Chen Zhi-da. The Finite Rotation Parameter of a Deformable Body and Gyromagnetic Effect[J]. Applied Mathematics and Mechanics, 1983, 4(2): 151-157.
Citation: Chen Zhi-da. The Finite Rotation Parameter of a Deformable Body and Gyromagnetic Effect[J]. Applied Mathematics and Mechanics, 1983, 4(2): 151-157.

The Finite Rotation Parameter of a Deformable Body and Gyromagnetic Effect

  • Received Date: 1981-07-01
  • Publish Date: 1983-04-15
  • The derivation of Synge for the finite rotation formula in terms of Euler parameter is put into tensor form.Hence a further clarification of the geometric meaning of the orthogonal transformation obtained in the author's paper[7] is made. The tensor properties of rotation axis vector are also discussed. By means of the method of co-moving coordinate system established in[8],[9], we explain the gyromagnetic effect,and derive a simple formula for calculating body couple which is induced by magnetization.
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    Love.,A.E.H.,A treatise on the mathematical theory of elasticity,Dover,(1944),p.69.
    [2]
    Synge,J.L.,Classical dynamics,in“Handbuch der Physik”,Bd.ⅡI/1,10.
    [3]
    Kozik,T.J.,Finite rotations and associated displacement vector,J.Appl.Nech.,98(1976),698-699.
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    Koehler,T.R.and S.B.Trickey,Euler vectors and rotations about an arbitrary axis,Am.J.Phys.,46(6)(1978),650-651.
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    Wikes,J.M.,Rotations as solutions of a matrix differential equation,Am.J.Phys.46(6)(1978),685-687.
    [6]
    Beatty,M.F.,Vector analysis of finite rigid rotation,J.Appl.Mech.,99(1977),501-502.
    [7]
    陈至达,连续介质有限变形力学几何场论,力学学报,8(1979),107-117.中国矿院学报,1(1978),1-19.
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    陈至达,连续介质有限变形力学几何场论(广义弹性力学,岩石中的冲激波),中国矿院学报,2(1979),11-26.
    [9]
    陈至达,连续介质有限变形力学几何场论(弹性有限变形能量原理),清华大学学报,19,4(1979),44-57
    [10]
    陈至达,《有理力学》,中国矿院,北京,研究生部讲义,(1980).
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