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Walker, J. , "Three-Dimensional Laminar MHD Flows in Rectangular Ducts with Thin Conducting Walls and Strong Transverse Nonuniform Magnetic Fields," Liquid-Metal Flows and Magnetohydrodynamics, Proceedings of the Third Beer-Sheva International Seminar, New York, 1982, pp. 3-19. 7 Walker, J. , Ludford, G. S. , and Hunt, J. C. , "Three-Dimensional MHD Duct Flows with Strong Transverse Magnetic Fields, Part 2: Variable-Area Rectangular Ducts with Conducting Sides," Journal of Fluid Mechanics, Vol.

Figure 2 presents Ci(0) = f(M) and C i ( 2 ) = f (M) when increased from 0 to 350. We note that Ci (2) -> 0 rapidly and becomes very small, compared with Ci(o), when M > 150. 3 M for the values in Fig. 1. 10-3 (/= 2,714 )>=1,75 160 260 300 M Fig. 2 Influence of the Hartmann number upon the moment of the viscous friction torques (first case). HERVE AND C. 54 M. Consequently, when M increases from 0 to 200, the moment of the viscous friction torque upon the fixed disk is multiplied by 1100, whereas, at the same time, this moment is strongly decreased upon the rotating disk.

4 Influence of the m = w0/w parameter upon the function Cj* (M) with Z = 0. MHD FLOWS BETWEEN ROTATING DISKS 41 Consequently, the effect of the magnetic field upon the viscous couples remains very important. It enables us to envisage, from such an apparatus, the working of liquid metal electromagnetic clutches offering the advantage of being progressively adjusted by a separate or simultaneous action on COQ and BQ and with a very slight wear since there is no solid-solid friction. 6 mm All the walls of the container were made of Plexiglas, except one of the disks, which was made of copper with a thickness e = 10 mm.

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Abrasion and Ablation of Heavy Ions


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