114 research outputs found

    Estimates in Beurling--Helson type theorems. Multidimensional case

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    We consider the spaces Ap(Tm)A_p(\mathbb T^m) of functions ff on the mm -dimensional torus Tm\mathbb T^m such that the sequence of the Fourier coefficients f^={f^(k),Β k∈Zm}\hat{f}=\{\hat{f}(k), ~k \in \mathbb Z^m\} belongs to lp(Zm),Β 1≀p<2l^p(\mathbb Z^m), ~1\leq p<2. The norm on Ap(Tm)A_p(\mathbb T^m) is defined by βˆ₯fβˆ₯Ap(Tm)=βˆ₯f^βˆ₯lp(Zm)\|f\|_{A_p(\mathbb T^m)}=\|\hat{f}\|_{l^p(\mathbb Z^m)}. We study the rate of growth of the norms βˆ₯eiλφβˆ₯Ap(Tm)\|e^{i\lambda\varphi}\|_{A_p(\mathbb T^m)} as βˆ£Ξ»βˆ£β†’βˆž, λ∈R,|\lambda|\rightarrow \infty, ~\lambda\in\mathbb R, for C1C^1 -smooth real functions Ο†\varphi on Tm\mathbb T^m (the one-dimensional case was investigated by the author earlier). The lower estimates that we obtain have direct analogues for the spaces Ap(Rm)A_p(\mathbb R^m)

    Propagation of Light in the Field of Stationary and Radiative Gravitational Multipoles

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    Extremely high precision of near-future radio/optical interferometric observatories like SKA, Gaia, SIM and the unparalleled sensitivity of LIGO/LISA gravitational-wave detectors demands more deep theoretical treatment of relativistic effects in the propagation of electromagnetic signals through variable gravitational fields of the solar system, oscillating and precessing neutron stars, coalescing binary systems, exploding supernova, and colliding galaxies. Especially important for future gravitational-wave observatories is the problem of propagation of light rays in the field of multipolar gravitational waves emitted by a localized source of gravitational radiation. Present paper suggests physically-adequate and consistent mathematical solution of this problem in the first post-Minkowskian approximation of General Relativity which accounts for all time-dependent multipole moments of an isolated astronomical system.Comment: 36 pages, no figure

    Mathematical model of the starter system for a three-stage synchronous generator with a damping cage

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    Π’ Π΄Π°Π½Π½ΠΎΠΉ ΡΡ‚Π°Ρ‚ΡŒΠ΅ рассматриваСтся матСматичСская модСль стартСрной систСмы для Π³Π°Π·ΠΎΡ‚ΡƒΡ€Π±ΠΈΠ½Π½Ρ‹Ρ… Π΄Π²ΠΈΠ³Π°Ρ‚Π΅Π»Π΅ΠΉ. МодСль исслСдуСмого трСхкаскадного синхронного Π³Π΅Π½Π΅Ρ€Π°Ρ‚ΠΎΡ€Π° Π±Ρ‹Π»Π° построСна Π² систСмС d-q-ΠΊΠΎΠΎΡ€Π΄ΠΈΠ½Π°Ρ‚. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Π½Π°Ρ модСль позволяСт ΡΠΊΠΎΠ½Ρ„ΠΈΠ³ΡƒΡ€ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹ ΠΌΠ°ΡˆΠΈΠ½Ρ‹ Π² ΡˆΠΈΡ€ΠΎΠΊΠΎΠΌ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π΅, Π° Ρ‚Π°ΠΊΠΆΠ΅ ΠΏΠΎΠ»ΡƒΡ‡ΠΈΡ‚ΡŒ ΠΈΠ½Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΡŽ ΠΎ Ρ‚ΠΎΠΊΠ°Ρ… ΠΈ напряТСниях основных элСктричСских ΡƒΠ·Π»ΠΎΠ² ΠΌΠ°ΡˆΠΈΠ½Ρ‹. ΠœΠ°Ρ‚Π΅ΠΌΠ°Ρ‚ΠΈΡ‡Π΅ΡΠΊΠΎΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΎ ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½ΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈ Π°Π΄Π΅ΠΊΠ²Π°Ρ‚Π½ΠΎΡΡ‚ΡŒ ΠΏΡ€Π΅Π΄Π»ΠΎΠΆΠ΅Π½Π½ΠΎΠ³ΠΎ Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠ° элСктростартСрного запуска синхронной ΠΌΠ°ΡˆΠΈΠ½Ρ‹.This paper, considers a mathematical model the starter system for gas turbine engines. Model of the investigated three-stage synchronous generator has been built in the dq-coordinates. The obtained model allows one to configure the machine parameters in a wide range, as well as receive information about currents and voltages major electrical components of the machine. Mathematical modeling shown efficiency of the resulting model and adequacy of the proposed algorithms electric starter mode synchronous machine

    Silicon-carbide semiconductors as base for active rectifier

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    Π’ Π΄ΠΎΠΊΠ»Π°Π΄Π΅ прСдставлСна концСпция построСния прСобразоватСля частоты ΠΏΠΎ Ρ‚ΠΈΠΏΡƒ Π°ΠΊΡ‚ΠΈΠ²Π½ΠΎΠ³ΠΎ выпрямитСля Π½Π° свСрхмалыС массо-Π³Π°Π±Π°Ρ€ΠΈΡ‚Π½Ρ‹Π΅ ΠΏΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»ΠΈ (Π΄ΠΎ 0,4 ΠΊΠ³/ΠΊΠ’Ρ‚) с использованиСм ΠΊΠ°Ρ€Π±ΠΈΠ΄-ΠΊΡ€Π΅ΠΌΠ½ΠΈΠ΅Π²Ρ‹Ρ… транзисторов. Π’ основС ΠΊΠΎΠ½Ρ†Π΅ΠΏΡ†ΠΈΠΈ Π·Π°Π»ΠΎΠΆΠ΅Π½Ρ‹ ΠΏΡ€ΠΈΠ½Ρ†ΠΈΠΏΡ‹ наращивания мощности ΠΏΡ€Π΅ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Ρ‚Π΅Π»Π΅ΠΉ Π·Π° счСт ΠΏΠ°Ρ€Π°Π»Π»Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ соСдинСния ΠΏΡ€Π΅ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Ρ‚Π΅Π»Π΅ΠΉ мСньшСй мощности (ΠΌΠΎΠ΄ΡƒΠ»Π΅ΠΉ). Алгоритм управлСния всСм ΠΏΡ€Π΅ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Ρ‚Π΅Π»Π΅ΠΌ Ρ€Π΅Π°Π»ΠΈΠ·ΠΎΠ²Π°Π½ Π½Π° Π±Π°Π·Π΅ ΠΌΠΈΠΊΡ€ΠΎΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»Π»Π΅Ρ€Π° ΠΈ ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌΠΈΡ€ΡƒΠ΅ΠΌΠΎΠΉ логичСской ΠΈΠ½Ρ‚Π΅Π³Ρ€Π°Π»ΡŒΠ½ΠΎΠΉ схСмы (ΠŸΠ›Π˜Π‘). Π‘ΠΎΠ²ΠΎΠΊΡƒΠΏΠ½ΠΎΡΡ‚ΡŒ достоинств микросхСм, Π° Ρ‚Π°ΠΊΠΆΠ΅ ряд тСхничСских Ρ€Π΅ΡˆΠ΅Π½ΠΈΠΉ обСспСчили нСзависимоС Ρ†Π΅Π½Ρ‚Ρ€Π°Π»ΠΈΠ·ΠΎΠ²Π°Π½Π½ΠΎΠ΅ ΡƒΠΏΡ€Π°Π²Π»Π΅Π½ΠΈΠ΅ 36 транзисторами Π½Π° постоянной частотС ΠΊΠΎΠΌΠΌΡƒΡ‚Π°Ρ†ΠΈΠΈ 75 ΠΊΠ“Ρ†. ЭквивалСнтная ΠΏΡƒΠ»ΡŒΡΠ½ΠΎΡΡ‚ΡŒ Ρ‚ΠΎΠΊΠ° для рассматриваСмого Ρ‚Ρ€Π΅Ρ…Ρ„Π°Π·Π½ΠΎΠ³ΠΎ прСобразоватСля составляСт 450 ΠΊΠ“Ρ†. Π’ Ρ€Π°Π±ΠΎΡ‚Π΅ прСдставлСны ΠΏΡ€ΠΎΠΌΠ΅ΠΆΡƒΡ‚ΠΎΡ‡Π½Ρ‹Π΅ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ испытаний ΠΎΠ±Ρ€Π°Π·Ρ†Π° Π½Π° Π½ΠΎΠΌΠΈΠ½Π°Π»ΡŒΠ½ΡƒΡŽ ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒ 25 ΠΊΠ’Ρ‚.The report introduces the concept of building the inverter-type active rectifier on ultra-small weight and size parameters (up to 0.4 kg / kW). The concept based on the principles of increasing converters power due to the parallel connection of lower power converters (modules). The control algorithm is implemented on microcontroller and programmable logic integrated circuits (FPGAs) co-working. Set of advantages applied digital circuits, as well as a number of technical solutions that organize synchronous and discontinuous operation of two chips in a single computational cycle, ensure the independence of the centralized management of 36 transistors on a constant switching frequency of 75 kHz. Equivalent frequencyof ripples in current for the considered three-phase inverter is 450 kHz. The paper presents the interim results of the test sample to the nominal power of 25 kW

    Π£Π»ΡŒΡ‚Ρ€Π°Ρ„ΠΈΠΎΠ»Π΅Ρ‚ΠΎΠ²ΠΎΠ΅ ΠΈΠ·Π»ΡƒΡ‡Π΅Π½ΠΈΠ΅ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ½ΠΎβ€“ΠΏΠ΅Ρ€ΠΈΠΎΠ΄ΠΈΡ‡Π΅ΡΠΊΠΈΡ… разрядов высокого давлСния Π² ксСнонС

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    Pulsed quartz-jacketed high-pressure xenon lamps, operating in the periodic pulse repetition modes, despite the appearing UV radiation sources of other types, remain a critical component of the processing equipment used in photochemistry, photo-medicine, nanoelectronics, biology, etc. Their main advantages, namely high power and radiation energy are slightly devalued by a relatively low efficiency of the shortwave radiation. Available literature data concerning the influence of various factors on the energy level of short-wave radiation in xenon need to be systematised and generalised because they have been obtained under conditions of uncontrolled quartz-jacketed transmission. The transmission of quartz can degrade after a while and, in addition, undergo great changes during the pulse. Besides, as a rule, in the literature, there is no detailed description of a complete kit of experimental setting. As a result, to analyse the factors affecting the efficiency of studying in the UV range is difficult, and there arises a relevant problem to optimise this type of discharge parameters to increase the efficiency in the range of 220-400 nm. A mathematical model of the radiation source, realistically describing the processes in the xenon plasma and in the stabilising envelope, can be a reliable ground for such a study. The paper shows an impact of the discharge channel diameter and length, the filling pressure of xenon, the pulse duration, the parameters of discharge circuit, and the current of pilot arc on the radiation yield. Based on the simulation-found relationship of internal plasma parameters (temperature distributions, fields of particle concentration and radiation, dynamics of electrical resistance of discharge channel, and plasma emission spectra) with radiation characteristics of discharge, are determined conditions to ensure the greatest radiation yield in the UV region. Β The experimental data prove the computational results. A material obtained gives practice-critical guidelines for development and correct selection of the short-wave radiation source.Π˜ΠΌΠΏΡƒΠ»ΡŒΡΠ½Ρ‹Π΅ ксСноновыС Π»Π°ΠΌΠΏΡ‹ высокого давлСния Π² ΠΊΠ²Π°Ρ€Ρ†Π΅Π²ΠΎΠΉ ΠΎΠ±ΠΎΠ»ΠΎΡ‡ΠΊΠ΅, Ρ€Π°Π±ΠΎΡ‚Π°ΡŽΡ‰ΠΈΠ΅ Π² Ρ€Π΅ΠΆΠΈΠΌΠ°Ρ… пСриодичСского слСдования ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠΎΠ², нСсмотря Π½Π° появлСниС источников Π£Π€- излучСния Π΄Ρ€ΡƒΠ³ΠΈΡ… Ρ‚ΠΈΠΏΠΎΠ² ΠΎΡΡ‚Π°ΡŽΡ‚ΡΡ ваТнСйшим ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚ΠΎΠΌ тСхнологичСского оборудования, примСняСмого Π² Ρ„ΠΎΡ‚ΠΎΡ…ΠΈΠΌΠΈΠΈ, Ρ„ΠΎΡ‚ΠΎΠΌΠ΅Π΄ΠΈΡ†ΠΈΠ½Π΅, наноэлСктроникС, Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΈ Ρ‚.Π΄. Π“Π»Π°Π²Π½Ρ‹Π΅ ΠΈΡ… достоинства -Β  высокая ΠΌΠΎΡ‰Π½ΠΎΡΡ‚ΡŒ ΠΈ энСргия излучСния - нСсколько обСсцСниваСт ΠΎΡ‚Π½ΠΎΡΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ низкая ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ излучСния Π² ΠΊΠΎΡ€ΠΎΡ‚ΠΊΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ области. Π˜ΠΌΠ΅ΡŽΡ‰ΠΈΠ΅ΡΡ Π»ΠΈΡ‚Π΅Ρ€Π°Ρ‚ΡƒΡ€Π½Ρ‹Π΅ Π΄Π°Π½Π½Ρ‹Π΅ ΠΎ влиянии Ρ€Π°Π·Π»ΠΈΡ‡Π½Ρ‹Ρ… Ρ„Π°ΠΊΡ‚ΠΎΡ€ΠΎΠ² Π½Π° ΡƒΡ€ΠΎΠ²Π΅Π½ΡŒ энСргии ΠΊΠΎΡ€ΠΎΡ‚ΠΊΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ³ΠΎ излучСния разрядов Π² ксСнонС Π½ΡƒΠΆΠ΄Π°ΡŽΡ‚ΡΡ Π² систСматизации ΠΈ ΠΎΠ±ΠΎΠ±Ρ‰Π΅Π½ΠΈΠΈ, Ρ‚.ΠΊ. ΠΎΠ½ΠΈ ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Ρ‹ Π² условиях Π½Π΅ΠΊΠΎΠ½Ρ‚Ρ€ΠΎΠ»ΠΈΡ€ΡƒΠ΅ΠΌΠΎΠ³ΠΎ значСния пропускания ΠΊΠ²Π°Ρ€Ρ†Π΅Π²ΠΎΠΉ ΠΎΠ±ΠΎΠ»ΠΎΡ‡ΠΊΠΈ. ΠŸΡ€ΠΎΠΏΡƒΡΠΊΠ°Π½ΠΈΠ΅ ΠΊΠ²Π°Ρ€Ρ†Π° ΠΌΠΎΠΆΠ΅Ρ‚ Π΄Π΅Π³Ρ€Π°Π΄ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ со Π²Ρ€Π΅ΠΌΠ΅Π½Π΅ΠΌ ΠΈ, ΠΊΡ€ΠΎΠΌΠ΅ Ρ‚ΠΎΠ³ΠΎ,Β  сильно ΠΌΠ΅Π½ΡΡ‚ΡŒΡΡ Π² Ρ‚Π΅Ρ‡Π΅Π½ΠΈΠ΅ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ°. ΠšΡ€ΠΎΠΌΠ΅ Ρ‚ΠΎΠ³ΠΎ,Β  Π² Π»ΠΈΡ‚Π΅Ρ€Π°Ρ‚ΡƒΡ€Π΅ отсутствуСт, ΠΊΠ°ΠΊ ΠΏΡ€Π°Π²ΠΈΠ»ΠΎ, Π΄Π΅Ρ‚Π°Π»ΡŒΠ½ΠΎΠ΅ описаниС ΠΏΠΎΠ»Π½ΠΎΠ³ΠΎ Π½Π°Π±ΠΎΡ€Π° условий провСдСния экспСримСнта. Π’ ΠΈΡ‚ΠΎΠ³Π΅ Π°Π½Π°Π»ΠΈΠ· Ρ„Π°ΠΊΡ‚ΠΎΡ€ΠΎΠ², Π²Π»ΠΈΡΡŽΡ‰ΠΈΡ… Π½Π°Β  ΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒ изучСния Π² Π£Π€- области Π·Π°Ρ‚Ρ€ΡƒΠ΄Π½Π΅Π½, ΠΈ Π²ΠΎΠ·Π½ΠΈΠΊΠ°Π΅Ρ‚ Π°ΠΊΡ‚ΡƒΠ°Π»ΡŒΠ½Π°Ρ Π·Π°Π΄Π°Ρ‡Π° ΠΎΠΏΡ‚ΠΈΠΌΠΈΠ·Π°Ρ†ΠΈΠΈ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² разрядов ΡƒΠΊΠ°Π·Π°Π½Π½ΠΎΠ³ΠΎ Ρ‚ΠΈΠΏΠ° с Ρ†Π΅Π»ΡŒΡŽ увСличСния ΠšΠŸΠ” Π² области 220-400 Π½ΠΌ. НадСТной основой для провСдСния Ρ‚Π°ΠΊΠΎΠΉ Ρ€Π°Π±ΠΎΡ‚Ρ‹ ΠΌΠΎΠΆΠ΅Ρ‚ ΡΠ»ΡƒΠΆΠΈΡ‚ΡŒ расчСтно- тСорСтичСскоС исслСдованиС с ΠΏΠΎΠΌΠΎΡ‰ΡŒΡŽΒ  матСматичСской ΠΌΠΎΠ΄Π΅Π»ΠΈ источника излучСния, рСалистично ΠΎΠΏΠΈΡΡ‹Π²Π°ΡŽΡ‰Π΅ΠΉ процСссы Π² ΠΏΠ»Π°Π·ΠΌΠ΅ ксСнона ΠΈ ΡΡ‚Π°Π±ΠΈΠ»ΠΈΠ·ΠΈΡ€ΡƒΡŽΡ‰Π΅ΠΉ ΠΎΠ±ΠΎΠ»ΠΎΡ‡ΠΊΠ΅. Π’ Ρ€Π°Π±ΠΎΡ‚Π΅Β  ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ влияниС Π½Π°Β  Π²Ρ‹Ρ…ΠΎΠ΄ излучСния Π΄ΠΈΠ°ΠΌΠ΅Ρ‚Ρ€Π° ΠΈ Π΄Π»ΠΈΠ½Ρ‹ разрядного ΠΊΠ°Π½Π°Π»Π°, давлСния наполнСния ксСнона, Π΄Π»ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΡΡ‚ΠΈ ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ°, ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² разрядного ΠΊΠΎΠ½Ρ‚ΡƒΡ€Π°, Ρ‚ΠΎΠΊΠ° Π΄Π΅ΠΆΡƒΡ€Π½ΠΎΠΉ Π΄ΡƒΠ³ΠΈ. На основС устанавливаСмой ΠΏΡ€ΠΈ ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠΈ связи Π²Π½ΡƒΡ‚Ρ€Π΅Π½Π½ΠΈΡ… ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² ΠΏΠ»Π°Π·ΠΌΡ‹ (Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Π½Ρ‹Ρ… распрСдСлСний, ΠΏΠΎΠ»Π΅ΠΉ ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΠΈ частиц ΠΈ Ρ€Π°Π΄ΠΈΠ°Ρ†ΠΈΠΈ, Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΈ элСктричСского сопротивлСния ΠΊΠ°Π½Π°Π»Π° разряда ΠΈ спСктров излучСния ΠΏΠ»Π°Π·ΠΌΡ‹) с Ρ€Π°Π΄ΠΈΠ°Ρ†ΠΈΠΎΠ½Π½Ρ‹ΠΌΠΈ характСристиками разряда ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Ρ‹ условия, ΠΎΠ±Π΅ΡΠΏΠ΅Ρ‡ΠΈΠ²Π°ΡŽΡ‰ΠΈΠ΅ наибольший Π²Ρ‹Ρ…ΠΎΠ΄ излучСния Π² Π£Π€- области. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ вычислСний  ΠΏΠΎΠ΄Ρ‚Π²Π΅Ρ€ΠΆΠ΄Π΅Π½Ρ‹ ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹ΠΌΠΈ Π΄Π°Π½Π½Ρ‹ΠΌΠΈ. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹ΠΉΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π» Π΄Π°Π΅Ρ‚ Π²Π°ΠΆΠ½Ρ‹Π΅ для ΠΏΡ€Π°ΠΊΡ‚ΠΈΠΊΠΈ ΠΎΡ€ΠΈΠ΅Π½Ρ‚ΠΈΡ€Ρ‹ для Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ ΠΈ ΠΏΡ€Π°Π²ΠΈΠ»ΡŒΠ½ΠΎΠ³ΠΎ Π²Ρ‹Π±ΠΎΡ€Π° источника излучСния ΠΊΠΎΡ€ΠΎΡ‚ΠΊΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ³ΠΎ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π°

    Inferring possible magnetic field strength of accreting inflows in EXor-type objects from scaled laboratory experiments

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    Aims. EXor-type objects are protostars that display powerful UV-optical outbursts caused by intermittent and powerful events of magnetospheric accretion. These objects are not yet well investigated and are quite difficult to characterize. Several parameters, such as plasma stream velocities, characteristic densities, and temperatures, can be retrieved from present observations. As of yet, however, there is no information about the magnetic field values and the exact underlying accretion scenario is also under discussion. Methods. We use laboratory plasmas, created by a high power laser impacting a solid target or by a plasma gun injector, and make these plasmas propagate perpendicularly to a strong external magnetic field. The propagating plasmas are found to be well scaled to the presently inferred parameters of EXor-type accretion event, thus allowing us to study the behaviour of such episodic accretion processes in scaled conditions. Results. We propose a scenario of additional matter accretion in the equatorial plane, which claims to explain the increased accretion rates of the EXor objects, supported by the experimental demonstration of effective plasma propagation across the magnetic field. In particular, our laboratory investigation allows us to determine that the field strength in the accretion stream of EXor objects, in a position intermediate between the truncation radius and the stellar surface, should be of the order of 100 G. This, in turn, suggests a field strength of a few kilogausses on the stellar surface, which is similar to values inferred from observations of classical T Tauri stars

    Orbital effects of a monochromatic plane gravitational wave with ultra-low frequency incident on a gravitationally bound two-body system

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    We analytically compute the long-term orbital variations of a test particle orbiting a central body acted upon by an incident monochromatic plane gravitational wave. We assume that the characteristic size of the perturbed two-body system is much smaller than the wavelength of the wave. Moreover, we also suppose that the wave's frequency is much smaller than the particle's orbital one. We make neither a priori assumptions about the direction of the wavevector nor on the orbital geometry of the planet. We find that, while the semi-major axis is left unaffected, the eccentricity, the inclination, the longitude of the ascending node, the longitude of pericenter and the mean anomaly undergo non-vanishing long-term changes. They are not secular trends because of the slow modulation introduced by the tidal matrix coefficients and by the orbital elements themselves. They could be useful to indepenedently constrain the ultra-low frequency waves which may have been indirectly detected in the BICEP2 experiment. Our calculation holds, in general, for any gravitationally bound two-body system whose characteristic frequency is much larger than the frequency of the external wave. It is also valid for a generic perturbation of tidal type with constant coefficients over timescales of the order of the orbital period of the perturbed particle.Comment: LaTex2e, 24 pages, no figures, no tables. Changes suggested by the referees include

    Molecular and electronic structure of terminal and alkali metal-capped uranium(V) nitride complexes

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    Determining the electronic structure of actinide complexes is intrinsically challenging because inter-electronic repulsion, crystal field, and spin–orbit coupling effects can be of similar magnitude. Moreover, such efforts have been hampered by the lack of structurally analogous families of complexes to study. Here we report an improved method to U≑N triple bonds, and assemble a family of uranium(V) nitrides. Along with an isoelectronic oxo, we quantify the electronic structure of this 5f1 family by magnetometry, optical and electron paramagnetic resonance (EPR) spectroscopies and modelling. Thus, we define the relative importance of the spin–orbit and crystal field interactions, and explain the experimentally observed different ground states. We find optical absorption linewidths give a potential tool to identify spin–orbit coupled states, and show measurement of UVΒ·Β·Β·UV super-exchange coupling in dimers by EPR. We show that observed slow magnetic relaxation occurs via two-phonon processes, with no obvious correlation to the crystal field

    An ancient bison from the mouth of the Rauchua River (Chukotka, Russia)

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    An incomplete carcass of an extinct bison, Bison ex gr. priscus, was discovered in 2012 in the mouth of the Rauchua River (69Β°30'N, 166Β°49'E), Chukotka. The carcass included the rump with two hind limbs, ribs, and large flap of hide from the abdomen and sides, several vertebrae, bones of the forelimbs and anterior autopodia, stomach with its contents, and wool. The limb bones are relatively gracile, which is unusual in bison, and a SEM study of the hair microstructure suggests higher insulating capacity than in extant members of the genus. Additionally, mitochondrial DNA analyses indicate that the Rauchua bison belonged to a distinct and previously unidentified lineage of steppe bison. Two radiocarbon dates suggest a Holocene age for the bison: a traditional 14C date provided an estimate of 8030Β±70 14C yr BP (SPb-743) and an AMS radiocarbon date provided an age of 9497Β±92 14C yr BP (AA101271). These dates make this the youngest known bison from Chukotka. Analysis of stomach contents revealed a diet of herbaceous plants (meadow grasses and sedges) and shrubs, suggesting that the early Holocene vegetation near the mouth of the Rauchua River was similar to that of the present day: tundra-associated vegetation with undersized plants
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