Page 29 - Numerical Analysis and Modelling in Geomechanics
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10 JOHN W.BULL AND C.H.WOODFORD

            Table 1.2 Deflection readings in percent for the undisturbed subgrade.















            model  was  constructed  by  rotating  a  three-dimensional  slice  about  its  vertical
            axis using the interactive facilities of the PAFEC software. It would have been
            possible  to  obtain  the  three-dimensional  slice  by  rotating  a  two-dimensional
            cross-section and in so doing form three-dimensional brick and wedge elements
            from  two-dimensional  quadrilateral  and  triangular  elements,  but  this  was
            considered to be an unnecessary simplification. The analysis could not be carried
            out in two dimensions as the camouflet is a three-dimensional structure with some
            load combinations, not reported here, also being in three dimensions.
              The manual production of the PAFEC data for a single slice would have been
            a fairly routine matter but in order to allow for varying depths of the camouflet
            the  process  was  automated.  A  program  was  written  to  produce  PAFEC  data,
            which used an input depth parameter to calculate nodal coordinates. In order to
            keep  the  total  number  of  elements  within  reasonable  bounds  and  maintain
            element aspect ratios consistent with PAFEC guidelines, the relatively thin 300
            mm  layer  of  the  cement  concrete  runway  and  the  size  of  the  slice  decided
            effectively  the  finite  element  mesh.  For  the  uniform  pressure  load  cases  under
            consideration  a  single  layering  of  elements  was  used  to  model  the  runway
            surface  layer.  The  size  of  the  slice  was  such  that  five  successive  18°  rotations
            produced  a  quarter  section  of  the  cylindrical  model,  which  through
            considerations of symmetry and by the application of appropriate restraints was
            sufficient  for  subsequent  analysis.  Natural  boundary  conditions  were  modelled
            by  fully  restraining  the  lower  flat  surface  of  the  cylinder.  Movement  in  the
            curved surface of the cylinder was restricted to the vertical direction.
              The  subgrade  surrounding  the  camouflet  was  modelled  to  a  depth  below  its
            detonation point equal to the height above. The radius of the modelling cylinder
            was comparable with its height. By opting for an aspect ratio of approximately 1:
            3  in  the  surface  elements  it  was  found  that  the  overwhelming  majority  of
            remaining  elements  in  the  model  had  aspect  ratios  within  the  1:5  ratio
            recommended by PAFEC. Breaches of the guidelines, which did occur, were not
            sufficient to incur error messages and did not occur in significant areas.
              A  typical  cross-section  of  the  finite  element  mesh  is  shown  in  Figure  1.2.
            There would be up to 4350 elements and 47, 750 degrees of freedom. The stress
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