24 research outputs found
Carbon footprint of Power-to-X derived dimethyl ether using the sorption enhanced DME synthesis process
Dimethyl ether (DME) could have a promising future as a sustainable diesel fuel replacement as it requires only relatively minor engine modifications. It can be produced from renewable H2 and captured CO2 using Power-to-X technologies. To gain support through the EU Renewable Energy Directive, the production and use of CO2-derived DME as a fuel needs to produce emission savings of at least 70% over the petrodiesel alternative. This study assesses the carbon footprint of producing DME via the sorption-enhanced DME synthesis (SEDMES) process and using it as a transport fuel, compared to producing and using fossil-based petrodiesel. The cradle-to-grave (well-to-wheel) carbon footprint of using DME as a transport fuel is found to be 77% lower than for petrodiesel, if offshore wind power is used for H2 synthesis and DME production. If renewable energy is also used for CO2 capture and waste heat is used for the DME production and purification steps, the DME carbon footprint has the potential to be over 90% lower than that of the fossil-fuel comparator
A clinical case of demyelinating lesions of the brain: Central pontine myelinolysis
In the scientific review a rare demielinizirute disease of the brain - central pontine myelinolysis is presented. Prior to the introduction of the technique of visualization, diagnosis of the disease was through autopsy. Clinical case, which describes the variety neurological and somatic symptoms, was presented. The attention is focused on the importance of an integrated approach to diagnosis and management of the patient with the disease.Π Π½Π°ΡΡΠ½ΠΎΠΌ ΠΎΠ±Π·ΠΎΡΠ΅ ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ΠΎ ΡΠ΅Π΄ΠΊΠΎΠ΅ Π΄Π΅ΠΌΠΈΠ΅Π»ΠΈΠ½ΠΈΠ·ΡΡΡΡΠ΅Π΅ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠ΅ Π³ΠΎΠ»ΠΎΠ²Π½ΠΎΠ³ΠΎ ΠΌΠΎΠ·Π³Π°: ΡΠ΅Π½ΡΡΠ°Π»ΡΠ½ΡΠΉ ΠΏΠΎΡΠΈΠ½Π½ΡΠΉ ΠΌΠΈΠ΅Π»ΠΈΠ½ΠΎΠ»ΠΈΠ·. ΠΠΎ Π²Π½Π΅Π΄ΡΠ΅Π½ΠΈΡ Π²ΠΈΠ·ΡΠ°Π»ΠΈΠ·ΠΈΡΡΡΡΠΈΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΎΠ½ΠΎ Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΡΠΎΠ²Π°Π»ΠΎΡΡ ΡΠΎΠ»ΡΠΊΠΎ ΠΏΡΠΈ Π°ΡΡΠΎΠΏΡΠΈΠΈ. ΠΡΠΈΠ²Π΅Π΄Π΅Π½ ΠΊΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠΈΠΉ ΡΠ»ΡΡΠ°ΠΉ, ΠΎΠΏΠΈΡΠ°Π½ΠΎ ΠΌΠ½ΠΎΠ³ΠΎΠΎΠ±ΡΠ°Π·ΠΈΠ΅ Π½Π΅Π²ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΈ ΡΠΎΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΈΠΌΠΏΡΠΎΠΌΠ°ΡΠΈΠΊΠΈ. ΠΠΊΡΠ΅Π½ΡΠΈΡΠΎΠ²Π°Π½ΠΎ Π²Π½ΠΈΠΌΠ°Π½ΠΈΠ΅ Π½Π° Π·Π½Π°ΡΠΈΠΌΠΎΡΡΡ ΠΊΠΎΠΌΠΏΠ»Π΅ΠΊΡΠ½ΠΎΠ³ΠΎ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄Π° ΠΊ Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠ΅ ΠΈ Π²Π΅Π΄Π΅Π½ΠΈΡ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠ° Ρ ΡΠ΅Π΄ΠΊΠΈΠΌ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠ΅ΠΌ
Pairs of electronic states supporting the wave process of martensite crystal growth
A model dispersion law for electrons (in the tight-binding approximation with allowance for the first Ξ΅1 and second Ξ΅2 nearest neighbors) is used for body-centered cubic (b.c.c.) crystals to analyze the shapes of the S-surfaces that separate the pairs of electronic states (ES) supporting of the controlling wave process in the non-equilibrium conditions. For b.c.c. and face-centered cubic crystals, the following parameters are calculated: the density of electronic states and portion ΞΆ of ES-pairs localized in the energy interval Ξ β 0.2 eV in the proximity of Fermi level ΞΌ for different values Ξ΅2. The value ΞΌ is choosed close to the energy Ξ΅p of the peak of density of electronic states. The results testify that the wave model of martensite crystal growth supporting non-equilibrium electrons is adequate. Β© 2006 Elsevier B.V. All rights reserved
Pairs of inversely occupied electronic states in the energy range best suited to wave generation
For a model electronic spectrum of a bcc crystal, characteristic s-surfaces are found that separate, in the quasi-momentum space, pairs of electronic states potentially active in the generation of elastic waves at the stage of growth of a martensite crystal. Numerical estimation of the fraction of active electronic states (R eff/R) is performed for the energy range Ξ = 0.2 eV near the Fermi level. The ratio R eff/R is calculated as a function of the parameter ratio for the interaction between the nearest and the second neighbors for both bcc and fcc lattices. Β© 2005 Springer Science+Business Media, Inc
Conditions required for nonequilibrium electrons to generate elastic waves in metals with a cubic lattice
A model dispersion law for electrons (in the tight-binding approximation with allowance for the first and second nearest neighbors) is used for bcc crystals to analyze the shapes of the s surfaces that separate the pairs of electronic states (in the quasi-momentum space) that are potentially active for the generation (amplification) of atomic-displacement waves that control the growth of a martensite crystal under conditions of high chemical-potential gradients. For bcc and fee crystals, the following parameters are calculated: the densities of states and the fractions of the pairs of electronic states (which are potentially active for phonon generation) depending on the Fermi level ΞΌ with respect to the energy Ξ΅p of a peak in the density of states at a fixed energy range |ΞΌ - Ξ΅| β€ β³ for β³ = 0.2 eV. The results obtained are discussed, and it is shown that the effect of lattice distortions in the interphase region on the threshold conditions of phonon generation must be taken into account. Copyright Β© 2005 by Pleiades Publishing, Inc
Ab initio analysis of the effect of strain on the density of non-equilibrium electronic states and their role in the wave model of martensitic transformations
In the wave model of martensitic transformations, the influence of the tensile strain on the creation of non-equilibrium electrons is crucial for the principle of wave amplification by stimulated emission of phonons from an inverted electronic population. By consideration of the strain-effect on the electronic energy spectrum it is shown that - for certain interval of finite strain - the density of active electronic non-equilibrium states in a strained lattice can satisfy the conditions for a phonon-maser effect. Β© 2007 Elsevier B.V. All rights reserved
Effect of uniaxial deformation on the number of pairs of inversely populated electronic states
Simple electronic spectra are considered in the tight-binding approximation for the case of uniform uniaxial deformation. It is shown that there is a range of deformations (considerably exceeding a threshold one) in which conditions for the generation of phonons by nonequilibrium electrons are satisfied. Moreover, in this range an increase in the deformation is accompanied by an increase in the number of pairs of potentially active electronic states. The effect is pronounced more strongly in the case of tensile deformation. The results obtained are important for the development of the theory of reconstructive martensitic transformations. Β© 2008 Pleiades Publishing, Ltd
Critical Diameters of Grains or Individual Particles for the Start of a Martensitic Reaction from the Positions of Dynamic Theory
In the case of spontaneous (under cooling) Ξ³βΞ± martensitic transition in iron alloys, the formation of a martensitic crystal is determined by a wave controlling process and occurs at a supersonic velocity as compared to longitudinal waves. The initiation of three-dimensional threshold deformation is associated with the coordinated action of relatively long (Formula presented.)-wave and relatively short s-waves. The (Formula presented.)-waves appearing during the formation of an initial excited state (IES) are responsible for the description of habit planes. This approach is efficient both in the description of twinned crystals and in the limit case of a degenerate twin structure comparable to the formation of dislocation crystals at initial Ξ³-phase grain sizes exceeding the critical values of Dc. In the case of a nanocrystalline state, the variants of grain transformation as a whole are observed and provisionally classified as an accommodative martensitic transition (AMT). The critical size Dac for AMT is less than Dc. In dynamic theory, Dac can be associated with the spatial IES scaling process compared with the propagation of cylindrical and spherical waves for a relative change in volume. In such a transformation scenario, Dac and the critical size for the transition of small free particles are determined by the threshold deformation value. Β© 2022, Pleiades Publishing, Ltd