Computational Methods and Experimental Measurements: by T. F. Swean Jr., G. A. Keramidas (auth.), C. A. Brebbia, G.

By T. F. Swean Jr., G. A. Keramidas (auth.), C. A. Brebbia, G. A. Keramidas (eds.)

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Extra info for Computational Methods and Experimental Measurements: Proceedings of the 2nd International Conference, on board the liner, the Queen Elizabeth 2, New York to Southampton, June/July 1984

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And E. D. " J. Engrg Mech. , Proc. ASCE, 90, EM4, pp. 49-77. Einstein, A. " Ann. d. Physik, 17, p. 549. Hinze, J. O. (1975) Turbulence, McGraw-Hill, New York. Karweit, M. J. and S. " lecture Notes in Physics, 12, Springer-Verlag, Berlin, pp. 317-326. Kraichnan, R. H. " Phys. Fluids, 6-11, pp. 1603-1609. lorenz, E. N. " Tellus, 12-1, pp. 243-254. lumley, J. , and S. " Advances in Geophysics, 6, pp. 179-184. Patterson, G. , Jr. (1958) Private communication. Patterson, G. , Jr. and S. " Dynamics of Fluids and Plasmas, Academic Press, New York, pp.

The maximum direct capacitance between conductors was 30 pF per foot. The #18 AWG conductor had a maximum dc resistance of 7 ohms per 1000 feet. 1 ohms per 1000 feet. The kevlar stress braid provided the strength to the cable, resulting in a minimum breaking strength of 4000 lbf.

Inuous Field \ \ \ \ \ m _____ RE \ ,, ,, ,, " ", " .................. _--------- -- ... ,6------T,6----~;la====~~t2~~~t4 Figure 5. Eu1erian temporal corre1ation RE(T) for continuous and discrete fie1ds: T is the separation in timesteps. Resu1ts averaged over 50 rea1izations and all fie1d points. s. dispersion of a single particle at the end of 15 timesteps was the same as that of the discrete fields. s. single-particle dispersions. s. relative dispersion over time between two particles whose initial separations are given at t=O, using the second scaling.

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