903 research outputs found

    Theoretical pressure distributions over arbitrarily shaped periodic waves in subsonic compressible flow and comparison with experiment

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    Theoretical solution for pressure distribution over arbitrarily shaped periodic waves using Fourier serie

    Pressure drags due to two-dimensional fabrication-type surface roughness on an ogive cylinder at transonic speeds

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    Pressure drags due to two-dimensional fabrication- type surface roughness on ogive cylinder at transonic speed

    Semileptonic b --> u decays: lepton invariant mass spectrum

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    We compute O(alpha_s^2) QCD corrections to the lepton invariant mass spectrum in the decay b --> u l nu_l, relevant for the determination of the CKM matrix element |V_{ub}|. Our method can also be used to evaluate moments of the lepton energy distribution with an O(alpha_s^2) accuracy. The abelian part of our result gives the neutrino invariant mass spectrum in the muon decay and, upon integration, the O(alpha^2) correction to the muon lifetime.Comment: 5 pages, revte

    Dipole Excitation of Dipositronium

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    The energy interval between the ground and the P-wave excited states of the recently discovered positronium molecule Ps_2 is evaluated, including the relativistic and the leading logarithmic radiative corrections, E_P-E_S = 0.181 586 7(8) a.u. The P-state, decaying usually via annihilation, is found to decay into the ground state by an electric dipole transition 19 percent of the time. Anticipated observation of this transition will provide insight into this exotic system.Comment: 5 page

    Lepton flavor violating μ→eγ\mu\to e\gamma and μ−e\mu-e conversion in unparticle physics

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    We have studied lepton flavor violation processes μ→eγ\mu\to e\gamma and μ−e\mu-e conversion in nuclei induced by unparticle. Both Br(μ→eγ){\rm Br}(\mu\to e\gamma) and μ−e\mu-e conversion rate CR(μ−e,Nuclei){\rm CR}(\mu-e,{\rm Nuclei}) strongly depend on the scale dimension dUd_{\cal U} and the unparticle coupling λKff′\lambda^{ff'}_{\rm K}(K=V, A, S, P). Present experimental upper bounds on Br(μ→eγ){\rm Br}(\mu\to e\gamma), CR(μ−e,Ti){\rm CR}(\mu-e,{\rm Ti}) and CR(μ−e,Au){\rm CR}(\mu-e,{\rm Au}) put stringent constraints on the parameters of unaprticle physics. The scale dimensions dUd_{\cal U} around 2 are favored for the unparticle scale ΛU\Lambda_{\cal U} of O(10TeV){\cal O}(10 {\rm TeV}) and the unparticle coupling of O(10−3){\cal O}(10^{-3}). CR(μ−e,Nuclei){\rm CR}(\mu-e,{\rm Nuclei}) is proportional to Zeff4A2/Z\rm{Z^4_{eff}A^2/Z} for the pure vector and scalar couplings between unparticle and SM fermions, this peculiar atomatic number dependence can be used to distinguish unparticle from other theoretical models.Comment: 16 pages, 5 figure

    Turbulent Skin Friction at High Reynolds Numbers and Low Supersonic Velocities

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    Turbulent skin friction at high Reynolds number and low supersonic speed

    Measurement by wake momentum surveys at Mach 1.61 and 2.01 of turbulent boundary-layer skin friction on five swept wings

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    Measurement by wake momentum surveys at Mach 1.61 and 2.01 of turbulent boundary layer skin friction on five swept wing

    Effects of Nose Angle and Mach Number on Transition on Cones at Supersonic Speeds

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    An investigation has been made to determine the transition characteristics of a group of smooth, sharp-nosed cones varying from 10 degrees to sixty degrees in included apex angle over a Mach number range from 1.61 to 2.20 and a range of Reynolds number per foot from about 1.5 x 10 to the 6th power to 8 x 10 to the 6th power. Increasing the cone angle is shown to decrease slightly the transition Reynolds number, whereas the effects of changes of Mach number and unit Reynolds number are negligible. When transition occurred within 15 to 20 percent of the model length from the base there was a dropoff in transition Reynolds number. (author

    An estimate of the QCD corrections to the decay Z --> W u d

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    We present an estimate of perturbative QCD corrections to the decay Z→WudˉZ \to Wu\bar d. A simple approximate approach is described in detail. The difference of masses of MZM_Z and MWM_W is used as an expansion parameter. A complete analytical formula for a part of the corrections is also presented.Comment: 9 pages, late

    Boundary-Layer Transition on a Group of Blunt Nose Shapes at a Mach Number of 2.20

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    An investigation has been made to study boundary-layer transition on six axisymmetrical blunt bodies of revolution. Model shapes were selected with respect to the degree of favorable pressure gradient over the model surface. Tests were conducted at a Mach number of 2.20 and over a range of free-stream Reynolds number per foot of about 1.4 x 10(exp 6) to 6.5 x 10(exp 6). The tests were made at an angle of attack of 0 deg. with zero heat transfer. For the hemisphere, the flow remained essentially laminar over the model surface length for the entire pressure range of the tests. For a strong favorable pressure gradient followed by any weak favorable, neutral, or adverse gradient, the tendency was for transition to occur at or immediately behind the shoulder. A single strip of three-dimensional roughness in the region of strong favorable pressure gradient did not fix transition on the models at the roughness location except at the maximum test pressures, whereas a second roughness strip added in a region of neutral or adverse pressure gradient did fix transition. Experimental pressure coefficients agreed closely with modified Newtonian theory except in the shoulder region
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