78,515 research outputs found

    A High Reliability Asymptotic Approach for Packet Inter-Delivery Time Optimization in Cyber-Physical Systems

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    In cyber-physical systems such as automobiles, measurement data from sensor nodes should be delivered to other consumer nodes such as actuators in a regular fashion. But, in practical systems over unreliable media such as wireless, it is a significant challenge to guarantee small enough inter-delivery times for different clients with heterogeneous channel conditions and inter-delivery requirements. In this paper, we design scheduling policies aiming at satisfying the inter-delivery requirements of such clients. We formulate the problem as a risk-sensitive Markov Decision Process (MDP). Although the resulting problem involves an infinite state space, we first prove that there is an equivalent MDP involving only a finite number of states. Then we prove the existence of a stationary optimal policy and establish an algorithm to compute it in a finite number of steps. However, the bane of this and many similar problems is the resulting complexity, and, in an attempt to make fundamental progress, we further propose a new high reliability asymptotic approach. In essence, this approach considers the scenario when the channel failure probabilities for different clients are of the same order, and asymptotically approach zero. We thus proceed to determine the asymptotically optimal policy: in a two-client scenario, we show that the asymptotically optimal policy is a "modified least time-to-go" policy, which is intuitively appealing and easily implementable; in the general multi-client scenario, we are led to an SN policy, and we develop an algorithm of low computational complexity to obtain it. Simulation results show that the resulting policies perform well even in the pre-asymptotic regime with moderate failure probabilities

    Effect of the symmetry energy on nuclear stopping and its relation to the production of light charged fragments

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    We present a complete systematics (excitation function, impact parameter, system size, isospin asymmetry, and equations of state dependences) of global stopping and fragment production for heavy-ion reactions in the energy range between 50 and 1000 MeV/nucleon in the presence of symmetry energy and an isospin-dependent cross section. It is observed that the degree of stopping depends weakly on the symmetry energy and strongly on the isospin-dependent cross section. However, the symmetry energy and isospin-dependent cross section has an effect of the order of more than 10% on the emission of light charged particles (LCP's). It means that nuclear stopping and LCP's can be used as a tool to get the information of an isospin-dependent cross section. Interestingly, the LCP's emission in the presence of symmetry energy is found to be highly correlated with the global stopping.Comment: 16 pages, 8 figure

    The modern technology of iron and steel production and possible ways of their development

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    Π’ ΠΈΠ·ΠΌΠ΅Π½ΡΡŽΡ‰Π΅ΠΉΡΡ ΠΌΠΈΡ€ΠΎΠ²ΠΎΠΉ обстановкС Π½Π° Ρ€Ρ‹Π½ΠΊΠ΅ сырых ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ² для Ρ‡Π΅Ρ€Π½ΠΎΠΉ ΠΌΠ΅Ρ‚Π°Π»Π»ΡƒΡ€Π³ΠΈΠΈ разрабатываСтся ряд Π½ΠΎΠ²Ρ‹Ρ… Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ ΠΏΠΎ производству Ρ‡ΡƒΠ³ΡƒΠ½Π° ΠΈ стали, Π°Π»ΡŒΡ‚Π΅Ρ€Π½Π°Ρ‚ΠΈΠ²Π½Ρ‹Ρ… ΡΡƒΡ‰Π΅ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΠΌ тСхнологиям, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ способны ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΡ‚ΡŒ экономичСски ΡƒΡΡ‚ΠΎΠΉΡ‡ΠΈΠ²ΡƒΡŽ Ρ€Π°Π±ΠΎΡ‚Ρƒ мСталлургичСских ΠΊΠΎΠΌΠΏΠ°Π½ΠΈΠΉ. Π’ Π΄ΠΎΠΏΠΎΠ»Π½Π΅Π½ΠΈΠΈ ΠΊ этому фокусируСтся Π²Π½ΠΈΠΌΠ°Π½ΠΈΠ΅ Π½Π° экономии энСргии ΠΈ сниТСнии выбросов ΠΏΠ°Ρ€Π½ΠΈΠΊΠΎΠ²Ρ‹Ρ… Π³Π°Π·ΠΎΠ² Π² цСлях Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ Π²Π°ΠΆΠ½Π΅ΠΉΡˆΠΈΡ… вопросов ΠΎΡ…Ρ€Π°Π½Ρ‹ ΠΎΠΊΡ€ΡƒΠΆΠ°ΡŽΡ‰Π΅ΠΉ срСды. ИзмСнСниС состояния ΠΎΠΊΡ€ΡƒΠΆΠ°ΡŽΡ‰Π΅ΠΉ срСды ставит Π½ΠΎΠ²Ρ‹Π΅ ΠΏΡ€ΠΎΠ±Π»Π΅ΠΌΡ‹ ΠΏΠ΅Ρ€Π΅Π΄ мСталлургичСской ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½ΠΎΡΡ‚ΡŒΡŽ, ΠΏΠΎΡ‚Ρ€Π΅Π±Π»ΡΡŽΡ‰Π΅ΠΉ Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Π΅ энСргСтичСскиС ΠΈ Ρ‚ΠΎΠΏΠ»ΠΈΠ²Π½Ρ‹Π΅ рСсурсы. ΠžΡ‚Ρ€Π°ΡΠ»ΡŒ Π²Ρ‹Π½ΡƒΠΆΠ΄Π΅Π½Π° ΡΠΎΡΡ€Π΅Π΄ΠΎΡ‚ΠΎΡ‡ΠΈΡ‚ΡŒ своС Π²Π½ΠΈΠΌΠ°Π½ΠΈΠ΅ Π½Π° сокращСнии всСх Π²ΠΈΠ΄ΠΎΠ² энСргии, Ρ‡Ρ‚ΠΎ ΠΏΡ€ΠΈΠ²Π΅Π΄Π΅Ρ‚ ΠΈ ΠΊ сниТСнию выброса ΠΏΠ°Ρ€Π½ΠΈΠΊΠΎΠ²Ρ‹Ρ… Π³Π°Π·ΠΎΠ². Π Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠ° Π°Π»ΡŒΡ‚Π΅Ρ€Π½Π°Ρ‚ΠΈΠ²Π½Ρ‹Ρ… тСхнологичСских процСссов производства Ρ‡ΡƒΠ³ΡƒΠ½Π° ΠΈ стали способна ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΡ‚ΡŒ мСталлургичСским компаниям экономичСски Π²Ρ‹Π³ΠΎΠ΄Π½ΡƒΡŽ ΠΈ ΡƒΡΡ‚ΠΎΠΉΡ‡ΠΈΠ²ΡƒΡŽ Ρ€Π°Π±ΠΎΡ‚Ρƒ Π² производствС стали. Для ΠΎΡ†Π΅Π½ΠΊΠΈ воздСйствий Π΄Π΅ΡΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΠΈ мСталлургичСских ΠΊΠΎΠΌΠΏΠ°Π½ΠΈΠΉ Π½Π° ΠΎΠΊΡ€ΡƒΠΆΠ°ΡŽΡ‰ΡƒΡŽ срСду Π˜Π½ΠΆΠ΅Π½Π΅Ρ€Π½ΠΎ-консалтинговой ΠΊΠΎΠΌΠΏΠ°Π½ΠΈΠ΅ΠΉ Π₯АВЧ (НАВБH, Π‘anada) Π±Ρ‹Π»ΠΈ Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½Ρ‹ Π½ΠΎΠ²Ρ‹Π΅ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠΈ модСлирования, ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‰ΠΈΠ΅ ΠΊΠ²Π°Π»ΠΈΡ„ΠΈΡ†ΠΈΡ€ΠΎΠ²Π°Π½Π½ΠΎ ΠΈ качСствСнно ΠΎΡ†Π΅Π½ΠΈΠ²Π°Ρ‚ΡŒ риски Π² ΠΏΠΎΡ‚Ρ€Π΅Π±Π»Π΅Π½ΠΈΠΈ энСргии ΠΈ выбросах БО2 Π² мСталлургичСской ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½ΠΎΡΡ‚ΠΈ. ΠœΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠ° для Π°Π½Π°Π»ΠΈΠ·Π° выбросов углСродсодСрТащих ΠΏΠ°Ρ€Π½ΠΈΠΊΠΎΠ²Ρ‹Ρ… Π³Π°Π·ΠΎΠ² Π½Π°Π·Π²Π°Π½Π° G-CAP β„’ (Π—Π΅Π»Π΅Π½Ρ‹ΠΉ Π”ΠΎΠΌ β€” Π‘ΠΎΡ€ΡŒΠ±Π° с загрязнСниСм Π²ΠΎΠ·Π΄ΡƒΡ…Π° углСкислым Π³Π°Π·ΠΎΠΌ), Π° для Π°Π½Π°Π»ΠΈΠ·Π° энСргоэффСктивности β€” En-MAPTM (ΠŸΠ»Π°Π½ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ дСйствий ΠΏΡ€ΠΈ ΡƒΠΏΡ€Π°Π²Π»Π΅Π½ΠΈΠΈ энСргиСй). ΠžΡ†Π΅Π½ΠΊΠ° ΡΡƒΡ‰Π΅ΡΡ‚Π²ΡƒΡŽΡ‰Π΅Π³ΠΎ полоТСния Π² Π±ΠΎΠ»ΡŒΡˆΠΈΠ½ΡΡ‚Π²Π΅ ΠΈΠ½Ρ‚Π΅Π³Ρ€ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… Π·Π°Π²ΠΎΠ΄ΠΎΠ² ΠΏΠΎΠΊΠ°Π·Π°Π»Π°, Ρ‡Ρ‚ΠΎ ΠΎΠ½ΠΈ Ρ€Π°ΡΠΏΠΎΠ»Π°Π³Π°ΡŽΡ‚ возмоТностями ΠΏΠΎ экономии энСргии ΠΈ Π±ΠΎΡ€ΡŒΠ±Ρ‹ с загрязнСниСм атмосфСры ΠΏΠ°Ρ€Π½ΠΈΠΊΠΎΠ²Ρ‹ΠΌΠΈ Π³Π°Π·Π°ΠΌΠΈ, Π»ΡƒΡ‡ΡˆΠΈΠ΅ ΠΈΠ· этих Π·Π°Π²ΠΎΠ΄ΠΎΠ² исчСрпали эти возмоТности Π΄Π°ΠΆΠ΅ ΠΏΡ€ΠΈ высоких Ρ†Π΅Π½Π°Ρ… Π½Π° ΠΊΠ²ΠΎΡ‚Ρ‹ выбросов БО2. Π’ этом контСкстС Π²Π°ΠΆΠ½ΠΎ ΠΎΡ†Π΅Π½ΠΈΡ‚ΡŒ Ρ‚Π΅ Π²Π°ΠΆΠ½Ρ‹Π΅ особСнности Π°Π»ΡŒΡ‚Π΅Ρ€Π½Π°Ρ‚ΠΈΠ²Π½Ρ‹Ρ… Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ получСния Ρ‡ΡƒΠ³ΡƒΠ½Π° ΠΈ стали, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½Ρ‹ ΠΊ настоящСму Π²Ρ€Π΅ΠΌΠ΅Π½ΠΈ. Π­Ρ‚Π° ΡΡ‚Π°Ρ‚ΡŒΡ содСрТит ΡΡ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΡƒΡŽ ΠΎΡ†Π΅Π½ΠΊΡƒ энСргоэффСктивности ΠΈ выбросов ΠŸΠ“ для Π½Π΅ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… Π²Ρ‹Π±Ρ€Π°Π½Π½Ρ‹Ρ… Π°Π»ΡŒΡ‚Π΅Ρ€Π½Π°Ρ‚ΠΈΠ²Π½Ρ‹Ρ… Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ производства Ρ‡ΡƒΠ³ΡƒΠ½Π° ΠΈ стали, ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Π΅ Ρ€Π°ΡΡΠΌΠ°Ρ‚Ρ€ΠΈΠ²Π°ΡŽΡ‚ΡΡ для ΠΈΡ… Ρ€Π΅Π°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ. Для этого ΠΏΡ€ΠΈΠΌΠ΅Π½Π΅Π½Ρ‹ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠΈ G-CAP β„’ ΠΈ G-CAP β„’ , элСмСнты ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… Π±Ρ‹Π»ΠΈ Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½Ρ‹ Π² ΠΊΠΎΠΌΠΏΠ°Π½ΠΈΠΈ HATCH с основной Ρ†Π΅Π»ΡŒΡŽ количСствСнной ΠΈ ΠΊΠ²Π°Π»ΠΈΡ„ΠΈΠΊΠ°Ρ†ΠΈΠΎΠ½Π½ΠΎΠΉ ΠΎΡ†Π΅Π½ΠΊΠΈ ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»Π° экономии энСргии ΠΈ сокращСния выбросов БО2 Π² мСталлургичСской ΠΏΡ€ΠΎΠΌΡ‹ΡˆΠ»Π΅Π½Π½ΠΎΡΡ‚ΠΈIn the changing global market scenario for raw materials for the steel industry, a number of novel iron and steelmaking process technologies are being developed to provide the steel companies with economically-sustainable alternatives for iron and steel-making. In addition, the steel industry is also focusing on reduction of energy consumption as well as green-house gas (GHG) emissions to address the crucial subject of climate change. Climate change is presenting new risks to the highly energy and carbon-intensive, iron and steel industry. The industry needs to focus on reduction of energy consumption as GHG emissions to address climate change. Development of alternate iron and steelmaking process technologies can provide steel companies with economically-sustainable alternatives for steel production. For managing climate change risks, novel modelling tools have been developed by Hatch to quantify and qualify potential energy savings and CO2 abatement within the iron and steel industry. The tool developed for abatement of greenhouse gas carbon is called G-CAPTM (Green-House Gas Carbon Abatement Process) while that developed for improving energy efficiency is called En-MAPTM (Energy Management Action Planning). Evaluation of existing operations have shown that most integrated plants have GHG and energy abatement opportunities; on the other hand, the best-in-class plants may not have a lot of low-risk abatement opportunities left, even at high CO2 price. In this context, it is important to assess these critical issues for the alternate iron and steelmaking technologies that have been developed. This paper presents a comparative evaluation of energy-efficiency and GHG emissions for some selected iron- and steelmaking technologies that are being considered for implementation. In this work, Hatch’s G-CAPβ„’ and En-MAPβ„’ tools that were developed with the main objective of quantifying and qualifying the potential energy savings and CO2 abatement within the iron and steel industry, were employed in the evaluation conducted

    Electromagnetic induction and damping - quantitative experiments using PC interface

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    A bar magnet, attached to an oscillating system, passes through a coil periodically, generating a series of emf pulses. A novel method is described for the quantitative verification of Faraday's law which eliminates all errors associated with angular measurements, thereby revealing delicate features of the underlying mechanics. When electromagnetic damping is activated by short-circuiting the coil, a distinctly linear decay of oscillation amplitude is surprisingly observed. A quantitative analysis reveals an interesting interplay of the electromagnetic and mechanical time scales.Comment: 4 pages, to appear in Am. J. Phy

    Direct and secondary nuclear excitation with x-ray free-electron lasers

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    The direct and secondary nuclear excitation produced by an x-ray free electron laser when interacting with a solid-state nuclear target is investigated theoretically. When driven at the resonance energy, the x-ray free electron laser can produce direct photoexcitation. However, the dominant process in that interaction is the photoelectric effect producing a cold and very dense plasma in which also secondary processes such as nuclear excitation by electron capture may occur. We develop a realistic theoretical model to quantify the temporal dynamics of the plasma and the magnitude of the secondary excitation therein. Numerical results show that depending on the nuclear transition energy and the temperature and charge states reached in the plasma, secondary nuclear excitation by electron capture may dominate the direct photoexcitation by several orders of magnitude, as it is the case for the 4.8 keV transition from the isomeric state of 93^{93}Mo, or it can be negligible, as it is the case for the 14.4 keV M\"ossbauer transition in 57Fe^{57}\mathrm{Fe}. These findings are most relevant for future nuclear quantum optics experiments at x-ray free electron laser facilities.Comment: 17 pages, 7 figures; minor corrections made; accepted by Physics of Plasma
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