311 research outputs found

    Study on Excitation Forces Generated by Defective Races of Rolling Bearing

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    AbstractThe vibrations generated by defective rolling elements bearing play vital role in dynamics of rotating machines. In this paper different approach for simulation and numerical analysis of defective bearing races presented by researchers have been compared and extended for multiple defects. This work has been attempted to demonstrate the way of modelling and simulation of local and distributed defect on inner and outer race of deep groove ball bearing. The bearing defect has been modelled as impulse train force or impact force to cause an additional deflection or excitation of rolling elements. The simulated results have been analysed in time and frequency domain. The characteristics defect frequency and its harmonics and amplitude of vibration response of defective bearing is broadly investigated through simulated results

    Evaluation of new insecticide molecules for their effectiveness in the management of sugarcane early shoot borer, Chilo infuscatellus (Snellen)

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    An experiment was conducted at Zonal Agricultural Research Station, V.C farm, Mandya (Karnataka), India during 2015, to assess the chemical control of sugarcane early shoot borer (Chilo infuscatellus). Nine insecticides namely, Fipronil 0.3G, Chlorantraniliprole 0.4G, Chlorantraniliprole 18.5 SC, Spinosad 45SC, Flubendiamide 39.35SC, Cartap hydrochloride 4G, Phorate 10G, Carbofuran 3G, Chlorpyriphos 20EC, and compared with untreated (Check plot)using randomized block design with three replications. Significant differences were noticed among the treatments. Chlorantraniliprole 0.4G recorded lowest cumulative incidence (2.79 %) and highest per cent reduction over the control (85.78 %) which was followed by Cartap hydrochloride 4G (5.37% and 72.65%), Chlorantraniliprole 18.5 SC (5.95% and 75.62%), Flubendiamide 39.35SC (6.64% and 66.19%) and Fipronil 0.3G (6.83% and 65.22%) were found significantly superior in reducing the cumulative incidence of C. infuscatellus.In Co 86032 Cartap hydrochloride 4G was found to be the best insecticide in getting a highest cost benefit ratio (1:12.39). Other insecticides such as Fipronil 0.3G (1:8.84), Chlorantraniliprole 0.4G (1:6.96), Flubendiamide 39.35SC (1:5.42) and Spinosad 45SC (1:4.16) have also recorded better cost benefit ratio. Since Cartap hydrochloride 4G does not have crop label so we can recommend Fipronil 0.3G or Chlorantraniliprole 0.4G for the management of sugarcane early shoot borer

    Statistics of Coulomb Blockade Peak Spacings within the Hartree-Fock Approximation

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    We study the effect of electronic interactions on the addition spectra and on the energy level distributions of two-dimensional quantum dots with weak disorder using the self-consistent Hartree-Fock approximation for spinless electrons. We show that the distribution of the conductance peak spacings is Gaussian with large fluctuations that exceed, in agreement with experiments, the mean level spacing of the non-interacting system. We analyze this distribution on the basis of Koopmans' theorem. We show furthermore that the occupied and unoccupied Hartree-Fock levels exhibit Wigner-Dyson statistics.Comment: 5 pages, 2 figures, submitted for publicatio

    Semiclassical Theory of Coulomb Blockade Peak Heights in Chaotic Quantum Dots

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    We develop a semiclassical theory of Coulomb blockade peak heights in chaotic quantum dots. Using Berry's conjecture, we calculate the peak height distributions and the correlation functions. We demonstrate that the corrections to the corresponding results of the standard statistical theory are non-universal and can be expressed in terms of the classical periodic orbits of the dot that are well coupled to the leads. The main effect is an oscillatory dependence of the peak heights on any parameter which is varied; it is substantial for both symmetric and asymmetric lead placement. Surprisingly, these dynamical effects do not influence the full distribution of peak heights, but are clearly seen in the correlation function or power spectrum. For non-zero temperature, the correlation function obtained theoretically is in good agreement with that measured experimentally.Comment: 5 color eps figure

    Structure and collective dynamics of liquid sodium

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    The temperature variation of the longitudinal and transverse phonon frequencies of liquid sodium is investigated using the approach by Hubbard Beeby. The molecular dynamics simulation is used to generate the pair correlation function of liquid sodium at various temperatures viz. T = 378 K, 473 K, 573 K, and 723 K, with 672 particles. To describe the electron-ion interaction our own model potential is employed along with a recent local field correction function due to Sarkar et al. To evaluate the parameter of the potential the zero pressure condition has been applied. The present results of g(r) are in good agreement with available experimental findings. The computed g(r) are used to investigate the temperature variation of the collective dynamics of liquid sodium. The amplitudes of the peaks of the longitudinal and transverse frequencies are suppressed while the width of the propagation gap for the transverse sound waves decreases with an increase in temperature. The computed longitudinal and transverse sound velocities at these temperatures are found to be encouraging.За ĐŽĐŸĐżĐŸĐŒĐŸĐłĐŸŃŽ ĐŒĐ”Ń‚ĐŸĐŽŃƒ ГаббарЎа-Бiбi ĐŽĐŸŃĐ»iЎжуĐČĐ°Đ»Đ°ŃŃŒ Ń‚Đ”ĐŒĐżĐ”Ń€Đ°Ń‚ŃƒŃ€ĐœĐ° Đ·Đ°Đ»Đ”Đ¶Đœiсть ĐżĐŸĐČĐ·ĐŽĐŸĐČĐ¶ĐœŃŒĐŸŃ— та ĐżĐŸĐżĐ”Ń€Đ”Ń‡ĐœĐŸŃ— Ń„ĐŸĐœĐŸĐœĐœĐžŃ… Ń‡Đ°ŃŃ‚ĐŸŃ‚ рiĐŽĐșĐŸĐłĐŸ ĐœĐ°Ń‚Ń€iю. ĐŸĐ°Ń€ĐœĐ° ĐșĐŸŃ€Đ”Đ»ŃŃ†iĐčĐœĐ° Ń„ŃƒĐœĐșцiя рiĐŽĐșĐŸĐłĐŸ ĐœĐ°Ń‚Ń€iю була Đ·Đ°ĐżŃ€ĐŸĐżĐŸĐœĐŸĐČĐ°ĐœĐ° про рiĐ·ĐœĐžŃ… Ń‚Đ”ĐŒĐżĐ”Ń€Đ°Ń‚ŃƒŃ€Đ°Ń…, Đ° ŃĐ°ĐŒĐ” T = 378 K, 473 K, 573 K та 723 K, Đ·Đ°ŃŃ‚ĐŸŃĐŸĐČуючо ĐŒĐ”Ń‚ĐŸĐŽ ĐŒĐŸĐ»Đ”ĐșŃƒĐ»ŃŃ€ĐœĐŸŃ— ĐŽĐžĐœĐ°ĐŒiĐșĐž ĐŽĐ»Ń 672 Ń‡Đ°ŃŃ‚ĐžĐœĐŸĐș. Опос ДлДĐșŃ‚Ń€ĐŸĐœ-iĐŸĐœĐœĐŸŃ— ĐČĐ·Đ°Ń”ĐŒĐŸĐŽiї Đ·ĐŽiĐčŃĐœŃŽĐČĐ°ĐČся Đ·Đ° ĐŽĐŸĐżĐŸĐŒĐŸĐłĐŸŃŽ Đ·Đ°ĐżŃ€ĐŸĐżĐŸĐœĐŸĐČĐ°ĐœĐŸĐłĐŸ Đ°ĐČŃ‚ĐŸŃ€Đ°ĐŒĐž ĐŒĐŸĐŽĐ”Đ»ŃŒĐœĐŸĐłĐŸ ĐżĐŸŃ‚Đ”ĐœŃ†iалу, ĐŽĐŸĐżĐŸĐČĐœĐ”ĐœĐŸĐłĐŸ Ń„ŃƒĐœĐșцiєю ХДрĐșара та iĐœ., Ń‰ĐŸ ĐŸĐżĐžŃŃƒŃ” ĐżĐŸĐżŃ€Đ°ĐČĐșу ĐœĐ° Đ»ĐŸĐșĐ°Đ»ŃŒĐœĐ” ĐżĐŸĐ»Đ”. Đ©ĐŸĐ± ĐŸŃ†iĐœĐžŃ‚Đž ĐżĐ°Ń€Đ°ĐŒĐ”Ń‚Ń€ ĐżĐŸŃ‚Đ”ĐœŃ†iалу, була Đ·Đ°ŃŃ‚ĐŸŃĐŸĐČĐ°ĐœĐ° ŃƒĐŒĐŸĐČĐ° ĐœŃƒĐ»ŃŒĐŸĐČĐŸĐłĐŸ тосĐșу. ĐžŃ‚Ń€ĐžĐŒĐ°Đœi Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Đž ĐŽĐ»Ń g(r) ĐŽĐŸĐ±Ń€Đ” ŃƒĐ·ĐłĐŸĐŽĐ¶ŃƒŃŽŃ‚ŃŒŃŃ Đ· Đ”ĐșŃĐżĐ”Ń€ĐžĐŒĐ”ĐœŃ‚Đ°Đ»ŃŒĐœĐžĐŒĐž ĐŽĐ°ĐœĐžĐŒĐž. На ĐŸŃĐœĐŸĐČi ĐŸĐ±Ń‡ĐžŃĐ»Đ”ĐœĐŸŃ— g(r) ĐČĐžĐČŃ‡Đ°Đ»Đ°ŃŃŒ Ń‚Đ”ĐŒĐżĐ”Ń€Đ°Ń‚ŃƒŃ€ĐœĐ° Đ·Đ°Đ»Đ”Đ¶Đœiсть ĐșĐŸĐ»Đ”ĐșтоĐČĐœĐŸŃ— ĐŽĐžĐœĐ°ĐŒiĐșĐž рiĐŽĐșĐŸĐłĐŸ ĐœĐ°Ń‚Ń€iю. ĐŸĐŸĐșĐ°Đ·Đ°ĐœĐŸ, Ń‰ĐŸ Đ· ĐżiĐŽĐČĐžŃ‰Đ”ĐœĐœŃĐŒ Ń‚Đ”ĐŒĐżĐ”Ń€Đ°Ń‚ŃƒŃ€Đž Đ°ĐŒĐżĐ»iтуЮо ĐŒĐ°ĐșŃĐžĐŒŃƒĐŒiĐČ ĐżĐŸĐČĐ·ĐŽĐŸĐČĐ¶ĐœŃŒĐŸŃ— i ĐżĐŸĐżĐ”Ń€Đ”Ń‡ĐœĐŸŃ— Ń‡Đ°ŃŃ‚ĐŸŃ‚ ĐżĐŸĐœĐžĐ¶ŃƒŃŽŃ‚ŃŒŃŃ, Đ° ŃˆĐžŃ€ĐžĐœĐ° ĐżŃ€ĐŸĐżĐ°ĐłĐ°Ń‚ĐŸŃ€ĐœĐŸŃ— щiĐ»ĐžĐœĐž ĐŽĐ»Ń ĐżĐŸĐżĐ”Ń€Đ”Ń‡ĐœĐžŃ… Đ°ĐșŃƒŃŃ‚ĐžŃ‡ĐœĐžŃ… хĐČĐžĐ»ŃŒ Đ·ĐČŃƒĐ¶ŃƒŃ”Ń‚ŃŒŃŃ

    Periodic orbit effects on conductance peak heights in a chaotic quantum dot

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    We study the effects of short-time classical dynamics on the distribution of Coulomb blockade peak heights in a chaotic quantum dot. The location of one or both leads relative to the short unstable orbits, as well as relative to the symmetry lines, can have large effects on the moments and on the head and tail of the conductance distribution. We study these effects analytically as a function of the stability exponent of the orbits involved, and also numerically using the stadium billiard as a model. The predicted behavior is robust, depending only on the short-time behavior of the many-body quantum system, and consequently insensitive to moderate-sized perturbations.Comment: 14 pages, including 6 figure

    Measurement of the Bs0→J/ψKS0B_s^0\to J/\psi K_S^0 branching fraction

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    The Bs0→J/ψKS0B_s^0\to J/\psi K_S^0 branching fraction is measured in a data sample corresponding to 0.41fb−1fb^{-1} of integrated luminosity collected with the LHCb detector at the LHC. This channel is sensitive to the penguin contributions affecting the sin2ÎČ\beta measurement from B0→J/ψKS0B^0\to J/\psi K_S^0 The time-integrated branching fraction is measured to be BF(Bs0→J/ψKS0)=(1.83±0.28)×10−5BF(B_s^0\to J/\psi K_S^0)=(1.83\pm0.28)\times10^{-5}. This is the most precise measurement to date

    Measurement of the CP-violating phase \phi s in Bs->J/\psi\pi+\pi- decays

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    Measurement of the mixing-induced CP-violating phase phi_s in Bs decays is of prime importance in probing new physics. Here 7421 +/- 105 signal events from the dominantly CP-odd final state J/\psi pi+ pi- are selected in 1/fb of pp collision data collected at sqrt{s} = 7 TeV with the LHCb detector. A time-dependent fit to the data yields a value of phi_s=-0.019^{+0.173+0.004}_{-0.174-0.003} rad, consistent with the Standard Model expectation. No evidence of direct CP violation is found.Comment: 15 pages, 10 figures; minor revisions on May 23, 201

    Model-independent search for CP violation in D0→K−K+π−π+ and D0→π−π+π+π− decays

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    A search for CP violation in the phase-space structures of D0 and View the MathML source decays to the final states K−K+π−π+ and π−π+π+π− is presented. The search is carried out with a data set corresponding to an integrated luminosity of 1.0 fb−1 collected in 2011 by the LHCb experiment in pp collisions at a centre-of-mass energy of 7 TeV. For the K−K+π−π+ final state, the four-body phase space is divided into 32 bins, each bin with approximately 1800 decays. The p-value under the hypothesis of no CP violation is 9.1%, and in no bin is a CP asymmetry greater than 6.5% observed. The phase space of the π−π+π+π− final state is partitioned into 128 bins, each bin with approximately 2500 decays. The p-value under the hypothesis of no CP violation is 41%, and in no bin is a CP asymmetry greater than 5.5% observed. All results are consistent with the hypothesis of no CP violation at the current sensitivity

    Search for the lepton-flavor-violating decays Bs0→e±Ό∓ and B0→e±Ό∓

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    A search for the lepton-flavor-violating decays Bs0→e±Ό∓ and B0→e±Ό∓ is performed with a data sample, corresponding to an integrated luminosity of 1.0  fb-1 of pp collisions at √s=7  TeV, collected by the LHCb experiment. The observed number of Bs0→e±Ό∓ and B0→e±Ό∓ candidates is consistent with background expectations. Upper limits on the branching fractions of both decays are determined to be B(Bs0→e±Ό∓)101  TeV/c2 and MLQ(B0→e±Ό∓)>126  TeV/c2 at 95% C.L., and are a factor of 2 higher than the previous bounds
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