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Online since: June 2012
Authors: Li Bo Wang, Ai Guo Zhou, Fei Xiang Hu, Liang Li
Introduction
Titanium silicon carbide (Ti3SiC2) combines the properties of metals and ceramics [1, 2].
Like other ceramic materials, it possesses good high temperature mechanical properties and oxidation resistance [4].
El-Raghy, et al, Tensile properties of Ti3SiC2 in the 25-1300°C temperature range, Acta Mater. 48 (2000) 453-459
Zhai, Synthesis and reaction mechanism of Ti3SiC2 by mechanical alloying of elemental Ti, Si, and C powders, J.
Like other ceramic materials, it possesses good high temperature mechanical properties and oxidation resistance [4].
El-Raghy, et al, Tensile properties of Ti3SiC2 in the 25-1300°C temperature range, Acta Mater. 48 (2000) 453-459
Zhai, Synthesis and reaction mechanism of Ti3SiC2 by mechanical alloying of elemental Ti, Si, and C powders, J.
Online since: June 2022
Authors: Silviana Silviana, Amar Ma'ruf, Febio Dalanta
The resulting silica still contained metal impurities and their presents affected the properties and quality of processed silica [4].
The electrochemical properties of the battery were checked in a glove box containing argon (Ar).
Santos, Characterization and properties of blended cement matrices containing activated bamboo leaf wastes, Cement and Concrete Composites. 34 (2012) 1019–1023
Mamat, A critical assessment and new research directions of rice husk silica processing methods and properties, Maejo Int.
Fray, Black silicon: Fabrication methods, properties and solar energy applications, Energy and Environmental Science. 7 (2014) 3223–3263
The electrochemical properties of the battery were checked in a glove box containing argon (Ar).
Santos, Characterization and properties of blended cement matrices containing activated bamboo leaf wastes, Cement and Concrete Composites. 34 (2012) 1019–1023
Mamat, A critical assessment and new research directions of rice husk silica processing methods and properties, Maejo Int.
Fray, Black silicon: Fabrication methods, properties and solar energy applications, Energy and Environmental Science. 7 (2014) 3223–3263
Online since: September 2010
Authors: Traian V. Chirila, Andrew K. Whittaker, Lynette Lambert, Imelda Keen, Stefan M. Paterson
For instance, the nature and extent of crosslinking in hydrogels may have a significant effect on
their swelling capacity, mechanical properties and ability to degrade, which are all features of
importance in various applications.
Due to their large range of properties and to the possibilities to manipulate them, the hydrogels have a prominent position as biomaterials.
Based on extensive studies on the excretion of uncrosslinked poly(1-vinyl-2-pyrrolidinone) (PVP), comprehensively reviewed by Robinson et al. [45], it appears that for a synthetic polymer with a C−C backbone administered to the body by injection or implantation, MW is a governing factor in its clearance by renal excretion.
We believe that solubility in water of the residual polymer fragments remaining after the cleavage of the crosslinks is a factor that may facilitate their elimination through renal pathways.
Similar kinetic curve profiles obtained by FT-NIR spectroscopy for the polymerization of HEMA with and without PEGDMA suggested that the addition of a small amount of the crosslinking agent has not affected the rate of RAFT polymerization of HEMA.
Due to their large range of properties and to the possibilities to manipulate them, the hydrogels have a prominent position as biomaterials.
Based on extensive studies on the excretion of uncrosslinked poly(1-vinyl-2-pyrrolidinone) (PVP), comprehensively reviewed by Robinson et al. [45], it appears that for a synthetic polymer with a C−C backbone administered to the body by injection or implantation, MW is a governing factor in its clearance by renal excretion.
We believe that solubility in water of the residual polymer fragments remaining after the cleavage of the crosslinks is a factor that may facilitate their elimination through renal pathways.
Similar kinetic curve profiles obtained by FT-NIR spectroscopy for the polymerization of HEMA with and without PEGDMA suggested that the addition of a small amount of the crosslinking agent has not affected the rate of RAFT polymerization of HEMA.
Online since: July 2025
Authors: Sergey V. Stepanov, Liliya I. Budaeva, Olga V. Ilyukhina
An external electric field can affect only
the positrons that are outside the blob, Fig. 3.
All these factors indicate that the Ore mechanism is ineffective in condensed media [15].
Capture of the hydrated electrons by NO−3 ions (which definitely takes place in the e+ blob) does not affect at all the qf-Ps formation probability [25].
The growth of the Ps bubble is driven by the quantum mechanical pressure exerted by the e+e− pair inside the bubble.
HB = −ˆµ ˆB = e mcB(ˆsze − ˆszp). (40)Here ˆµ is the operator of the magnetic moment of the pair, and the spin operators ˆsze and ˆszp (in essence, they are just the Pauli matrices) have the following obvious properties (for the positron and electron, respectively): ˆsz| ↑i = ¯h 2| ↑i, ˆsz| ↓i = −¯h 2| ↓i, ˆsz = ¯h 2 �1 0 0 −1 � , | ↑i = �1 0 � , | ↓i = �0 1 � . (41) The arrows | ↑i and | ↓i mean that the spin of the particle (electron or positron) is directed either up (ms = 1 2), or down (ms = −12).
All these factors indicate that the Ore mechanism is ineffective in condensed media [15].
Capture of the hydrated electrons by NO−3 ions (which definitely takes place in the e+ blob) does not affect at all the qf-Ps formation probability [25].
The growth of the Ps bubble is driven by the quantum mechanical pressure exerted by the e+e− pair inside the bubble.
HB = −ˆµ ˆB = e mcB(ˆsze − ˆszp). (40)Here ˆµ is the operator of the magnetic moment of the pair, and the spin operators ˆsze and ˆszp (in essence, they are just the Pauli matrices) have the following obvious properties (for the positron and electron, respectively): ˆsz| ↑i = ¯h 2| ↑i, ˆsz| ↓i = −¯h 2| ↓i, ˆsz = ¯h 2 �1 0 0 −1 � , | ↑i = �1 0 � , | ↓i = �0 1 � . (41) The arrows | ↑i and | ↓i mean that the spin of the particle (electron or positron) is directed either up (ms = 1 2), or down (ms = −12).
Online since: May 2009
Authors: H.M. Lu
The properties of a solid are essentially controlled by related
surface/interface energies.
The so-called computation materials science considers the interface properties from three different size scales [2]: 1.
Indeed in many cases, experimental data on nanoparticle properties are rather scanty and contradictory.
Semiempirical predictions based on the correlation between the surface and bulk thermodynamic properties are always active [194,195,196,197].
Raabe: Computational materials science: the simulation of materials, microstructures and properties (Wiley-VCH, Weinheim 1998)
The so-called computation materials science considers the interface properties from three different size scales [2]: 1.
Indeed in many cases, experimental data on nanoparticle properties are rather scanty and contradictory.
Semiempirical predictions based on the correlation between the surface and bulk thermodynamic properties are always active [194,195,196,197].
Raabe: Computational materials science: the simulation of materials, microstructures and properties (Wiley-VCH, Weinheim 1998)
Online since: March 2022
Authors: Peter Anuoluwapo Gbadega, Akshay Kumar Saha
However, power generation from clean energy sources (RESs) such as wind energy has been affected by environmental and geographical factors, resulting in a mismatch between supply and demand [4].
As a consequence, the amount of energy converted by the cells is influenced by temperature, material properties, and solar radiation.
Similarly, the mathematical equations that model the kinetic energy generated by the dynamic system, the corresponding mechanical torque and wind turbine power, the turbine power coefficient of the wind turbine system used in this paper are taken from our previous work in refs [32, 33].
is the sum of the following terms: Velz,0cellt=Eelz0+∆Selz02FTelzt-Telz0+2.3RTelzt2FlnPH2tPO212tPH2Ot (15) Velz,actcellt=RTelztFsinh-1Ielzt2Aelzia0,elz+sinh-1Ielzt2Aelzic0,elz (16) Velz,ohmcellt=IelztRohm (17) Velz,conccellt=K1,elzconceK2,elzconcIelzt (18) Where Telzt is the electrolyser temperature, Telz0 is the temperature in standard conditions, ∆Selz0 is the entropy change, R and F are ideal gas and Faraday constant respectively, PO2 is the oxygen partial pressure, PH2 is the hydrogen partial pressure, Ielz is the electrolyser current, ia0,elz and ic0,elz are the anode and cathode current densities respectively, and K1,elzconc and K2,elzconc are the concentration-losses factors
The energy profile sold to the external grid, and the lifespan of the battery is directly affected by the irradiance oscillation, which is caused by the cloudy weather.
As a consequence, the amount of energy converted by the cells is influenced by temperature, material properties, and solar radiation.
Similarly, the mathematical equations that model the kinetic energy generated by the dynamic system, the corresponding mechanical torque and wind turbine power, the turbine power coefficient of the wind turbine system used in this paper are taken from our previous work in refs [32, 33].
is the sum of the following terms: Velz,0cellt=Eelz0+∆Selz02FTelzt-Telz0+2.3RTelzt2FlnPH2tPO212tPH2Ot (15) Velz,actcellt=RTelztFsinh-1Ielzt2Aelzia0,elz+sinh-1Ielzt2Aelzic0,elz (16) Velz,ohmcellt=IelztRohm (17) Velz,conccellt=K1,elzconceK2,elzconcIelzt (18) Where Telzt is the electrolyser temperature, Telz0 is the temperature in standard conditions, ∆Selz0 is the entropy change, R and F are ideal gas and Faraday constant respectively, PO2 is the oxygen partial pressure, PH2 is the hydrogen partial pressure, Ielz is the electrolyser current, ia0,elz and ic0,elz are the anode and cathode current densities respectively, and K1,elzconc and K2,elzconc are the concentration-losses factors
The energy profile sold to the external grid, and the lifespan of the battery is directly affected by the irradiance oscillation, which is caused by the cloudy weather.
Online since: August 2017
Authors: Ralf Müller, Alexander Schlüter, Charlotte Kuhn, Timo Noll, Felix Diewald
Ee = ∫
Ω ψe (ε, s) dV . (8)
The constitutive behaviour is determined by the definition of the strain energy density
ψe (ε, s) = ψe− (ε) + g(s)ψe+ (ε) . (9)
The strain energy density is decomposed in a crack driving, strain part ψe+ that is affected by the degradation
function g(s) and a part that is associated with compressive strain states ψe−.
The compressive strain energy is not affected by g(s) which models the impenetrability of cracks during crack closure, i.e. no degradation of the 'compressive' stress see (17).
The stress is σ = ∂ψe ∂ε = ∂ψe− ∂ε + g(s)∂ψe+ ∂ε . (17) The wave speed of dilatational waves in the considered elastic medium is cd = √λ + 2µ ρ . (18) The total kinetic energy of the body is assumed not to be affected by the phase field, i.e K( ˙u) = ∫ Ω 1 2ρ ˙u · ˙u dV . (19) The work of external forces acting on the boundary ∂Ω reads P = ∫ ∂Ωt t∗ · u dA. (20) Finally, the dynamic fracture problem can be stated using Hamilton's principle δ t2∫ t1 L dt = 0, (21) for arbitrary times t1 < t2, where the Lagrangian is given by L = K − (Ee + Es − P). (22) For the problem at hand, the Euler-Lagrange equations following from (21) are the equation of motion ρ¨u − divσ = 0, (23) Applied Mechanics and Materials Vol. 869 103and the phase field equation g'(s)ψ+e − Gc [ 2ϵ∆s + 1 − s 2ϵ ] = 0 (24) as well as the Neumann boundary conditions for the displacement σn = t∗ on ∂Ωt (25) and for the phase field ∇s · n = 0 on ∂Ω. (26) In (24) it becomes apparent, that the property
The factor δ further reduces the allowable time step and accounts for nonlinear effects.
Development of Non-standard Discretization Methods, Mechanical and Mathematical Analysis" References [1] Ambati, M., Gerasimov, T., Lorenzis, L. (2015).
The compressive strain energy is not affected by g(s) which models the impenetrability of cracks during crack closure, i.e. no degradation of the 'compressive' stress see (17).
The stress is σ = ∂ψe ∂ε = ∂ψe− ∂ε + g(s)∂ψe+ ∂ε . (17) The wave speed of dilatational waves in the considered elastic medium is cd = √λ + 2µ ρ . (18) The total kinetic energy of the body is assumed not to be affected by the phase field, i.e K( ˙u) = ∫ Ω 1 2ρ ˙u · ˙u dV . (19) The work of external forces acting on the boundary ∂Ω reads P = ∫ ∂Ωt t∗ · u dA. (20) Finally, the dynamic fracture problem can be stated using Hamilton's principle δ t2∫ t1 L dt = 0, (21) for arbitrary times t1 < t2, where the Lagrangian is given by L = K − (Ee + Es − P). (22) For the problem at hand, the Euler-Lagrange equations following from (21) are the equation of motion ρ¨u − divσ = 0, (23) Applied Mechanics and Materials Vol. 869 103and the phase field equation g'(s)ψ+e − Gc [ 2ϵ∆s + 1 − s 2ϵ ] = 0 (24) as well as the Neumann boundary conditions for the displacement σn = t∗ on ∂Ωt (25) and for the phase field ∇s · n = 0 on ∂Ω. (26) In (24) it becomes apparent, that the property
The factor δ further reduces the allowable time step and accounts for nonlinear effects.
Development of Non-standard Discretization Methods, Mechanical and Mathematical Analysis" References [1] Ambati, M., Gerasimov, T., Lorenzis, L. (2015).
Online since: July 2015
Authors: Rukshana I. Kureshy, Wan Kuen Jo, Rajesh J. Tayade, Kalithasan Natarajan, Thillai Sivakumar Natarajan, Hari C. Bajaj
The efficient photocatalytic H2 production has been majorly relies on the properties of the photocatalyst used for the reaction.
Nevertheless it is apparently reveals that H2 production efficiency is relying on the properties of semiconductor TiO2 photocatalyst.
Hawai, Catalytic properties of ruthenium oxide on n-type semiconductors under illumination, J.
Ma, Photoelectrical and charge transfer properties of hydrogen evolving TiO2 nanotube arrays electrodes annealed in different gases, Int.
Lee, Preparation of highly ordered cubic mesoporous WO3/TiO2 films and their photocatalytic properties, Chem.
Nevertheless it is apparently reveals that H2 production efficiency is relying on the properties of semiconductor TiO2 photocatalyst.
Hawai, Catalytic properties of ruthenium oxide on n-type semiconductors under illumination, J.
Ma, Photoelectrical and charge transfer properties of hydrogen evolving TiO2 nanotube arrays electrodes annealed in different gases, Int.
Lee, Preparation of highly ordered cubic mesoporous WO3/TiO2 films and their photocatalytic properties, Chem.
Online since: March 2019
Authors: Aloke Paul
The reactive diffusion process is followed to grow tungsten disilicides for the use as integrated circuits due to their beneficial properties of low electrical resistivity and good thermal stability.
Other than the importance of understanding the diffusion-controlled growth process, the estimation of the diffusion coefficients is important to understanding many physical and mechanical properties of materials.
Bulk diffusion couple experiments are important for an extensive analysis of the diffusion process without the influence of other factors.
On the other hand, the growth kinetics is affected when it grows along with other phases.
Study on diffusion is important for developing indepth understanding of many properties.
Other than the importance of understanding the diffusion-controlled growth process, the estimation of the diffusion coefficients is important to understanding many physical and mechanical properties of materials.
Bulk diffusion couple experiments are important for an extensive analysis of the diffusion process without the influence of other factors.
On the other hand, the growth kinetics is affected when it grows along with other phases.
Study on diffusion is important for developing indepth understanding of many properties.