. Yuki, K. Suzuki, 53rd Japan Heat Transfer Symposium, G113 (2016) (in Japanese)'},{id:"B44",body:'Choongho Yu, Li Shi, Alan M. Cassell, Brett A. Cruden, Quoc Ngo, Jun Li, Thermal contact resistance and thermal conductivity of a carbon nanofiber, Proceedings of 2005 ASME Summer Heat Transfer Conference (2005)'},{id:"B45",body:'Hideo Nakajima, Fabrication, properties and application of porous metals with directional pores, Progress in Materials Science, 52, 7, pp. 1091-1173 (2007)'},{id:"B46",body:'H. Chiba, T. Ogushi, H. Nakajima, Heat transfer capacity of lotus-type porous copper heat sink for air cooling, Journal of Thermal Science and Technology (Journal of Thermal Science and Technology, 5, 2, pp. 222-237 (2010)'},{id:"B47",body:'K. Hokamoto, M. Vesenjak, Z. Ren, Fabrication of cylindrical uni-directional porous metal with explosive compaction, Materials Letters, 137, pp. 323-327 (2014)'},{id:"B48",body:'K. Yuki, Y. Sato, R. Kibushi, N. Unno, K. Suzuki, T. Tomimura and K. Hokamoto, Heat transfer performance of porous copper pipe with uniformly-distributed holes fabricated by explosive welding technique, Proceedings of the 27th International Symposium on Transport Phenomena, Paper no. 126 (2016)'},{id:"B49",body:'K. Takai, D. Suga, K. Yuki, R. Kibushi, N. Unno, K. Shimamoto, Development of Cooling Device utilizing, Uni-directional Porous Copper Manufactured by Metal 3D Printer Proceedings of the 56th Japan Heat Transfer Symposium, I114 (2019) (in Japanese)'},{id:"B50",body:'Kio Takai, Kohei Yuki, Kazuhisa Yuki, Risako Kibushi, Noriyuki Unno, Teruya Tanaka, Heat transfer performance of an energy-saving heat removal device with uni-directional porous copper for divertor cooling, Fusion Engineering and Design, 136, Part A, pp. 518-521 (2018)'},{id:"B51",body:'K. Yuki, R. Tsuji, K. Takai, R. Kibushi, N. Unno, K. Suzuki, Development of a small cooling device with uni-directional porous copper, Proceedings of the 54th Japan Heat Transfer Symposium, C115 (2017) (in Japanese)'},{id:"B52",body:'Kazuhisa Yuki, Tomohiro Hara, Soichiro Ikezawa, Kentaro Anju, Koichi Suzuki, Tetsuro Ogushi, Takuya Ide, Masaaki Murakami, Immersion Cooling of Electronics utilizing Lotus-Type Porous Copper, Transactions of The Japan Institute of Electronics Packaging, 9 (2016), pp. E16-013-1-E16-013-7'},{id:"B53",body:'K. Yuki, K. Takai, K. Anju, R. Kibushi, N. Unno, T. Ogushi, M. Murakami, T. Ide, Thermal management of electronics by uni-directional porous heat sinks (CHF enhancement of saturated pool boiling toward immersion cooling of on-vehicle inverter), 2017 Annual Meeting of the Japan Society of Mechanical Engineers, J0330103 (2017) (in Japanese)'},{id:"B54",body:'Yuki, K., Kibushi, R., Unno, N., Ide, T., Ogushi, T., Murakami, M., Patent publication number 2018-204882 (2018)'},{id:"B55",body:'D. Negita, K. Yuki, N. Unno, R. Kibushi, T. Ide, T. Ogushi, M. Murakami, T. Numata, H. Nomura, Critical heat flux improvement of two-phase immersion cooling by controlling breathing phenomenon, Proceedings of the International Technical Conference and Exhibition on Packaging and Integration of Electronic and Photonic Microsystems (InterPACK2020-Online), (2020)'},{id:"B56",body:'Daiki Suga, Kazuhisa Yuki, Risako Kibushi and Kio Takai, Visualization of two-phase flow in uni-directional porous copper, Proceedings of the the 31st International Symposium on Transport Phenomena (ISTP31), Paper no. 128, (2020)'}],footnotes:[],contributors:[{corresp:"yes",contributorFullName:"Kazuhisa Yuki",address:"kyuki@rs.socu.ac.jp",affiliation:'
Tokyo University of Science, Yamaguchi, Japan
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Probiotics produce many bactericidal compounds, which inhibit the growth of pathogenic microorganisms and their toxins, promoting the sustainability and structural integrity of enterocytes. 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These Terms and Conditions outline the rules and regulations pertaining to the use of IntechOpen’s website www.intechopen.com and all the subdomains owned by IntechOpen located at 5 Princes Gate Court, London, SW7 2QJ, United Kingdom.
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The following terminology applies to these Terms and Conditions, Privacy Statement, Disclaimer Notice, and any or all Agreements:
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“Client”, “Customer”, “You” and “Your” refers to you, the person accessing this website and accepting the Company’s Terms and Conditions;
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Any use of the above terminology, or other words in the singular, plural, capitalization and/or he/she or they, are taken as interchangeable.
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The toxic and allergic reactions of synthetic dyes are compelling the people to think about natural dyes. Natural dyes are renewable source of colouring materials. Besides textiles it has application in colouration of foods, medicine and in handicraft items. Though natural dyes are ecofriendly, protective to skin and pleasing colour to eyes, they are having very poor bonding with textile fibre materials, which necessitate mordanting with metallic mordants, some of which are not eco friendly, for fixation of natural dyes on textile fibres. So the supremacy of natural dyes is somewhat subdued. This necessitates newer research on application of natural dyes on different natural fibres for completely eco friendly textiles. The fundamentals of natural dyes chemistry and some of the important research work are therefore discussed in this review article.",book:{id:"9203",slug:"chemistry-and-technology-of-natural-and-synthetic-dyes-and-pigments",title:"Chemistry and Technology of Natural and Synthetic Dyes and Pigments",fullTitle:"Chemistry and Technology of Natural and Synthetic Dyes and Pigments"},signatures:"Virendra Kumar Gupta",authors:[{id:"305259",title:"Dr.",name:"Virendra",middleName:null,surname:"Kumar Gupta",slug:"virendra-kumar-gupta",fullName:"Virendra Kumar Gupta"}]},{id:"49647",title:"Fiber Selection for the Production of Nonwovens",slug:"fiber-selection-for-the-production-of-nonwovens",totalDownloads:10441,totalCrossrefCites:9,totalDimensionsCites:17,abstract:"The most significant feature of nonwoven fabric is made directly from fibers in a continuous production line. While manufacturing nonwovens, some conventional textile operations, such as carding, drawing, roving, spinning, weaving or knitting, are partially or completely eliminated. For this reason the choice of fiber is very important for nonwoven manufacturers. The commonly used fibers include natural fibers (cotton, jute, flax, wool), synthetic fibers (polyester (PES), polypropylene (PP), polyamide, rayon), special fibers (glass, carbon, nanofiber, bi-component, superabsorbent fibers). Raw materials have not only delivered significant product improvements but also benefited people using these products by providing hygiene and comfort.",book:{id:"5062",slug:"non-woven-fabrics",title:"Non-woven Fabrics",fullTitle:"Non-woven Fabrics"},signatures:"Nazan Avcioglu Kalebek and Osman Babaarslan",authors:[{id:"119775",title:"Prof.",name:"Osman",middleName:null,surname:"Babaarslan",slug:"osman-babaarslan",fullName:"Osman Babaarslan"},{id:"175829",title:"Dr.",name:"Nazan",middleName:null,surname:"Kalebek",slug:"nazan-kalebek",fullName:"Nazan Kalebek"}]},{id:"41409",title:"Surface Modification Methods for Improving the Dyeability of Textile Fabrics",slug:"surface-modification-methods-for-improving-the-dyeability-of-textile-fabrics",totalDownloads:7011,totalCrossrefCites:13,totalDimensionsCites:36,abstract:null,book:{id:"3137",slug:"eco-friendly-textile-dyeing-and-finishing",title:"Eco-Friendly Textile Dyeing and Finishing",fullTitle:"Eco-Friendly Textile Dyeing and Finishing"},signatures:"Sheila Shahidi, Jakub Wiener and Mahmood Ghoranneviss",authors:[{id:"58854",title:"Dr.",name:null,middleName:null,surname:"Shahidi",slug:"shahidi",fullName:"Shahidi"}]}],onlineFirstChaptersFilter:{topicId:"296",limit:6,offset:0},onlineFirstChaptersCollection:[],onlineFirstChaptersTotal:0},preDownload:{success:null,errors:{}},subscriptionForm:{success:null,errors:{}},aboutIntechopen:{},privacyPolicy:{},peerReviewing:{},howOpenAccessPublishingWithIntechopenWorks:{},sponsorshipBooks:{sponsorshipBooks:[],offset:8,limit:8,total:0},allSeries:{pteSeriesList:[{id:"14",title:"Artificial Intelligence",numberOfPublishedBooks:9,numberOfPublishedChapters:87,numberOfOpenTopics:6,numberOfUpcomingTopics:0,issn:"2633-1403",doi:"10.5772/intechopen.79920",isOpenForSubmission:!0},{id:"7",title:"Biomedical Engineering",numberOfPublishedBooks:12,numberOfPublishedChapters:98,numberOfOpenTopics:3,numberOfUpcomingTopics:0,issn:"2631-5343",doi:"10.5772/intechopen.71985",isOpenForSubmission:!0}],lsSeriesList:[{id:"11",title:"Biochemistry",numberOfPublishedBooks:27,numberOfPublishedChapters:287,numberOfOpenTopics:4,numberOfUpcomingTopics:0,issn:"2632-0983",doi:"10.5772/intechopen.72877",isOpenForSubmission:!0},{id:"25",title:"Environmental Sciences",numberOfPublishedBooks:1,numberOfPublishedChapters:9,numberOfOpenTopics:4,numberOfUpcomingTopics:0,issn:"2754-6713",doi:"10.5772/intechopen.100362",isOpenForSubmission:!0},{id:"10",title:"Physiology",numberOfPublishedBooks:11,numberOfPublishedChapters:139,numberOfOpenTopics:4,numberOfUpcomingTopics:0,issn:"2631-8261",doi:"10.5772/intechopen.72796",isOpenForSubmission:!0}],hsSeriesList:[{id:"3",title:"Dentistry",numberOfPublishedBooks:8,numberOfPublishedChapters:129,numberOfOpenTopics:0,numberOfUpcomingTopics:2,issn:"2631-6218",doi:"10.5772/intechopen.71199",isOpenForSubmission:!1},{id:"6",title:"Infectious Diseases",numberOfPublishedBooks:13,numberOfPublishedChapters:107,numberOfOpenTopics:3,numberOfUpcomingTopics:1,issn:"2631-6188",doi:"10.5772/intechopen.71852",isOpenForSubmission:!0},{id:"13",title:"Veterinary Medicine and Science",numberOfPublishedBooks:10,numberOfPublishedChapters:103,numberOfOpenTopics:3,numberOfUpcomingTopics:0,issn:"2632-0517",doi:"10.5772/intechopen.73681",isOpenForSubmission:!0}],sshSeriesList:[{id:"22",title:"Business, Management and Economics",numberOfPublishedBooks:1,numberOfPublishedChapters:12,numberOfOpenTopics:2,numberOfUpcomingTopics:1,issn:null,doi:"10.5772/intechopen.100359",isOpenForSubmission:!0},{id:"23",title:"Education and Human Development",numberOfPublishedBooks:0,numberOfPublishedChapters:0,numberOfOpenTopics:2,numberOfUpcomingTopics:0,issn:null,doi:"10.5772/intechopen.100360",isOpenForSubmission:!1},{id:"24",title:"Sustainable Development",numberOfPublishedBooks:0,numberOfPublishedChapters:10,numberOfOpenTopics:4,numberOfUpcomingTopics:1,issn:null,doi:"10.5772/intechopen.100361",isOpenForSubmission:!0}],testimonialsList:[{id:"13",text:"The collaboration with and support of the technical staff of IntechOpen is fantastic. 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He also has an honorary appointment to serve as a Collaborative Professor at Kanazawa University, Japan, from Mar 2015 to the present. \nFormerly, Dr. Rahman was a faculty member of the University of Chittagong, Bangladesh, affiliated with the Department of Chemistry (Oct 2002 to Mar 2012) and the Department of Applied Chemistry and Chemical Engineering (Mar 2012 to Sep 2015). Dr. Rahman was also adjunctly attached with Kanazawa University, Japan (Visiting Research Professor, Dec 2014 to Mar 2015; JSPS Postdoctoral Research Fellow, Apr 2012 to Mar 2014), and Tokyo Institute of Technology, Japan (TokyoTech-UNESCO Research Fellow, Oct 2004–Sep 2005). \nHe received his Ph.D. degree in Environmental Analytical Chemistry from Kanazawa University, Japan (2011). He also achieved a Diploma in Environment from the Tokyo Institute of Technology, Japan (2005). Besides, he has an M.Sc. degree in Applied Chemistry and a B.Sc. degree in Chemistry, all from the University of Chittagong, Bangladesh. \nDr. Rahman’s research interest includes the study of the fate and behavior of environmental pollutants in the biosphere; design of low energy and low burden environmental improvement (remediation) technology; implementation of sustainable waste management practices for treatment, handling, reuse, and ultimate residual disposition of solid wastes; nature and type of interactions in organic liquid mixtures for process engineering design applications.",institutionString:null,institution:{name:"Fukushima University",institutionURL:null,country:{name:"Japan"}}},editorTwo:{id:"201020",title:"Dr.",name:"Zinnat Ara",middleName:null,surname:"Begum",slug:"zinnat-ara-begum",fullName:"Zinnat Ara Begum",profilePictureURL:"https://mts.intechopen.com/storage/users/201020/images/system/201020.jpeg",biography:"Zinnat A. 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Graduate in Sciences (Chemist), graduate in Geography and History (Geography), master in Water Management, Treatment, master in Fertilizers and Environment and master in Environmental Management; Ph.D. in Environmental Sciences. His research is focused on soil-water and waste-environment relations, mainly on soil-water and soil-waste interactions under different management and waste reuse. His work is reflected in more than 230 communications presented in national and international conferences and congresses, 29 invited lectures from universities, associations and government agencies. 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He has developed his research activity in the fields of fauna and soil ecology, and in the treatment of organic waste, having been the founder and principal investigator of the Environmental Biotechnology Group of the University of Vigo.\r\nHis research activity in the field of Environmental Biotechnology has been focused on the development of novel organic waste treatment systems through composting. 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She has focused her research activity on the taxonomy, fauna and ecology of aquatic beetles, in addition to other lines of research such as the conservation of biodiversity in freshwater ecosystems; conservation of protected areas (Red Natura 2000) and assessment of the effectiveness of wetlands as priority areas for the conservation of aquatic invertebrates; studies of water quality in freshwater ecosystems through biological indicators and physicochemical parameters; surveillance and research of vector arthropods and invasive alien species.",institutionString:null,institution:{name:"University of Vigo",institutionURL:null,country:{name:"Spain"}}},editorThree:{id:"464288",title:"Dr.",name:"Francisco",middleName:null,surname:"Ramil",slug:"francisco-ramil",fullName:"Francisco Ramil",profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0033Y00003RI7lHQAT/Profile_Picture_2022-03-31T10:15:35.png",biography:"Fran Ramil Blanco (Porto de Espasante, A Coruña, 1960), is a doctor in biology from the University of Santiago de Compostela and a Professor of Zoology at the Department of Ecology and Animal Biology at the University of Vigo. His research activity is linked to the taxonomy, fauna and ecology of marine benthic invertebrates and especially the Cnidarian group. Since 2004, he has been part of the EcoAfrik project, aimed at the study, protection and conservation of biodiversity and benthic habitats in West Africa. 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That is exactly what he does, diving into Machine Learning algorithms and technologies to help TECNALIA to decide whether something is great in theory or will actually impact on the product or processes of its projects. So, he is expert at framing experiments, developing hypotheses, and proving whether they’re true or not, in order to investigate fundamental problems with a longer time horizon. He is also able to design and develop PoCs and system prototypes in simulation. He has participated in several national and internacional R&D projects.\n\nAs another relevant part of his everyday research work, he usually publishes his findings in reputed scientific refereed journals and international conferences, occasionally acting as reviewer and Programme Commitee member. Concretely, since 2018 he has published 9 JCR (8 Q1) journal papers, 9 conference papers (e.g. ECML PKDD 2021), and he has co-edited a book. He is also active in popular science writing data science stories for reputed blogs (KDNuggets, TowardsDataScience, Naukas). Besides, he has recently embarked on mentoring programmes as mentor, and has also worked as data science trainer.",institutionString:"TECNALIA Research & Innovation",institution:{name:"Tecnalia",country:{name:"Spain"}}},{id:"103779",title:"Prof.",name:"Yalcin",middleName:null,surname:"Isler",slug:"yalcin-isler",fullName:"Yalcin Isler",position:null,profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0030O00002bRyQ8QAK/Profile_Picture_1628834958734",biography:"Yalcin Isler (1971 - Burdur / Turkey) received the B.Sc. degree in the Department of Electrical and Electronics Engineering from Anadolu University, Eskisehir, Turkey, in 1993, the M.Sc. degree from the Department of Electronics and Communication Engineering, Suleyman Demirel University, Isparta, Turkey, in 1996, the Ph.D. degree from the Department of Electrical and Electronics Engineering, Dokuz Eylul University, Izmir, Turkey, in 2009, and the Competence of Associate Professorship from the Turkish Interuniversity Council in 2019.\n\nHe was Lecturer at Burdur Vocational School in Suleyman Demirel University (1993-2000, Burdur / Turkey), Software Engineer (2000-2002, Izmir / Turkey), Research Assistant in Bulent Ecevit University (2002-2003, Zonguldak / Turkey), Research Assistant in Dokuz Eylul University (2003-2010, Izmir / Turkey), Assistant Professor at the Department of Electrical and Electronics Engineering in Bulent Ecevit University (2010-2012, Zonguldak / Turkey), Assistant Professor at the Department of Biomedical Engineering in Izmir Katip Celebi University (2012-2019, Izmir / Turkey). He is an Associate Professor at the Department of Biomedical Engineering at Izmir Katip Celebi University, Izmir / Turkey, since 2019. In addition to academics, he has also founded Islerya Medical and Information Technologies Company, Izmir / Turkey, since 2017.\n\nHis main research interests cover biomedical signal processing, pattern recognition, medical device design, programming, and embedded systems. He has many scientific papers and participated in several projects in these study fields. He was an IEEE Student Member (2009-2011) and IEEE Member (2011-2014) and has been IEEE Senior Member since 2014.",institutionString:null,institution:{name:"Izmir Kâtip Çelebi University",country:{name:"Turkey"}}},{id:"339677",title:"Dr.",name:"Mrinmoy",middleName:null,surname:"Roy",slug:"mrinmoy-roy",fullName:"Mrinmoy Roy",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/339677/images/16768_n.jpg",biography:"An accomplished Sales & Marketing professional with 12 years of cross-functional experience in well-known organisations such as CIPLA, LUPIN, GLENMARK, ASTRAZENECA across different segment of Sales & Marketing, International Business, Institutional Business, Product Management, Strategic Marketing of HIV, Oncology, Derma, Respiratory, Anti-Diabetic, Nutraceutical & Stomatological Product Portfolio and Generic as well as Chronic Critical Care Portfolio. A First Class MBA in International Business & Strategic Marketing, B.Pharm, D.Pharm, Google Certified Digital Marketing Professional. Qualified PhD Candidate in Operations and Management with special focus on Artificial Intelligence and Machine Learning adoption, analysis and use in Healthcare, Hospital & Pharma Domain. Seasoned with diverse therapy area of Pharmaceutical Sales & Marketing ranging from generating revenue through generating prescriptions, launching new products, and making them big brands with continuous strategy execution at the Physician and Patients level. Moved from Sales to Marketing and Business Development for 3.5 years in South East Asian Market operating from Manila, Philippines. Came back to India and handled and developed Brands such as Gluconorm, Lupisulin, Supracal, Absolut Woman, Hemozink, Fabiflu (For COVID 19), and many more. In my previous assignment I used to develop and execute strategies on Sales & Marketing, Commercialization & Business Development for Institution and Corporate Hospital Business portfolio of Oncology Therapy Area for AstraZeneca Pharma India Ltd. Being a Research Scholar and Student of ‘Operations Research & Management: Artificial Intelligence’ I published several pioneer research papers and book chapters on the same in Internationally reputed journals and Books indexed in Scopus, Springer and Ei Compendex, Google Scholar etc. Currently, I am launching PGDM Pharmaceutical Management Program in IIHMR Bangalore and spearheading the course curriculum and structure of the same. I am interested in Collaboration for Healthcare Innovation, Pharma AI Innovation, Future trend in Marketing and Management with incubation on Healthcare, Healthcare IT startups, AI-ML Modelling and Healthcare Algorithm based training module development. I am also an affiliated member of the Institute of Management Consultant of India, looking forward to Healthcare, Healthcare IT and Innovation, Pharma and Hospital Management Consulting works.",institutionString:null,institution:{name:"Lovely Professional University",country:{name:"India"}}},{id:"1063",title:"Prof.",name:"Constantin",middleName:null,surname:"Volosencu",slug:"constantin-volosencu",fullName:"Constantin Volosencu",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/1063/images/system/1063.png",biography:"Prof. Dr. Constantin Voloşencu graduated as an engineer from\nPolitehnica University of Timișoara, Romania, where he also\nobtained a doctorate degree. He is currently a full professor in\nthe Department of Automation and Applied Informatics at the\nsame university. Dr. Voloşencu is the author of ten books, seven\nbook chapters, and more than 160 papers published in journals\nand conference proceedings. He has also edited twelve books and\nhas twenty-seven patents to his name. He is a manager of research grants, editor in\nchief and member of international journal editorial boards, a former plenary speaker, a member of scientific committees, and chair at international conferences. His\nresearch is in the fields of control systems, control of electric drives, fuzzy control\nsystems, neural network applications, fault detection and diagnosis, sensor network\napplications, monitoring of distributed parameter systems, and power ultrasound\napplications. He has developed automation equipment for machine tools, spooling\nmachines, high-power ultrasound processes, and more.",institutionString:"Polytechnic University of Timişoara",institution:{name:"Polytechnic University of Timişoara",country:{name:"Romania"}}},{id:"221364",title:"Dr.",name:"Eneko",middleName:null,surname:"Osaba",slug:"eneko-osaba",fullName:"Eneko Osaba",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/221364/images/system/221364.jpg",biography:"Dr. Eneko Osaba works at TECNALIA as a senior researcher. He obtained his Ph.D. in Artificial Intelligence in 2015. He has participated in more than twenty-five local and European research projects, and in the publication of more than 130 papers. He has performed several stays at universities in the United Kingdom, Italy, and Malta. Dr. Osaba has served as a program committee member in more than forty international conferences and participated in organizing activities in more than ten international conferences. He is a member of the editorial board of the International Journal of Artificial Intelligence, Data in Brief, and Journal of Advanced Transportation. He is also a guest editor for the Journal of Computational Science, Neurocomputing, Swarm, and Evolutionary Computation and IEEE ITS Magazine.",institutionString:"TECNALIA Research & Innovation",institution:{name:"Tecnalia",country:{name:"Spain"}}},{id:"275829",title:"Dr.",name:"Esther",middleName:null,surname:"Villar-Rodriguez",slug:"esther-villar-rodriguez",fullName:"Esther Villar-Rodriguez",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/275829/images/system/275829.jpg",biography:"Dr. Esther Villar obtained a Ph.D. in Information and Communication Technologies from the University of Alcalá, Spain, in 2015. She obtained a degree in Computer Science from the University of Deusto, Spain, in 2010, and an MSc in Computer Languages and Systems from the National University of Distance Education, Spain, in 2012. Her areas of interest and knowledge include natural language processing (NLP), detection of impersonation in social networks, semantic web, and machine learning. Dr. Esther Villar made several contributions at conferences and publishing in various journals in those fields. Currently, she is working within the OPTIMA (Optimization Modeling & Analytics) business of TECNALIA’s ICT Division as a data scientist in projects related to the prediction and optimization of management and industrial processes (resource planning, energy efficiency, etc).",institutionString:"TECNALIA Research & Innovation",institution:{name:"Tecnalia",country:{name:"Spain"}}},{id:"49813",title:"Dr.",name:"Javier",middleName:null,surname:"Del Ser",slug:"javier-del-ser",fullName:"Javier Del Ser",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/49813/images/system/49813.png",biography:"Prof. Dr. Javier Del Ser received his first PhD in Telecommunication Engineering (Cum Laude) from the University of Navarra, Spain, in 2006, and a second PhD in Computational Intelligence (Summa Cum Laude) from the University of Alcala, Spain, in 2013. He is currently a principal researcher in data analytics and optimisation at TECNALIA (Spain), a visiting fellow at the Basque Center for Applied Mathematics (BCAM) and a part-time lecturer at the University of the Basque Country (UPV/EHU). His research interests gravitate on the use of descriptive, prescriptive and predictive algorithms for data mining and optimization in a diverse range of application fields such as Energy, Transport, Telecommunications, Health and Industry, among others. In these fields he has published more than 240 articles, co-supervised 8 Ph.D. theses, edited 6 books, coauthored 7 patents and participated/led more than 40 research projects. He is a Senior Member of the IEEE, and a recipient of the Biscay Talent prize for his academic career.",institutionString:"Tecnalia Research & Innovation",institution:null},{id:"278948",title:"Dr.",name:"Carlos Pedro",middleName:null,surname:"Gonçalves",slug:"carlos-pedro-goncalves",fullName:"Carlos Pedro Gonçalves",position:null,profilePictureURL:"https://s3.us-east-1.amazonaws.com/intech-files/0030O00002bRcmyQAC/Profile_Picture_1564224512145",biography:'Carlos Pedro Gonçalves (PhD) is an Associate Professor at Lusophone University of Humanities and Technologies and a researcher on Complexity Sciences, Quantum Technologies, Artificial Intelligence, Strategic Studies, Studies in Intelligence and Security, FinTech and Financial Risk Modeling. He is also a progammer with programming experience in:\n\nA) Quantum Computing using Qiskit Python module and IBM Quantum Experience Platform, with software developed on the simulation of Quantum Artificial Neural Networks and Quantum Cybersecurity;\n\nB) Artificial Intelligence and Machine learning programming in Python;\n\nC) Artificial Intelligence, Multiagent Systems Modeling and System Dynamics Modeling in Netlogo, with models developed in the areas of Chaos Theory, Econophysics, Artificial Intelligence, Classical and Quantum Complex Systems Science, with the Econophysics models having been cited worldwide and incorporated in PhD programs by different Universities.\n\nReceived an Arctic Code Vault Contributor status by GitHub, due to having developed open source software preserved in the \\"Arctic Code Vault\\" for future generations (https://archiveprogram.github.com/arctic-vault/), with the Strategy Analyzer A.I. module for decision making support (based on his PhD thesis, used in his Classes on Decision Making and in Strategic Intelligence Consulting Activities) and QNeural Python Quantum Neural Network simulator also preserved in the \\"Arctic Code Vault\\", for access to these software modules see: https://github.com/cpgoncalves. He is also a peer reviewer with outsanding review status from Elsevier journals, including Physica A, Neurocomputing and Engineering Applications of Artificial Intelligence. Science CV available at: https://www.cienciavitae.pt//pt/8E1C-A8B3-78C5 and ORCID: https://orcid.org/0000-0002-0298-3974',institutionString:"University of Lisbon",institution:{name:"Universidade Lusófona",country:{name:"Portugal"}}},{id:"241400",title:"Prof.",name:"Mohammed",middleName:null,surname:"Bsiss",slug:"mohammed-bsiss",fullName:"Mohammed Bsiss",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/241400/images/8062_n.jpg",biography:null,institutionString:null,institution:null},{id:"276128",title:"Dr.",name:"Hira",middleName:null,surname:"Fatima",slug:"hira-fatima",fullName:"Hira Fatima",position:null,profilePictureURL:"https://mts.intechopen.com/storage/users/276128/images/14420_n.jpg",biography:"Dr. Hira Fatima\nAssistant Professor\nDepartment of Mathematics\nInstitute of Applied Science\nMangalayatan University, Aligarh\nMobile: no : 8532041179\nhirafatima2014@gmal.com\n\nDr. Hira Fatima has received his Ph.D. degree in pure Mathematics from Aligarh Muslim University, Aligarh India. Currently working as an Assistant Professor in the Department of Mathematics, Institute of Applied Science, Mangalayatan University, Aligarh. She taught so many courses of Mathematics of UG and PG level. Her research Area of Expertise is Functional Analysis & Sequence Spaces. She has been working on Ideal Convergence of double sequence. She has published 17 research papers in National and International Journals including Cogent Mathematics, Filomat, Journal of Intelligent and Fuzzy Systems, Advances in Difference Equations, Journal of Mathematical Analysis, Journal of Mathematical & Computer Science etc. She has also reviewed few research papers for the and international journals. She is a member of Indian Mathematical Society.",institutionString:null,institution:null},{id:"414880",title:"Dr.",name:"Maryam",middleName:null,surname:"Vatankhah",slug:"maryam-vatankhah",fullName:"Maryam Vatankhah",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"Borough of Manhattan Community College",country:{name:"United States of America"}}},{id:"414879",title:"Prof.",name:"Mohammad-Reza",middleName:null,surname:"Akbarzadeh-Totonchi",slug:"mohammad-reza-akbarzadeh-totonchi",fullName:"Mohammad-Reza Akbarzadeh-Totonchi",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"Ferdowsi University of Mashhad",country:{name:"Iran"}}},{id:"414878",title:"Prof.",name:"Reza",middleName:null,surname:"Fazel-Rezai",slug:"reza-fazel-rezai",fullName:"Reza Fazel-Rezai",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"American Public University System",country:{name:"United States of America"}}},{id:"302698",title:"Dr.",name:"Yao",middleName:null,surname:"Shan",slug:"yao-shan",fullName:"Yao Shan",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"Dalian University of Technology",country:{name:"China"}}},{id:"125911",title:"Prof.",name:"Jia-Ching",middleName:null,surname:"Wang",slug:"jia-ching-wang",fullName:"Jia-Ching Wang",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"National Central University",country:{name:"Taiwan"}}},{id:"357085",title:"Mr.",name:"P. Mohan",middleName:null,surname:"Anand",slug:"p.-mohan-anand",fullName:"P. Mohan Anand",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"Indian Institute of Technology Kanpur",country:{name:"India"}}},{id:"356696",title:"Ph.D. Student",name:"P.V.",middleName:null,surname:"Sai Charan",slug:"p.v.-sai-charan",fullName:"P.V. Sai Charan",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"Indian Institute of Technology Kanpur",country:{name:"India"}}},{id:"357086",title:"Prof.",name:"Sandeep K.",middleName:null,surname:"Shukla",slug:"sandeep-k.-shukla",fullName:"Sandeep K. Shukla",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"Indian Institute of Technology Kanpur",country:{name:"India"}}},{id:"356823",title:"MSc.",name:"Seonghee",middleName:null,surname:"Min",slug:"seonghee-min",fullName:"Seonghee Min",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"Daegu University",country:{name:"Korea, South"}}},{id:"353307",title:"Prof.",name:"Yoosoo",middleName:null,surname:"Oh",slug:"yoosoo-oh",fullName:"Yoosoo Oh",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:"Yoosoo Oh received his Bachelor's degree in the Department of Electronics and Engineering from Kyungpook National University in 2002. He obtained his Master’s degree in the Department of Information and Communications from Gwangju Institute of Science and Technology (GIST) in 2003. In 2010, he received his Ph.D. degree in the School of Information and Mechatronics from GIST. In the meantime, he was an executed team leader at Culture Technology Institute, GIST, 2010-2012. In 2011, he worked at Lancaster University, the UK as a visiting scholar. In September 2012, he joined Daegu University, where he is currently an associate professor in the School of ICT Conver, Daegu University. Also, he served as the Board of Directors of KSIIS since 2019, and HCI Korea since 2016. From 2017~2019, he worked as a center director of the Mixed Reality Convergence Research Center at Daegu University. From 2015-2017, He worked as a director in the Enterprise Supporting Office of LINC Project Group, Daegu University. His research interests include Activity Fusion & Reasoning, Machine Learning, Context-aware Middleware, Human-Computer Interaction, etc.",institutionString:null,institution:{name:"Daegu Gyeongbuk Institute of Science and Technology",country:{name:"Korea, South"}}},{id:"262719",title:"Dr.",name:"Esma",middleName:null,surname:"Ergüner Özkoç",slug:"esma-erguner-ozkoc",fullName:"Esma Ergüner Özkoç",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"Başkent University",country:{name:"Turkey"}}},{id:"346530",title:"Dr.",name:"Ibrahim",middleName:null,surname:"Kaya",slug:"ibrahim-kaya",fullName:"Ibrahim Kaya",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"Izmir Kâtip Çelebi University",country:{name:"Turkey"}}},{id:"419199",title:"Dr.",name:"Qun",middleName:null,surname:"Yang",slug:"qun-yang",fullName:"Qun Yang",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"University of Auckland",country:{name:"New Zealand"}}},{id:"351158",title:"Prof.",name:"David W.",middleName:null,surname:"Anderson",slug:"david-w.-anderson",fullName:"David W. Anderson",position:null,profilePictureURL:"//cdnintech.com/web/frontend/www/assets/author.svg",biography:null,institutionString:null,institution:{name:"University of Calgary",country:{name:"Canada"}}}]}},subseries:{item:{id:"95",type:"subseries",title:"Urban Planning and Environmental Management",keywords:"Circular economy, Contingency planning and response to disasters, Ecosystem services, Integrated urban water management, Nature-based solutions, Sustainable urban development, Urban green spaces",scope:"
\r\n\tIf we aim to prosper as a society and as a species, there is no alternative to sustainability-oriented development and growth. Sustainable development is no longer a choice but a necessity for us all. Ecosystems and preserving ecosystem services and inclusive urban development present promising solutions to environmental problems. Contextually, the emphasis on studying these fields will enable us to identify and define the critical factors for territorial success in the upcoming decades to be considered by the main-actors, decision and policy makers, technicians, and public in general.
\r\n
\r\n\tHolistic urban planning and environmental management are therefore crucial spheres that will define sustainable trajectories for our urbanizing planet. This urban and environmental planning topic aims to attract contributions that address sustainable urban development challenges and solutions, including integrated urban water management, planning for the urban circular economy, monitoring of risks, contingency planning and response to disasters, among several other challenges and solutions.
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Since 2015 he heads the research department Sanitation, Water and Solid Waste for Development (Sandec) at the Swiss Federal Institute of Aquatic Research and Technology (Eawag).",institutionString:"Swiss Federal Institute of Aquatic Science and Technology, Switzerland",institution:null},editorTwo:{id:"290571",title:"Dr.",name:"Rui Alexandre",middleName:null,surname:"Castanho",slug:"rui-alexandre-castanho",fullName:"Rui Alexandre Castanho",profilePictureURL:"https://mts.intechopen.com/storage/users/290571/images/system/290571.jpg",biography:"Rui Alexandre Castanho has a master\\'s degree in Planning, Audit, and Control in Urban Green Spaces and an international Ph.D. in Sustainable Planning in Borderlands. Currently, he is a professor at WSB University, Poland, and a visiting professor at the University of Johannesburg, South Africa. Dr. Castanho is a post-doc researcher on the GREAT Project, University of Azores, Ponta Delgada, Portugal. He collaborates with the Environmental Resources Analysis Research Group (ARAM), University of Extremadura (UEx), Spain; VALORIZA - Research Center for the Enhancement of Endogenous Resources, Polytechnic Institute of Portalegre (IPP), Portugal; Centre for Tourism Research, Development and Innovation (CITUR), Madeira, Portugal; and AQUAGEO Research Group, University of Campinas (UNICAMP), Brazil.",institutionString:"University of Johannesburg, South Africa and WSB University, Poland",institution:{name:"University of Johannesburg",institutionURL:null,country:{name:"South Africa"}}},editorThree:null,series:{id:"24",title:"Sustainable Development",doi:"10.5772/intechopen.100361",issn:null},editorialBoard:[{id:"181486",title:"Dr.",name:"Claudia",middleName:null,surname:"Trillo",slug:"claudia-trillo",fullName:"Claudia 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