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Bulk nanocrystalline (NC) silvers were fabricated by spark plasma sintering process. The effects of sintering temperature on physical and mechanical properties of the NC silvers were investigated. The results indicate that no impurities were introduced into the bulk compacts during the preparation procedure. Both the density and the electrical conductivity of the NC Ag increase with an increase in sintering temperature. However, the micro-hardness and ultimate tensile strength (UTS) of the bulk compacts increase initially and then decrease with increasing sintering temperature. The NC Ag sintered at 500 °C exhibits the highest micro-hardness of 85.3 HV along with the best compression yield strength of 379 MPa and the highest UTS of 534 MPa. The deterioration of the mechanical properties of the NC Ag sintered at 550 °C should be attributed to the rapid grain growth.
The title compound, the 4-phenyl-6-(trifluoromethyl)-3,4-dihydroquinolin-2(1H)-one (4) with chemical formula: (C16H12F3NO), was synthesized from N-[4-(trifluoromethyl)phenyl]cinnamamide (3), chemical formula: (C16H12F3NO), through an intramolecular cyclization mediated by triflic acid. Preliminary molecular characterization of both compounds was performed by Fourier transform infrared spectroscopy, gas chromatography mass spectrometry, and nuclear magnetic resonance spectroscopy (1H, 13C); crystallographic characterization was completed by X-ray diffraction of polycrystalline samples. The title compound 4 crystallized in a monoclinic system and unit-cell parameters are reported [a = 16.002 (3), b = 5.170 (1), c = 17.733 (3) Å, β = 111.11 (2)°, unit-cell volume V = 1368.5 (3) Å3, Z = 4] P21/c (No. 14) space group; the title compound 3 crystallized in a monoclinic system and unit-cell parameters are reported [a = 12.902 (2), b = 5.144 (1), c = 20.513 (5) Å, β = 91.67 (2)°, unit-cell volume V = 1360.7 (4) Å3, Z = 4] P21/c (No. 14) space group.
The slip systems in ZrB2 flexural tested at 1000 °C and 1500 °C have been quantified. The dislocations in both samples were long and straight with a dislocation density of approximately 1013 m−2. The structure of the dislocations as well as the low density is in agreement with a ceramic that is hard and brittle and dislocation nucleation and motion is restricted. The low temperature slip systems were found to include c-prismatic slip—${1 \mathord{\left/ {\vphantom {1 3}} \right. \kern-\nulldelimiterspace} 3}\left[ {0001} \right]\left( {\bar 1010} \right)$—and a-pyramidal slip—${1 \mathord{\left/ {\vphantom {1 3}} \right. \kern-\nulldelimiterspace} 3}\left[ {11\bar 20} \right]\left( {\bar 1101} \right)$ whereas the elevated temperature sample revealed a-basal slip—${1 \mathord{\left/ {\vphantom {1 3}} \right. \kern-\nulldelimiterspace} 3}\left[ {11\bar 20} \right]\left( {0001} \right)$. Density functional theory Generalized Stacking Fault Energy curves for perfect slip were calculated and agreed well with geometric considerations for slip, including interplanar spacing and planar packing. Though basal slip has the lowest fault energy, the presence of the other dislocation types is suggestive that the activation barrier is not a hindrance for the temperatures studied and is likely activated to increase the number of plastic degrees of freedom.
Recently, a new boron allotrope B52 with orthorhombic structure was theoretically predicted to be more stable than α-tetragonal boron B50. In experiments however, only tetragonal boron phases have been obtained so far. Here, we report for the first time on the preparation of orthorhombic boron phase of B52-type, space group Pnnn, a = 8.894 Å, b = 8.784 Å, c = 5.019 Å, by normal-pressure annealing of α-tetragonal boron, synthesized at high pressures by pyrolysis of decaborane, B10H14. We have investigated temperature-induced structure evolution and thermal desorption of boron samples, which allowed us to regard the structure of mother “α-tetragonal boron” as a boron-rich hydride with composition close to B51.5H7.7. In accordance with density-functional theory calculations, the most preferable sites of hydrogen placement in tetragonal unit cell are 8j and 4g; the tetragonal-to-orthorhombic transition takes place spontaneously upon complete dehydrogenation.
A new quaternary compound AlCeCo2Ni2 was synthesized and studied by means of X-ray powder diffraction technique. The powder pattern of AlCeCo2Ni2 was indexed and refined, giving a hexagonal structure, space group P6/mmm (No. 191) with the CaCu5 structure type. a = 4.9242(2) Å, c = 4.0524(1) Å, V = 85.1 Å3, Z = 1, ρx = 7.85 g cm−3, F30 = 130.2(0.010, 30), and RIR = 0.71(2).
In this investigation, the ability of Rietveld refinement method was used to simultaneously refine the structure and microstructure and evaluate the linear defects of cubic crystals. To do this, the basis of Stephans theory, about the anisotropic strain broadening, was developed and the values of dislocation density as well as the fraction of dislocation types were estimated. The reliability of this procedure was checked by selecting four different nanocrystaslline samples and evaluating the microstructure of these materials. Finally, the results were compared with those extracted from the whole powder pattern modeling method. Good agreement was achieved between the results of two methods.
In the present work, a multi response optimization technique based on Taguchi method coupled with grey relational analysis is used for electrical discharge machining operations on duplex (α–β) brass. Stir casting technique was used to fabricate the duplex brass plates. The mechanical properties of the material are reported. Experiments were conducted with three machining variables such as current, pulse-on time and spark voltage and planned as per Taguchi technique. Material removal rate (MRR), electrode wear rate (EWR), and surface roughness (SR) are chosen as output parameters for this study. Results showed that, peak current and spark voltage were the significant parameters to affect MRR, EWR, and SR as per grey relational grade. The optimal combination parameters were identified as A3B3C2 i.e., pulse current at 14 A, pulse on-time at 200 μs, and voltage at 50 V. Analysis of variance was used for analyzing the results. The confirmation tests were performed to validate the results obtained by grey relational analysis and the improvement was achieved.
With the emergence of flexible/stretchable electronics, flexible solar cells (SCs) are able to attract much academic and industrial attention due to its advantages of lightweight, foldability, low cost, and extensive applications. Wearable technology has become a hot topic in the tech industry in this few years, shirts that read wearer's biological and physiological information are just beginning to make their way into society and will change the way that we interact with technology. The high strength and good electronic properties of graphene fiber make it a good candidate for some specific applications, such as wearable SCs, since it can be obtained at relatively low cost and it is amongst the strongest commercial yarns in existence. In this review, a summarized state of the art regarding wearable SCs is presented including several applications of graphene and its derivatives with their remarkable unconventional applications.
The effects of annealing temperatures on the structure and photocurrent response of nanoporous iron oxide film prepared by anodization of iron foil in an ethylene glycol, NH4F, and H2O electrolyte were studied. The as-anodized anodic film was found to be rather amorphous and crystallized to predominantly α-Fe2O3 upon annealing in nitrogen. Nitrogen was used as to reduce the thickening of the barrier layer which affects the photocurrent response of the oxide. However, annealing must be done above 300 °C to produce crystalline oxide but must be kept lower than 500 °C since high temperature promotes grain growth, destroying the nanoporous structure and also thickens the barrier layer, which significantly reduce the photocurrent of the film. Sample annealed at 450 °C in nitrogen has the highest photocurrent of 1.04 mA/cm2 (0.5 V versus Ag/AgCl in 1 M NaOH) compared to 0.13 mA/cm2 at 0.5 V for air-annealed sample.
The National Institute of Standards and Technology (NIST) certifies a suite of Standard Reference Materials (SRMs) to address specific aspects of the performance of X-ray powder diffraction instruments. This report describes SRM 1878b, the third generation of this powder diffraction SRM. SRM 1878b is intended for use in the preparation of calibration standards for the quantitative analyses of α-quartz by X-ray powder diffraction in accordance to National Institute for Occupational Safety and Health Analytical Method 7500, or equivalent. A unit of SRM 1878b consists of approximately 5 g of α-quartz powder bottled in an argon atmosphere. It is certified with respect to crystalline phase purity, or amorphous phase content, and lattice parameter. Neutron powder diffraction, both time of flight and constant wavelength, was used to certify the phase purity using SRM 676a as an internal standard. A NIST-built diffractometer, incorporating many advanced design features was used for certification measurements for lattice parameters.
Using the peeling-induced splitting method, the effect of the irradiation of ultraviolet (UV) light on the formation of surface gratings on the surface of PMMA(Poly(Methyl Methacrylate))-based films is investigated at room temperature. The thickness of the PMMA-based films is in range of 236–534 nm, and the irradiation dose is in range of 0–5 J/cm2. Surface gratings are formed on the surface of the irradiated PMMA-based films. The spatial wave length is a linear function of the film thickness, independent of the UV doses used. The peeling-induced splitting process introduces compressive stress on the surface of the PMMA-based films, much larger than the corresponding surface energy. The magnitude of the apparent surface force increases with the increase of the film thickness. All the surface gratings formed have amplitudes approximately in the same range.
The deformation behaviors (flow behavior, power dissipation, dynamic recrystallization, and microstructure evolution) of a typical powder metallurgy nickel-based superalloy were investigated in compression tests at temperatures range of 1020–1140 °C and strain rates range of 0.001–1.0 s−1 with the true strains of 0.3, 0.5, and 0.7, respectively. The efficiency of power dissipation can be shown by the power dissipation maps at different true strains. The results showed that true strain had a great effect on the power dissipation. Besides, the deformed microstructures were investigated. The processes of microstructure evolution at different deformation temperatures and strain rates are different. The continuous dynamic recrystallization takes place at the deformation condition of 1080 °C/0.1 s−1. The fine and uniform dynamic recrystallized grains gradually replace the pre-existing grains with the increase of true strain. The discontinuous dynamic recrystallization takes place at the deformation condition of 1110 °C/0.001 s−1. The fine dynamic recrystallized grains grow up and a part of new fine grains appear in the dynamic recrystallized grains because of the periodic dynamic recrystallization.
Zeolite–zeolite composite composed of alumina-rich hierarchically porous ZSM-5 cores and high-silicon MFI shells was prepared by a hydrothermal synthesis procedure, in which a commercial ZSM-5 zeolite with a SiO2/Al2O3 of 36 was treated by an alkaline solution and then used as a supporter for epitaxial growth of a polycrystalline Silicalite-1 zeolite shell (denoted as MMZsa). Acid sites associated with framework Al on exterior surfaces of ZSM-5 zeolite cores are therefore passivated in different degrees by the epitaxial MFI zeolite shell. The structural, crystalline, and textural properties of the as-synthesized samples were characterized by x-ray powder diffraction (XRD), energy-dispersive x-ray spectroscopy, X-ray photoelectron spectroscopy (XPS), scanning electron microscopy (SEM), transmission electron microscopy (TEM), selected area electron diffraction (SAED), N2 adsorption-desorption, in situ IR spectra of pyridine and NH3-TPD. Aluminum species were observed to transfer from the alumina-rich cores to the high-silica shells. The adjustable thickness and SiO2/Al2O3 ratio of the shell offer the as-synthesized composite a potential and high-efficiency catalyst for methanol conversion into gasoline and diesel. As compared with the commercial ZSM-5 zeolite, the composite catalyst exhibits excellent catalytic performances with a longer catalytic life as well as a higher conversion and a slightly higher yield of diesel oil.
Density modulated tungsten (W) thin films with nanoscale porosity contents of 7% to 40% by volume were grown on Si substrates through magnetron sputter deposition. Process parameters were selected according to the structure zone model, which resulted in film thicknesses between 105 nm and 520 nm. Nanomechanical properties of samples were investigated by means of instrumented nanoindentation. Reduced-χ2 analysis was carried out to assess four models formulated through differential effective medium approach. The model that factored in both the crowding effect and the maximum random packing of pores successfully captured the experimental trends. Attempts to breach the auxetic barrier resulted in large-scale pulverization or spontaneous conversion into WO3. Porosity corrected yield strength calculations underlined the possibility of defining a porosity threshold beyond which the compressive yield strength of density modulated nanoporous metallic thin films would drop abruptly due to aggravated geometric slenderness effects in agreement with earlier hypotheses.
This new updated edition provides an unrivaled overview of fibrous materials, their processing, microstructure, properties, and applications. The entire range of fibrous materials is discussed in depth, from natural polymeric fibers such as silk and vegetable fibers, and synthetic polymeric fibers such as aramid and polyethylene, to metallic fibers including steel, tungsten, Nb-Ti, and Nb3Sn, ceramic fibers such as alumina and silicon carbide, and carbon and glass fibers. Fundamental concepts are explained clearly and concisely along with detail on applications in areas including medicine, aerospace, optical communications, and recycling. Significant recent advances are also covered, with new information on the electrospinning of fibers, carbon nanotubes, and photonic bandgap fibers, and detail on advances made in the production and control of microstructure in high stiffness and high strength fibers. Accessibly written and unrivaled in scope, this is an ideal resource for students and researchers in materials science, physics, chemistry, and engineering.
Rolling is an important metal forming process which involves the passing of metal stock through a pair of rollers. It is categorized depending on the recrystallization temperature of the metal rolled. This book covers the entire gamut of rolling technology in one volume. It begins with a brief history of rolling, and goes on to discuss different rolling processes, the deformation of materials, and the classification of rolling mills and stands. The book discusses rolling applications of steel blooms, slabs, bars, plates, rods, heavy sections and non-ferrous metals in detail. It covers important rolling process parameters, including rolling friction, stress and strain across rolled strip thickness, rolling torque and power and roll separation force. It also provides details on the design and applications of various rolling equipment, including mill rolls, neck bearings, spindles, coilers and decoilers.
In this chapter we describe synthetic polymeric fibers, which saw tremendous advancement in the last half of the twentieth century. In fact, a reasonable case can be made that the so-called age of fibers began with the advent of synthetic fibers such as nylon, polyester, etc. in the late 1930s and early 1940s. Many companies such as DuPont, Monsanto, BASF, Hoechst, ICI, etc. contributed very heavily in this area. For a historical account of the scientific and technological progress made in this area, the reader is referred to a study of research and development activities at DuPont during the period of 1902–1980 (Hounshell and Smith, 1988). Most of these synthetic polymeric fibers such as polyester, nylon, etc. have very uniform and reproducible properties. They have a rather low elastic modulus, however, which restricts them mostly to the apparel or textile market. It was the research work aimed at making strong and stiff synthetic polymeric fibers for use as reinforcements in polymers, which started sometime in the late 1960s, that resulted in the commercial availability of strong and stiff fibers such as aramid and polyethylene. We describe below the processing, structure, and properties of some important synthetic polymeric fibers in some detail.
The age of synthetic polymeric fibers
A brief historical review of the work in the area of organic fibers will be helpful in placing things in perspective. We begin with the discovery of nylon, also known as polyamide (PA). Nylon was discovered and commercialized by DuPont in 1938 (Magat and Morrison, 1976). Wallace Carrothers of DuPont is generally regarded as the father of nylon. Nylon first penetrated the silk hosiery market just before the start of World War II. In fact, 1988 marked the 50th anniversary of the introduction of nylon silk stockings. Nylon is made by melt spinning. It is a very flexible, knittable, and durable fiber; all these attributes have made it one of the most important fibers for the textile industry. Nylon's reasonably high strength, good impact, and fatigue resistance also led to its use in the tire industry. It should be noted that the term nylon is a generic term that represents a group of similar materials, in the same vein as glass, steel, or carbon. Accordingly, we spell it without a capital letter.
We devote a whole chapter to fibers produced by a process called electrospinning. Although the process is thought to have originated in the early twentieth century, it was not until 1995 when Doshi and Reneker (1995) sort of rediscovered the process and used the term electrospinning for the process. Reneker and his group are credited with pointing out the diverse range of applications for electrospun nanofibers. It is a very versatile technique for making nanofibers, generally polymeric fibers although ceramic fibers have also been made by this technique. Most electrospun fibers are nanofibers because their diameters are less than 100 nm. There has been a tremendous increase in the use of the electrospinning technique and applications of nanofibers produced in fields as diverse as health care and filtration in aggressive environments (Laudenslager and Sigmund, 2015). The starting material can be in solution form or melt form. There are essentially three components in the process: a high voltage supply, a capillary tube with a needle, and a screen to collect the fibers. The high voltage creates an electrically charged jet of polymer solution or melt out of the needle. The solvent in the jet evaporates (or if a melt is used, it solidifies) and an interconnected web of small fibers is collected on the collector screen. Initially, this technique was used for making polymeric nanofibers. The technique has been used for the preparation of metal oxide/ceramic nanofibers; e.g., silica, zirconia, titania, nickel oxide, barium titanate, lead zirconate titanate, and other oxide materials (Ramakrishna et al., 2005).
It turns out that fibrous nanomaterials or nanofibers as processed by electrospinning are attractive for many applications because of their intrinsically high porosities and large surface areas. Porosity or voids in materials, as highlighted by Gladysz and Chawla (2014), are not always undesirable. Electrospinning is a simple, versatile technique for generating nanofibers from a variety of materials.
In this chapter, we describe the basic process of electrospinning, followed by some examples of nanofibrous structures produced by this process and applications of electrospun nanofibers.
Basic process
Under the action of an electrostatic field, a droplet of a conducting polymer solution at the tip of a capillary is deformed into a conical shape; this shape is called the Taylor cone. The Taylor cone is formed because of equilibrium between the surface tension of the droplet and the applied electric field. Figure 5.1 shows the Taylor cone schematically.