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    A new look at decomposition of turbulence forcing field and the structural response

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    Measured cross-spectrum of a turbulence field usually shows some decay in the statistical correlation in addition to convection at a characteristic velocity. It is shown that a decaying turbulence can be decomposed into frozen-pattern components thus permitting a simpler way to calculate the structural response. This procedure also provides a relationship whereby the measured input spectra can be incorporated. The theory is applied to an infinite beam which is backed on one side by a fluid filled cavity and is exposed on the other side by the turbulence excitation. The effect of the free stream velocity is also taken into consideration

    Vibroacoustic response of structures and perturbation Reynolds stress near structure-turbulence interface

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    The interaction between a turbulent flow and certain types of structures which respond to its excitation is investigated. One-dimensional models were used to develop the basic ideas applied to a second model resembling the fuselage construction of an aircraft. In the two-dimensional case a simple membrane, with a small random variation in the membrane tension, was used. A decaying turbulence was constructed by superposing infinitely many components, each of which is convected as a frozen pattern at a different velocity. Structure-turbulence interaction results are presented in terms of the spectral densities of the structural response and the perturbation Reynolds stress in the fluid at the vicinity of the interface

    Arithmetic Properties of Overpartition Pairs

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    Bringmann and Lovejoy introduced a rank for overpartition pairs and investigated its role in congruence properties of ppˉ(n)\bar{pp}(n), the number of overpartition pairs of n. In particular, they applied the theory of Klein forms to show that there exist many Ramanujan-type congruences for the number ppˉ(n)\bar{pp}(n). In this paper, we shall derive two Ramanujan-type identities and some explicit congruences for ppˉ(n)\bar{pp}(n). Moreover, we find three ranks as combinatorial interpretations of the fact that ppˉ(n)\bar{pp}(n) is divisible by three for any n. We also construct infinite families of congruences for ppˉ(n)\bar{pp}(n) modulo 3, 5, and 9.Comment: 19 page
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