Effect of Al content on impact resistance behavior of Al-Ti-B4C composite fabricated under air atmosphere

Reaction behavior, mechanical property and impact resistance of TiC-TiB₂/Al composite reacted from Al-Ti-B₄C system with various Al content via combination method of combustion synthesis and hot pressed sintering under air was investigated. Al content was the key point to the variation of mechanical property and impact resistance. Increasing Al content could increase the density, strength and toughness of the composite. Due to exorbitant ceramic content, 10 wt.% and 20 wt.% Al-Ti-B₄C composites exhibited poor molding ability and machinability. Flexural strength, fracture toughness, compressive strength and impact toughness of 30–50 wt.% Al-Ti-B₄C composite were higher than those of Al matrix. The intergranular fracture dispersed and defused impact load and restricted crack extension, enhancing the impact resistance of the composite. The composite with 50 wt.% Al content owned highest mechanical properties and impact resistance. The results were useful for the application of TiC-TiB₂/Al composite in impact resistance field of ceramic reinforced Al matrix composite.     

Effect of B4C diffusion barriers on the thermal stability of Sc/Si periodic multilayers

The optical properties of Sc/Si periodic multilayers are analyzed at three wavelengths in the X-ray range: 0.154, 0.712 and 12.7 nm. Fitting the reflectivity curves obtained at these three wavelengths enable us to constrain the parameters, thickness, density and roughness of the various layers, of the studied multilayers. Scattering curves were also measured at 12.7 nm on some samples to obtain an estimate of the correlation length of the roughness. Two sets of multilayers are used, with and without B₄C diffusion barrier at the interfaces. To see the efficiency of the B₄C layers the measures are performed after annealing up to 400 °C. A dramatic change of the structure of the Sc/Si multilayer is observed between 100 and 200 °C leading to a strong loss of reflectivity. For the Sc/B₄C/Si/B₄C multilayer the structure is stable up to 200 °C after which a progressive evolution of the stack occurs.     

Magnetic properties of nanocrystalline Fe86.7Zr3.3B4Ag6 thin film

The changes of magnetic properties with annealing temperature were studied in the amorphous Fe_86.7Zr_3.3B₄Ag₆ thin film. The thin films were deposited by a DC magnetron sputtering method, annealed at 300–700°C for 1 h in vacuum under a field of 1.5 kOe parallel to the film plane, and then furnace-cooled. As a result, it has been found that the Ag addition to Fe–Zr–B amorphous thin films resulted in the decrease of crystallization temperature to 400°C due to promoted crystallization ability. Also, it gave rise to formation of fine BCC α-Fe crystalline precipitates with a grain size smaller than 10 nm in the amorphous matrix near 400°C, and led to prominent enhancement in the magnetic properties of the Fe_86.7Zr_3.3B₄Ag₆ thin films. Significantly, excellent magnetic properties such as a saturation magnetization of 1.7 T, a coercive force of 1 Oe and a permeability of 7800 at 50 MHz were obtained in the amorphous Fe_86.7Zr_3.3B₄Ag₆ thin film containing 7.2 nm-size BCC α-Fe, which was annealed at 400°C. Also, core loss of 1.4 W cm⁻³ (B_m=0.1 T) at 1 MHz in the thin film was obtained, and it is a much lower value than had been obtained in any existing soft magnetic materials. Such excellent properties are inferred to originate from the uniform dispersion of nano-size BCC α-Fe in the amorphous matrix.     

Accumulating evidence for the two-step magnetic ordering in the borocarbides DyNi2B2C and DyCo2B2C

Accumulating evidence for a two-step magnetic ordering in the borocarbide DyNi₂B₂C is summarized, including earlier overlooked evidence for the initial magnetic transition and a recent magnetization study of polycrystalline samples. The two-step ordering involves initial two-dimensional ferromagnetic ordering in the DyC (basal) planes at T_N (=16.3 K), gradual build-up of the three-dimensional (3D) alternate stacking of ferromagnetic planes, and a final 3D ordering in the AF–I-related structure at a lower temperature T_o (=10.4 K), depicting a first-order transition. Supporting evidence for the two-step magnetic ordering in DyNi₂B₂C comes from point-contact spectroscopy measurements in the normal state for DyNi₂B₂C–Ag contact, and from similar behaviour of PrNi₂B₂C and (Pr_0.91Dy_0.09)Ni₂B₂C. In the isostructural borocarbide DyCo₂B₂C the two magnetic transitions (at 7.8 and 2.6 K) deduced from the specific-heat measurements are also attributed to a two-step magnetic ordering.     

Frequency and temperature-dependent electrical properties of LiNi3/5Fe2/5VO4 studied by complex impedance spectroscopy

The LiNi_3/5Fe_2/5VO₄ has been synthesized by solution-based chemical method. Grain morphology of the material is investigated using field emission scanning electron microscopy. The existence of electrical conduction due to bulk and grain boundary effects at 21, 75 and 250 °C, and grain boundary and polarization effects at 275 and 300 °C has been verified by impedance spectroscopy. DC conductivity shows electrical conduction in the material as a thermally activated process. The frequency dependence of AC conductivity is described by Jonscher's power law.     

TiB2-reinforced B4C composites produced by reaction sintering at high-pressure and high temperature

ABSTRACT

Obtaining both high hardness and toughness is a challenge in B₄C-nano-adhesive composites. Solving the inhomogeneous distribution of nano-adhesives in B₄C and forming the chemical bonding at grain boundary is an effective method. Here, we reported that the uniform distribution of titanium diboride (TiB₂)-reinforced B₄C composites synthesized by high-pressure and high temperature (HPHT). It is found that HPHT sintering can effectively inhibit the grain growth and increase the relative density. Moreover, HPHT sintering can cross high reaction energy barrier and effectively promote the formation of chemical bonding at grain boundary between B₄C and TiB₂. The optimal hardness and toughness value reach 30.0?±?0.9?GPa and 7.87?MPa·m^1/2, respectively. The improvement of hardness and toughness in the final products are ascribed to the strengthening of nanoTiB₂ connection of B₄C boundary and intergranular fracture mechanism. This work suggests a new way to achieve the uniform distribution of nanoTiB₂ in B₄C and form the chemical bonding at grain boundary, which is of great significance to the further development of TiB₂-reinforced B₄C composites with excellent mechanical properties.     

Crystal chemistry and physical properties of the ternary compounds RE5B4C5 (RE=Ce,Pr, Nd)

The ternary rare-earth metal boride carbides RE₅B₄C₅ (RE=Ce, Pr, Nd) were prepared by arc melting the mixtures of the pure elements and subsequent annealing at 1270 K. Their crystal structures were determined from single crystal X-ray diffraction data. They crystallize in the Ce₅B₄C₅ type of structure (space group Pna2₁, Z=8). Two new compounds were found, Pr₅B₄C₅: a=24.592(2) Å, b=8.4563(5) Å, c=8.4918(5) Å, R₁=0.043 (wR₂=0.076) for 2871 reflections with I_o?2σ(I_o)); for Nd₅B₄C₅: a=24.301(1) Å, b=8.3126(5) Å, c=8.3545(4) Å, R₁=0.035 (wR₂=0.069) for 3707 reflections with I_o?2σ(I_o)). Its structural arrangement consists of a three-dimensional framework of rare-earth atoms resulting from the stacking of slightly corrugated two-dimensional square nets, leading to voids filled with B₄C₄, B₃C₃, BC₂ finite chains and isolated carbon atoms. Ce₅B₄C₅ is an antiferromagnet at 5 K followed by a metamagnetic transition in elevated external fields. Pr₅B₄C₅ and Nd₅B₄C₅ are ferromagnets below T_C=12 and 15 K, respectively.     

Synthesis and electrochemical properties of Li2S–B2S3–Li4SiO4

New Li⁺ ion-conductive glasses Li₂S–B₂S₃–Li₄SiO₄ were synthesized by rapid quenching, and they were transformed into glass ceramics by heat treatment. The heat treatment increased the ionic conductivities of the Li₄SiO₄-doped glasses, and the highest ionic conductivity observed in the system was 1.0 × 10^− 3 S cm^− 1 at room temperature. The glass ceramics were highly stable against electrochemical oxidation with a wide electrochemical window of 10 V.     

A novel approach to accelerate the reaction between Ti and Al

Pure Ti foils and SiCp/Al composite foils were employed to investigate the parabolic growth kinetics of TiAl₃ at 660 °C. Compared with pure Al foils, the introduction of SiC particles significantly refined TiAl₃ grain size by the solid solution of silicon. Corresponding refinement mechanisms were concluded from the perspective of the nucleation of TiAl₃. Micromechanics analysis shows that the fine TiAl₃ grains own a small viscous resistance, and subsequently an improvement in the reaction rate could be achieved. This meaningful law also applies extensively to Ni/Al and Fe/Al systems.     

Influence of local environment on electronic properties of Co atoms in the Tm3Co11B4 compound

The electronic structure of the Tm₃Co₁₁B₄ compound has been studied by X-ray photoemission spectroscopy and ab initio self-consistent tight binding linear muffin tin orbital (TB LMTO) method. This compound crystallizes in the hexagonal Ce₃Co₁₁B₄-type structure (P6/mmm). We have found a good agreement between the experimental XPS valence band spectra and theoretical ab initio calculations. The calculated total magnetic moment is equal to 13.635 μ_B/f.u. The magnetic moments on the Co atoms are antiparallel to the moments of the Tm atoms. Their values are depended on the local environment, especially on the number of the Co neighbors. The theoretical results are compared with other calculations, saturation magnetization measurements as well as neutron diffraction data for R₃Co₁₁B₄ (R=Y, Nd, Gd, Tb).     

Interfacial microstructure and growth mechanism of Al4C3 in Grf/Al composites fabricated by liquid pressure method

In this study, Gr_f/Al composite was fabricated by liquid pressure method. The diffusion layer and the nucleation and growth of Al₄C₃ were observed at the interface of Gr_f/Al composites by TEM and HRTEM. The growth mechanism of Al₄C₃ was analyzed in detail by crystallography theory. It was found that Al₄C₃ had no phase relations with the carbon fiber. (0 0 0 1) layer of Al₄C₃ was parallel with main growth direction. Both the diffusion layer at the interface and crystal structure of Al₄C₃ affected the shape of Al₄C₃. At a certain position, Al₄C₃ could connect two fibers when the fibers were close to each other.     

Determining the effect of grain size and maximum induction upon coercive field of electrical steels

Although theoretical models have already been proposed, experimental data is still lacking to quantify the influence of grain size upon coercivity of electrical steels. Some authors consider a linear inverse proportionality, while others suggest a square root inverse proportionality. Results also differ with regard to the slope of the reciprocal of grain size–coercive field relation for a given material. This paper discusses two aspects of the problem: the maximum induction used for determining coercive force and the possible effect of lurking variables such as the grain size distribution breadth and crystallographic texture. Electrical steel sheets containing 0.7% Si, 0.3% Al and 24 ppm C were cold-rolled and annealed in order to produce different grain sizes (ranging from 20 to 150 μm). Coercive field was measured along the rolling direction and found to depend linearly on reciprocal of grain size with a slope of approximately 0.9 (A/m)mm at 1.0 T induction. A general relation for coercive field as a function of grain size and maximum induction was established, yielding an average absolute error below 4%. Through measurement of B₅₀ and image analysis of micrographs, the effects of crystallographic texture and grain size distribution breadth were qualitatively discussed.     

Enhanced piezoelectric properties and lowered sintering temperature of Ba(Zr0.07Ti0.93)O3 by B2O3 addition

The effects of B₂O₃ doping on densification, ferroelectric, and piezoelectric properties of Ba(Zr_0.07Ti_0.93)O₃(BZT) ceramics were investigated. The addition of B₂O₃ to the ceramics lowered the sintering temperature by ∼200 °C as well as changed their microstructures. Higher B₂O₃ concentration caused a decrease in remanent polarization and coercive field, while the piezoelectric coefficient d₃₃ remained at a high value of 291 pC/N for the ceramic sample with 2 wt.% B₂O₃. The relationship between piezoelectric properties and ferroelectric constant was examined.     

Photo-luminescence properties of Cu and Ag doped Li2B4O7 single crystals at low temperatures

UV excited photo luminescence from Li₂B₄O₇:Cu and Li₂B₄O₇:Cu, Ag single crystals has been investigated in the temperature range from 77 K to 300 K. An excitation band having a doublet structure at 240 nm and 262 nm was observed for the emission at 370 nm that corresponds to ¹A_1g→¹E_g and ¹A_1g→¹T_2g crystal field components of the 3d¹⁰→3d⁹4s¹ transition of Cu⁺. The relative intensity of these components and their temperature dependence provide a measure of the off-center displacement of the Cu⁺ ground state in the crystal lattice site. The co-doped Ag plays a role of a sensitizer when doped with Cu and increases the overall emission as the emission between Ag states lies in the excitation region of Cu states. The 370 nm emission in both the crystals slightly decreases with temperature; however a sudden increase in the intensity around 264 K was observed.     

Obtaining Ca(H2PO4)2·H2O,monocalcium phosphate monohydrate,via monetite from brushite by using sonication

Brushite was synthesized by precipitation of calcium chloride (CaCl₂) and sodium phosphate monobasic (Na₂HPO₄) dried in vacuum and monetite was obtained from this brushite by sonication with a frequency of 90 kHz at 500 W for 90 min. Monetite itself was also transformed in Ca(H₂PO₄)₂·H₂O, monocalcium phosphate monohydrate (MCPM), by sonication with a frequency of 90 kHz at 500 W for 60 min followed by lyophilization. The MCPM was sonicated and lyophilized by three times more until reach over 240 min, but any other phase transformation was observed. All these phase transformations were analyzed by X-ray diffraction (XRD) and infrared spectroscopy (FTIR). Scanning electron microscopy (SEM) and transmission electron microscopy (TEM) indicated a grain size of about 200 nm in all the samples. The morphology observed was a corn-flake-like grain for brushite, a pseudo-needle-like grains for monetite, and lamellar-like grains for MCPM.     

Studies of structural and electrical properties on four-layers Aurivillius phase BaBi4Ti4O15

BaBi₄Ti₄O₁₅ (BBT) ceramic was synthesized using mixed oxide route and the structural and electrical properties were investigated systematically. The structural studies confirmed it to be an n=4 member of the Aurivillius oxide. A broad dielectric peak with frequency dependent dielectric maximum temperature was observed. The dielectric relaxation obeyed the Vogel–Fulcher relation wherein f₀=8.37E+14 Hz, E_a=0.13 eV, and T_f=608.18 K. The diffuseness parameter γ established the relaxor nature and it was attributed to the A-site cationic disorder. The specimen exhibited the excellent reproducibility in the measurements of displacement current, a remnant polarization of 5.4 μC/cm², and a coercive field of 4.03 MV/m. The room temperature piezoelectric coefficient d₃₃ was found to be 23 pC/N and the field-induced strain S was about 0.018% at the 8 MV/m electric field.     

Influence of B2O3 on microstructure and microwave dielectric properties of 0.4Nd(Mg0.4Zn0.1Sn0.5)O3–0.6Ca0.8Sr0.2TiO3 ceramic system

The effects of B₂O₃ on the microstructure and microwave dielectric properties of the 0.4Nd(Mg_0.4Zn_0.1Sn_0.5)O₃–0.6Ca_0.8Sr_0.2TiO₃ ceramic system were investigated with a view to their use in microwave devices. A B₂O₃-doped 0.4Nd(Mg_0.4Zn_0.1Sn_0.5)O₃–0.6Ca_0.8Sr_0.2TiO₃ ceramic system was prepared by the conventional solid-state method. The X-ray diffraction patterns of the B₂O₃-doped 0.4Nd(Mg_0.4Zn_0.1Sn_0.5)O₃–0.6Ca_0.8Sr_0.2TiO₃ ceramic system did not significantly vary with sintering temperature. A 0.5 wt% B₂O₃-doped 0.4Nd(Mg_0.4Zn_0.1Sn_0.5)O₃–0.6Ca_0.8Sr_0.2TiO₃ ceramic system that was sintered at 1350 °C for 4 h had a dielectric constant of 38.3, a quality factor Qf of 35,000 GHz, and a temperature coefficient of resonant frequency of ?4.8 ppm/°C.     

Ultrasonic cavitation erosion of gas nitrided Ti–6Al–4V alloys

Ultrasonic cavitation erosion experiments were performed on Ti–6Al–4V alloys samples in annealed, nitrided and nitrided and subsequently heat treated state. The protective oxide layer formed as a result of annealing and heat treatment after nitriding is eliminated after less than 30 min cavitation time, while the nitride layer lasts up to 90 min cavitation time. Once the protective layer is removed, the cavitation process develops by grain boundary erosion, leading to the expulsion of grains from the surface. The gas nitrided Ti–6Al–4V alloy, forming a Ti_xN surface layer, proved to be a better solution to improve the cavitation erosion resistance, compared to the annealed and nitrided and heat treated state, respectively. The analysis of the mean depth of erosion rate at 165 min cavitation time showed an improvement of the cavitation erosion resistance of the nitrided samples of up to 77% higher compared to the one of the annealed samples.     

Effect of processing temperature on the superconducting properties of acetone doped MgB2 tapes

Correlation of phase formation, critical transition temperature T_c, microstructure, and critical current density J_c with sintering temperature has been studied for acetone doped MgB₂/Fe tapes. Sintering was performed at 600–850 °C for 1 h in a flowing Ar atmosphere. High boron substitution by carbon was obtained with increasing the sintering temperature; however, the acetone doped samples synthesized at 800 °C contain large size MgB₂ grains and more MgO impurities. Incomplete reaction for the acetone doped samples heated at 600 °C result in bad intergrain connectivity. At 4.2 K, the best J_c value was achieved in the acetone doped sample sintered at 700 °C, which reached 24,000 A/cm² at 10 T and 10,000 A/cm² at 12 T, respectively. Our results indicate that the small grain size and less impurity were also important for the improvement of J_c–B properties besides the substitutions of B by C.