2,425 research outputs found

    Wave Functions and Energy Terms of the SCHR\"Odinger Equation with Two-Center Coulomb Plus Harmonic Oscillator Potential

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    Schr\"odinger equation for two center Coulomb plus harmonic oscillator potential is solved by the method of ethalon equation at large intercenter separations. Asymptotical expansions for energy term and wave function are obtained in the analytical form.Comment: 4 pages, no figures, LaTeX, submitted to PR

    Damping Rotor Nutation Oscillations in a Gyroscope with Magnetic Suspension

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    A possibility of an effective damping of rotor nutations by modulating the field of the moment transducers in synchronism with the nutation frequency is considered. The algorithms for forming the control moments are proposed and their application is discussed

    Quantal Two-Centre Coulomb Problem treated by means of the Phase-Integral Method I. General Theory

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    The present paper concerns the derivation of phase-integral quantization conditions for the two-centre Coulomb problem under the assumption that the two Coulomb centres are fixed. With this restriction we treat the general two-centre Coulomb problem according to the phase-integral method, in which one uses an {\it a priori} unspecified {\it base function}. We consider base functions containing three unspecified parameters C,C~C, \tilde C and Ξ›\Lambda. When the absolute value of the magnetic quantum number mm is not too small, it is most appropriate to choose Ξ›=∣mβˆ£β‰ 0\Lambda=|m|\ne 0. When, on the other hand, ∣m∣|m| is sufficiently small, it is most appropriate to choose Ξ›=0\Lambda = 0. Arbitrary-order phase-integral quantization conditions are obtained for these choices of Ξ›\Lambda. The parameters CC and C~\tilde C are determined from the requirement that the results of the first and the third order of the phase-integral approximation coincide, which makes the first-order approximation as good as possible. In order to make the paper to some extent self-contained, a short review of the phase-integral method is given in the Appendix.Comment: 23 pages, RevTeX, 4 EPS figures, submitted to J. Math. Phy

    Spectra of Doubly Heavy Quark Baryons

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    Baryons containing two heavy quarks are treated in the Born-Oppenheimer approximation. Schr\"odinger equation for two center Coulomb plus harmonic oscillator potential is solved by the method of ethalon equation at large intercenter separations. Asymptotical expansions for energy term and wave function are obtained in the analytical form. Using those formulas, the energy spectra of doubly heavy baryons with various quark compositions are calculated analytically.Comment: 19 pages, latex2e, published at PRC61(2000)04520

    Relativistic dynamical polarizability of hydrogen-like atoms

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    Using the operator representation of the Dirac Coulomb Green function the analytical method in perturbation theory is employed in obtaining solutions of the Dirac equation for a hydrogen-like atom in a time-dependent electric field. The relativistic dynamical polarizability of hydrogen-like atoms is calculated and analysed.Comment: 15 pages, 3 figures (not included, but hard copies are available upon request

    ИсслСдованиС процСссов формирования пористых выплавляСмых ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ, примСняСмых для изготовлСния высокоточного Π»ΠΈΡ‚ΡŒΡ

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    Aerospace, manufacturing, and shipbuilding industries strive to enhance their competitiveness by optimizing material utilization and improving production processes. The investment casting process offers the capability to fabricate intricate and precise components using a diverse range of alloys. However, this method is not without its drawbacks, including high manufacturing costs and a significant rate of defective castings, which can reach up to 30 %. These defects primarily arise from the stresses imposed on the wax patterns and ceramic molds, leading to their distortion. To address this issue, efforts have been made to reduce stress by employing compacted wax powders for the production of investment patterns. However, stress relaxation in the wax patterns remains a concern as it can result in elastic deformation of the compacted material and subsequent alterations in the final product dimensions. To mitigate this issue, a series of tests were conducted with the objective of studying stress relaxation under constant compression strain, as described by the Kohlrausch equation. The obtained results provide valuable insights that enable the prediction of the ultimate dimensions of patterns created using different grades of wax.ΠšΠΎΠ½ΠΊΡƒΡ€Π΅Π½Ρ‚ΠΎΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡ‚ΡŒ соврСмСнных прСдприятий машино-, судо- ΠΈ авиастроСния Π²ΠΎ ΠΌΠ½ΠΎΠ³ΠΎΠΌ опрСдСляСтся ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎ- ΠΈ ΡΠ½Π΅Ρ€Π³ΠΎΡΡ„Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½ΠΎΡΡ‚ΡŒΡŽ Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ, Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½Π½Ρ‹Ρ… Π½Π° ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½ΠΈΠ΅ конструкций ΠΈ ΡƒΠ·Π»ΠΎΠ² Π΄Π΅Ρ‚Π°Π»Π΅ΠΉ отвСтствСнного назначСния. ΠŸΡ€ΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Π»ΠΈΡ‚ΡŒΡ ΠΏΠΎ выплавляСмым модСлям (Π›Π’Πœ) обСспСчиваСт ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½ΠΈΠ΅ Π·Π°Π³ΠΎΡ‚ΠΎΠ²ΠΎΠΊ ΠΏΠΎΠ²Ρ‹ΡˆΠ΅Π½Π½ΠΎΠΉ Ρ€Π°Π·ΠΌΠ΅Ρ€Π½ΠΎΠΉ ΠΈ гСомСтричСской точности, слоТной пространствСнной ΠΊΠΎΠ½Ρ„ΠΈΠ³ΡƒΡ€Π°Ρ†ΠΈΠΈ ΠΈΠ· ΡˆΠΈΡ€ΠΎΠΊΠΎΠΉ Π½ΠΎΠΌΠ΅Π½ΠΊΠ»Π°Ρ‚ΡƒΡ€Ρ‹ сплавов. К нСдостаткам Π›Π’Πœ слСдуСт отнСсти ΠΌΠ½ΠΎΠ³ΠΎΡΡ‚Π°Π΄ΠΈΠΉΠ½ΠΎΡΡ‚ΡŒ процСсса ΠΈ Π²Ρ‹ΡΠΎΠΊΡƒΡŽ ΡΡ‚ΠΎΠΈΠΌΠΎΡΡ‚ΡŒ ΠΊΠΎΠ½Π΅Ρ‡Π½ΠΎΠ³ΠΎ ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚Π°, Ρ‡Ρ‚ΠΎ ΠΏΡ€Π΅Π΄ΠΏΠΎΠ»Π°Π³Π°Π΅Ρ‚ Π½Π΅Π΄ΠΎΠΏΡƒΡΡ‚ΠΈΠΌΠΎΡΡ‚ΡŒ Π±Ρ€Π°ΠΊΠ°, доля ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠ³ΠΎ ΠΌΠΎΠΆΠ΅Ρ‚ Π΄ΠΎΡΡ‚ΠΈΠ³Π°Ρ‚ΡŒ 30 %. Π‘Ρ€Π°ΠΊ Π² Π›Π’Πœ прСимущСствСнно Π²Ρ‹Π·Π²Π°Π½ тСплофизичСскими явлСниями, ΡΠΎΠΏΡ€ΠΎΠ²ΠΎΠΆΠ΄Π°ΡŽΡ‰ΠΈΠΌΠΈ ряд тСхнологичСских ΠΎΠΏΠ΅Ρ€Π°Ρ†ΠΈΠΉ ΠΈ ΠΎΠ±ΡƒΡΠ»ΠΎΠ²Π»ΠΈΠ²Π°ΡŽΡ‰ΠΈΠΌΠΈ Π½Π°Π»ΠΈΡ‡ΠΈΠ΅ напряТСний Π² структурС воскообразных ΠΈ кСрамичСских ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ², Ρ‡Ρ‚ΠΎ опрСдСляСт Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΎΠ½Π½Ρ‹Π΅ процСссы Π² выплавляСмых модСлях ΠΈ ΠΎΠ±ΠΎΠ»ΠΎΡ‡ΠΊΠΎΠ²Ρ‹Ρ… Ρ„ΠΎΡ€ΠΌΠ°Ρ…. Для устранСния Π½Π΅Π³Π°Ρ‚ΠΈΠ²Π½ΠΎΠ³ΠΎ влияния тСплофизичСского Ρ„Π°ΠΊΡ‚ΠΎΡ€Π° ΠΈ сниТСния напряТСний Π² структурах ΠΏΡ€ΠΎΠΌΠ΅ΠΆΡƒΡ‚ΠΎΡ‡Π½Ρ‹Ρ… ΠΈΠ·Π΄Π΅Π»ΠΈΠΉ процСсса, выплавляСмыС ΠΌΠΎΠ΄Π΅Π»ΠΈ Ρ„ΠΎΡ€ΠΌΠΈΡ€ΡƒΡŽΡ‚ прСссованиСм ΠΏΠΎΡ€ΠΎΡˆΠΊΠΎΠ² воскообразных ΠΌΠΎΠ΄Π΅Π»ΡŒΠ½Ρ‹Ρ… ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡ†ΠΈΠΉ. ΠŸΡ€ΠΈ этом Π½Π΅Ρ€Π΅ΡˆΠ΅Π½Π½Ρ‹ΠΌ остаСтся вопрос рСлаксации напряТСний Π² прСссовках, приводящих ΠΊ ΡƒΠΏΡ€ΡƒΠ³ΠΎΠΌΡƒ ΠΎΡ‚ΠΊΠ»ΠΈΠΊΡƒ ΡƒΠΏΠ»ΠΎΡ‚Π½Π΅Π½Π½ΠΎΠ³ΠΎ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»Π° ΠΈ, ΠΊΠ°ΠΊ слСдствиС, измСнСнию Ρ€Π°Π·ΠΌΠ΅Ρ€ΠΎΠ² ΠΏΠΎΠ»ΡƒΡ‡Π°Π΅ΠΌΠΎΠ³ΠΎ издСлия. Поиск Π²Π°Ρ€ΠΈΠ°Π½Ρ‚ΠΎΠ² Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ Ρ€Π°Ρ†ΠΈΠΎΠ½Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ Ρ€Π΅ΠΆΠΈΠΌΠ° формирования прСссовки ΠΏΡ€ΠΈΠ²Π΅Π» ΠΊ нСобходимости провСдСния сСрии экспСримСнтов, Π² Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Π΅ ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… прСдполагаСтся достиТСниС рСлаксации напряТСний Οƒ Π² условиях постоянной Π΄Π΅Ρ„ΠΎΡ€ΠΌΠ°Ρ†ΠΈΠΈ сТатия, описываСмого ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠ΅ΠΌ ΠšΠΎΠ»ΡŒΡ€Π°ΡƒΡˆΠ°. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Π΅ Π² Ρ…ΠΎΠ΄Π΅ экспСримСнта Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹ позволят ΠΏΡ€ΠΎΠ³Π½ΠΎΠ·ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ ΠΊΠΎΠ½Π΅Ρ‡Π½Ρ‹Π΅ Ρ€Π°Π·ΠΌΠ΅Ρ€Ρ‹ прСссовок ΠΈ ΡΡ„ΠΎΡ€ΠΌΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ ΠΌΠ°Ρ‚Π΅ΠΌΠ°Ρ‚ΠΈΡ‡Π΅ΡΠΊΡƒΡŽ модСль процСсса, Π°ΠΊΡ‚ΡƒΠ°Π»ΡŒΠ½ΡƒΡŽ для ΡˆΠΈΡ€ΠΎΠΊΠΎΠΉ Π½ΠΎΠΌΠ΅Π½ΠΊΠ»Π°Ρ‚ΡƒΡ€Ρ‹ воскообразных ΠΌΠΎΠ΄Π΅Π»ΡŒΠ½Ρ‹Ρ… ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π»ΠΎΠ², примСняСмых Π² Π›Π’Πœ

    Glass capillary X-ray lens: fabrication technique and ray tracing calculations

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    A new method for producing a compound refractive X-ray lens is described. The lens is designed as glass capillary "lled by a set of concave individual lenses. The method is appropriate for the preparation of 10}1000 spherical lenses in a glass capillary with a diameter of 0.1}1 mm. Lens aberrations are considered and simple formulas for spot size are derived. Ray-tracing simulations on the focusing experiments using 18 keV X-rays are reported. ( 2000 Elsevier Science B.V. All rights reserved
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