3,637 research outputs found
ANĂLISE NĂO-LINEAR DA CONTRIBUIĂĂO DE ARMADURAS COMPLEMENTARES NA RESISTĂNCIA AO ARRANCAMENTO DE PINOS EMBUTIDOS EM CONCRETO
Conectores de aço com cabeça sĂŁo empregados na ligação entre estruturas mistas de aço e concreto e em estruturas prĂ©-moldadas. Quando solicitados Ă tração, a resistĂȘncia ao arrancamento Ă© fator determinante no projeto e o modo de ruptura pela formação do cone de concreto pode ser frĂĄgil. Uma das formas de aumentar a resistĂȘncia dessa ligação Ă© utilizar armaduras complementares. Para avaliar a influĂȘncia da armadura complementar na resistĂȘncia ao arrancamento, foram elaborados 6 modelos computacionais nĂŁo-lineares em EPD no programa MIDAS FEA, com base em uma sĂ©rie de ensaios experimentais de conectores embutidos em vigotas de concreto armado. A modelagem buscou avaliar a influĂȘncia do diĂąmetro da armadura complementar, do nĂșmero de pernas interceptando o cone de concreto e da distĂąncia do conector atĂ© da armadura complementar. Foi realizado um estudo paramĂ©trico para ajustar as propriedades do concreto, variando a resistĂȘncia Ă tração, mĂłdulo de elasticidade e a energia de fratura. A anĂĄlise computacional realizada apresenta tabelas com carga de ruptura, grĂĄficos de carga x deslocamento, carga x deformação na armadura longitudinal e carga x deformação na armadura transversal, de forma geral se apresentando em boa concordĂąncia com os resultados experimentais
The in-plane paraconductivity in La_{2-x}Sr_xCuO_4 thin film superconductors at high reduced-temperatures: Independence of the normal-state pseudogap
The in-plane resistivity has been measured in (LSxCO)
superconducting thin films of underdoped (), optimally-doped
() and overdoped () compositions. These films were grown
on (100)SrTiO substrates, and have about 150 nm thickness. The in-plane
conductivity induced by superconducting fluctuations above the superconducting
transition (the so-called in-plane paraconductivity, ) was
extracted from these data in the reduced-temperature range
10^{-2}\lsim\epsilon\equiv\ln(T/\Tc)\lsim1. Such a
was then analyzed in terms of the
mean-field--like Gaussian-Ginzburg-Landau (GGL) approach extended to the
high- region by means of the introduction of a total-energy cutoff,
which takes into account both the kinetic energy and the quantum localization
energy of each fluctuating mode. Our results strongly suggest that at all
temperatures above Tc, including the high reduced-temperature region, the
doping mainly affects in LSxCO thin films the normal-state properties and that
its influence on the superconducting fluctuations is relatively moderate: Even
in the high- region, the in-plane paraconductivity is found to be
independent of the opening of a pseudogap in the normal state of the underdoped
films.Comment: 35 pages including 10 figures and 1 tabl
ANĂLISE NĂO LINEAR DA INFLUĂNCIA DA FISSURAĂĂO NA RESISTĂNCIA AO ARRANCAMENTO DE PINOS EMBUTIDOS EM CONCRETO
Quando conectores de aço com cabeça sĂŁo solicitados Ă tração, uma forma de ruptura Ă© ocasionada pelo destacamento de uma regiĂŁo de concreto em torno do conector, em formato de cone. Sabe-se que o aumento do grau de fissuração na regiĂŁo do cone influencia negativamente na resistĂȘncia do conjunto. Este trabalho apresenta uma modelagem computacional com base em uma sĂ©rie de ensaios experimentais caracterizados pelo arrancamento de conectores de aço embutidos em prismas bi-apoiados de concreto armado. A modelagem visou avaliar a influĂȘncia do grau de fissuração na resistĂȘncia do conjunto, onde variou-se a taxa de armadura de flexĂŁo de 0,3 atĂ© 3,2% entre os modelos, resultando em diferentes graus de fissuração. A anĂĄlise numĂ©rica foi realizada usando o software MIDAS FEA. Foi feito um estudo paramĂ©trico em um dos modelos, para ajustar as propriedades do concreto, sendo os alvos do estudo a resistĂȘncia Ă tração, o mĂłdulo de elasticidade e a energia de fratura. Os valores definidos na anĂĄlise foram extrapolados para os outros modelos. Foram determinadas cargas de ruptura e grĂĄficos de carga x deslocamento para os modelos numĂ©ricos. Tais resultados foram comparados com os resultados experimentais, apresentando boa correlação, v dos modelos computacionais
Measurement of the relative rate of prompt Ïc0, Ïc1 and Ïc2 production at âs=7TeV
Prompt production of charmonium Ïc0, Ïc1 and Ïc2 mesons is studied using proton-proton collisions at the LHC at a centre-of-mass energy of âs=7TeV. The Ïc mesons are identified through their decay to J/ÏÎł, with J/ÏâÎŒ+muâ using photons that converted in the detector. A data sample, corresponding to an integrated luminosity of 1.0fbâ1 collected by the LHCb detector, is used to measure the relative prompt production rate of Ïc1 and Ïc2 in the rapidity range 2.0<y<4.5 as a function of the J/Ï transverse momentum from 3 to 20 GeV/c. First evidence for Ïc0 meson production at a hadron collider is also presented
Differential branching fraction and angular analysis of the decay B0âKâ0ÎŒ+ÎŒâ
The angular distribution and differential branching fraction of the decay B 0â K â0 ÎŒ + ÎŒ â are studied using a data sample, collected by the LHCb experiment in pp collisions at sâ=7 TeV, corresponding to an integrated luminosity of 1.0 fbâ1. Several angular observables are measured in bins of the dimuon invariant mass squared, q 2. A first measurement of the zero-crossing point of the forward-backward asymmetry of the dimuon system is also presented. The zero-crossing point is measured to be q20=4.9±0.9GeV2/c4 , where the uncertainty is the sum of statistical and systematic uncertainties. The results are consistent with the Standard Model predictions
Measurement of the CKM angle Îł from a combination of B±âDh± analyses
A combination of three LHCb measurements of the CKM angle Îł is presented. The decays B±âD K± and
B±âDϱ are used, where D denotes an admixture of D0 and D0 mesons, decaying into K+Kâ, Ï+Ïâ, K±Ïâ, K±ÏâϱÏâ, K0SÏ+Ïâ, or K0S K+Kâ ïŹnal states. All measurements use a dataset corresponding to 1.0 fbâ1 of integrated luminosity. Combining results from B±âD K± decays alone a best-ïŹt value of
Îł =72.0⊠is found, and conïŹdence intervals are set
Îł â [56.4,86.7]⊠at 68% CL,
Îł â [42.6,99.6]⊠at 95% CL.
The best-ïŹt value of Îł found from a combination of results from B±âDϱ decays alone, is Îł =18.9âŠ,
and the conïŹdence intervals
Îł â [7.4,99.2]⊠âȘ [167.9,176.4]⊠at 68% CL
are set, without constraint at 95% CL. The combination of results from B± â D K± and B± â Dϱ
decays gives a best-ïŹt value of Îł =72.6⊠and the conïŹdence intervals
Îł â [55.4,82.3]⊠at 68% CL,
Îł â [40.2,92.7]⊠at 95% CL
are set. All values are expressed modulo 180âŠ, and are obtained taking into account the effect of D0âD0
mixing
Observation of the decay
The decay is observed for the first
time, using proton-proton collisions collected with the LHCb detector
corresponding to an integrated luminosity of 3fb. A signal yield of
decays is reported with a significance of 6.2 standard deviations.
The ratio of the branching fraction of \B_c \rightarrow J/\psi K^+ K^- \pi^+
decays to that of decays is measured to be
, where the first uncertainty is statistical and the
second is systematic.Comment: 18 pages, 2 figure
Study of DJ meson decays to D+Ïâ, D0Ï+ and Dâ+Ïâ final states in pp collisions
A study of D+Ïâ, D0Ï+ and Dâ+Ïâ final states is performed using pp collision data, corresponding to an integrated luminosity of 1.0 fbâ1, collected at a centre-of-mass energy of 7 TeV with the LHCb detector. The D1(2420)0 resonance is observed in the Dâ+Ïâ final state and the Dâ2(2460) resonance is observed in the D+Ïâ, D0Ï+ and Dâ+Ïâ final states. For both resonances, their properties and spin-parity assignments are obtained. In addition, two natural parity and two unnatural parity resonances are observed in the mass region between 2500 and 2800 MeV. Further structures in the region around 3000 MeV are observed in all the Dâ+Ïâ, D+Ïâ and D0Ï+ final states
Study of B0(s)âK0Sh+hâČâ decays with first observation of B0sâK0SK±Ïâ and B0sâK0SÏ+Ïâ
A search for charmless three-body decays of B 0 and B0s mesons with a K0S meson in the final state is performed using the pp collision data, corresponding to an integrated luminosity of 1.0 fbâ1, collected at a centre-of-mass energy of 7 TeV recorded by the LHCb experiment. Branching fractions of the B0(s)âK0Sh+hâČâ decay modes (h (âČ) = Ï, K), relative to the well measured B0âK0SÏ+Ïâ decay, are obtained. First observation of the decay modes B0sâK0SK±Ïâ and B0sâK0SÏ+Ïâ and confirmation of the decay B0âK0SK±Ïâ are reported. The following relative branching fraction measurements or limits are obtained B(B0âK0SK±Ïâ)B(B0âK0SÏ+Ïâ)=0.128±0.017(stat.)±0.009(syst.), B(B0âK0SK+Kâ)B(B0âK0SÏ+Ïâ)=0.385±0.031(stat.)±0.023(syst.), B(B0sâK0SÏ+Ïâ)B(B0âK0SÏ+Ïâ)=0.29±0.06(stat.)±0.03(syst.)±0.02(fs/fd), B(B0sâK0SK±Ïâ)B(B0âK0SÏ+Ïâ)=1.48±0.12(stat.)±0.08(syst.)±0.12(fs/fd)B(B0sâK0SK+Kâ)B(B0âK0SÏ+Ïâ)â[0.004;0.068]at90%CL
Observations of BÂșsâÏ(2S)η and BÂș(s)âÏ(2S)Ï+Ï- decays
First observations of the B0s
âÏ(2S)η, B0 âÏ(2S)Ï
+
Ï
â and B0s
âÏ(2S)Ï
+
Ï
â decays are made
using a dataset corresponding to an integrated luminosity of 1.0 fbâ1 collected by the LHCb experiment in
protonâproton collisions at a centre-of-mass energy of
â
s = 7 TeV. The ratios of the branching fractions
of each of the Ï(2S) modes with respect to the corresponding J/Ï decays are
B(B0s
âÏ(2S)η)
Ă·
B(B0s
âJ/Ïη)
= 0.83± 0.14 (stat)±0.12 (syst) ±0.02 (B),
;
B(B0âÏ(2S)Ï
+
Ï
â
)
Ă·
B(B0âJ/ÏÏ
+
Ï
â
)
= 0.56± 0.07 (stat)±0.05 (syst)± 0.01 (B),
;
B(B0s
âÏ(2S)Ï
+
Ï
â
)
Ă·
B(B0s
âJ/ÏÏ
+
Ï
â
)
= 0.34± 0.04 (stat)±0.03 (syst)± 0.01 (B),
where the third uncertainty corresponds to the uncertainties of the dilepton branching fractions of the J/Ï
and Ï(2S) meson decays
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