• DocumentCode
    1040541
  • Title

    The seismic pulse, an example of wave propagation in a doubly refracting medium

  • Author

    Pekeris, C.L.

  • Author_Institution
    The Weizmann Institute, Rehovot, Israel
  • Volume
    4
  • Issue
    3
  • fYear
    1956
  • fDate
    7/1/1956 12:00:00 AM
  • Firstpage
    508
  • Lastpage
    511
  • Abstract
    An exact and closed solution is given for the motion produced on the surface of a uniform elastic half-space by the sudden application of a concentrated pressure-pulse at the surface. The time variation of the applied stress is taken as the Heaviside unit function, and its concentration at the origin is such that the integral of the force over the surface is finite. This problem gives an instructive illustration of wave propagation in a doubly refracting medium, since both shear waves and compressional waves are excited, and they travel with different speeds. There is, in addition, the Rayleigh surface wave. For a medium in which the elastic constants \\lambda and \\mu are equal, the vertical component of displacement \\omega _{o} at the surface is given by: \\omega _{o} = 0 , \\tau < frac{1}{\\sqrt {3}} , {\\omega}_{o} = - {Z \\over \\pi\\mu r} \\Bigg\\{ {3 \\over 16} - {\\sqrt{3} \\over 32\\sqrt{{\\tau}^{2} - {1 \\over 4}}} - {\\sqrt{5+3\\sqrt{3}} \\over 32\\sqrt{{3 \\over 4} + {\\sqrt{3} \\over 4} - {\\tau}^{2}}} + {\\sqrt{3\\sqrt{3} - 5} \\over 32\\sqrt{{\\tau}^{2} + {\\sqrt{3} \\over 4} - {3 \\over 4}}} \\Bigg\\} , frac{1}{\\sqrt {3}}< \\tau < 1 , \\omega _{o}= - \\frac{Z}{\\pi \\mu r} \\Bigg\\{ \\frac{3}{8} - \\frac{ \\sqrt{5 + 3 \\sqrt{3}}}{16\\sqrt{ \\frac{3}{4} + \\frac{\\sqrt{3}}{4} - \\tau ^{2} }} \\Bigg\\}, 1 < \\tau < \\frac{1}{2} \\sqrt{3+\\sqrt{3}} , \\omega _{o} = - frac{Z}{\\pi\\mu r}frac{3}{8}, \\tau > frac{1}{2}\\sqrt {3 + \\sqrt {3}} , where \\tau = (ct/r) , c -shear wave velocity, and -Z is the surface integral of the applied stress. The horizontal component of displacement is obtained similarly in terms of elliptic functions. A discussion is given of the various features of the waves. It is pointed out that in the case of a buried source, an observer on the surface will, under certain circumstances, receive a wave which travels to the surface as an S wave along the ray of total reflection, and from there along the surface as a dif- fracted P wave. An exact expression is given for this diffracted wave. The question of the suitability of automatic computing machines for the solution of pulse propagation problems is also discussed.
  • Keywords
    Acoustic propagation in anisotropic media; Acoustic transient propagation; Seismology; Diffraction; Helium; Integral equations; Mathematics; Reflection; Seismic waves; Stress; Surface waves;
  • fLanguage
    English
  • Journal_Title
    Antennas and Propagation, IRE Transactions on
  • Publisher
    ieee
  • ISSN
    0096-1973
  • Type

    jour

  • DOI
    10.1109/TAP.1956.1144429
  • Filename
    1144429