This Demonstration shows a cylindrical magnet falling inside a conducting pipe. This fall is damped by the opposing force due to eddy currents generated in the conducting pipe.
Two models are used for the calculations: the point-dipole model of a magnet [1–3] (model 1) and the exact cylindrical magnet model [4, 5] (model 2). The cylindrical magnet model contains a double integral; therefore, calculation is very slow. The results of both models coincide when  and  both equal 1.6.  = pipe length,  = outer diameter of the pipe,  = thickness of the pipe wall,  = radius of the magnet,  = height of the magnet,  = volume of the magnet,  = remnant field.  ,  ,  , terminal velocity,  , drag coefficient for infinite pipe (point-dipole models),  ,  , inner and outer radius of pipe,  volume of magnet,  = conductivity of metallic pipe,  , drag force.  , drag force for finite pipe (point-dipole model).  , drag coefficient for infinite pipe (point-dipole model). The velocity  was found as the solution of the equation of motion by an iterative method:  . [1] B. A. Knyazev, I. A. Kotelnikov, A. A. Tyutin and V. S. Cherkassky, "Braking of a Magnetic Dipole Moving with an Arbitrary Velocity through a Conducting Pipe," Physics-Uspekhi, 49(9), 2006 pp. 937–946. doi:10.1070/PU2006v049n09ABEH005881. [2] A. K. Thottoli, M. Fayis, T. C. Mohamed, T. Amjad, P. T. Shameem and M. Mishab, "Study of Magnet Fall through Conducting Pipes Using a Data Logger," SN Applied Sciences, 1(9), 2019 1050. doi:10.1007/s42452-019-1086-z. [3] C. S. MacLatchy, P. Backman and L. Bogan, "A Quantitative Magnetic Braking Experiment," American Journal of Physics, 61(12), 1993 pp. 1096–1101. doi:10.1119/1.17356. [4] N. Derby and S. Olbert, "Cylindrical Magnets and Ideal Solenoids," American Journal of Physics, 78(3), 2010 pp. 229–235. doi:10.1119/1.3256157. [5] Q. L. Peng, S. M. McMurry and J. M. D. Coey, "Axial Magnetic Field Produced by Axially and Radially Magnetized Permanent Rings," Journal of Magnetism and Magnetic Materials, 268(1–2), 2004 pp. 165–169. doi:10.1016/S0304-8853(03)00494-3.
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