By K. Miya
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It really is shut adequate to the top of the century to make a wager as to what the Encyclopedia Britannica article at the background of arithmetic will record in 2582: "We have stated that the dominating subject of the 19th Century was once the improvement and alertness of the speculation of services of 1 variable.
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Extra info for Applied Electromagnetics in Materials. Proceedings of the First International Symposium, Tokyo, 3–5 October 1988
Magnetic field and stress analysis of saturated steel. IEEE, Trans. Mag-24,230-233. Moon, F. C. and Pao, Y - H ( 1 9 6 8 ) . Magnetoelastic buckling thin plate. ASME J. Appl. , 35, 53-58. of Moon, F . C . ( 1 9 8 4 ) . Magneto-solid mechanics. John Wiley & New York. (1972). Postbuckling analysis of a beam. Appl. , 39, 207-211. (1971). Self-consistently computed magnetization patterns in thin magnetic recording media. IEEE Trans. Mag-7, 873. Tone,T. et a l . ( 1 9 8 3 ) . A study of the reactor structure concept of the tokamak power reactor SPTR-P.
191-196. Singular M o m e n t s in a Cracked Soft Ferromagnetic Plate Under Bending Y. SHINDO and K. HORIGUCHI Department of Mechanical Engineering II, Faculty of Engineering, Tohoku University, Sendai 980, Japan ABSTRACT A magneto-elastic analysis is presented for the bending problem of a soft ferromagnetic thin plate with a through crack under a uniform magnetic field. Fourier transform method is used to solve the magneto-elastic problem and the result is expressed in terms of an integro-differential equation for the deflection.
This coil was putted under the plate so that its center agreed with that of the plate. A schematic diagram of the test set -up is shown in Fig. 6. The current I(t) of the coil generates a time -varying magnetic induction. The magnetic induction can be determined Fig. 6 A schematic diagram of the test set-up. Dynamic Behavior of Flawed Thin Plates 33 analytically. 2 z [K(k) + E(k)] (R - r)* + z' 2iTr[(R + r ) + z ] (8) where Ν is the number of turn per unit length of the coil and k 2 _ 2 N4Rr 2 z (R + r ) + z In these equations, an origin of the cylindrical co-ordinates (r, Θ, z) is placed on the centre of the circular coil, and K(k) and E(k) are complete elliptic integrals of the first and second kind, respectively.