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of
            depth   Earth.   both   depth
        239   (P)  at  of  the  density  (p)  of  the   the   within   and  Airy  models,  the   the  density  and   blocks.  In   the   block   everywhere   the   at   is   p,   mantle   of  com-

        lsostasy   Pressure   a)   point   a   equalizes  at   crustal   a   same   is   block   where   p;.   the   than   compensation.   depth   p,hy )   crustal


            8.18   function   above   Pratt   depends  on  thickness  (h)  of  crustal   models,  pressure   compensation.   by   the   each   <   <p:   Jess   of  depth   the   at   +   (pzh,   of  each
            FIGURE   is  a   (z)   material   For  the   b)   pressure   m/s”)   exerted  pressure   must  be  pressure   of   base   the  model,    .   psths   =   paghy   (g):   poh   =   pghy   p;   <   ps   <   ps   and  constant   is   the   to  extends   exerted  pressure   =   )   p,hy   +   base   the   from   of  compensation.


                                    Depth  of Compensation  «Constant   9.8   (~  gravity   to   point.   the  8.18b),   (Fig.   pgh   =   P   block  crustal   the   by   block  crustal   block.   crustal   the  models,   Airy   Pratt   the   For   that:   =   pyghy   =   pygh,   =   block  of  each   block.  of  each  constant     acceleration  gravitational   =   pshs   =   pzh,   =        8.19a.   Fig.   in  shown   mantle).  (Earth’s   (p,)  density  crustal   block  crustal   th











                                         acceleration   due   the   to  depth   models   Airy   and   as:   exerted  pressure   the   of  density   the   of  thickness   and   Pratt   the   of  compensation.  of  compensation,  so   P   density   =   Pgs  Ps   thickness   =   hs   hy,   P/g       model   Pratt   substratum  of  the   the  model   thickest   the   Only   model  isostatic   is:   g)   by  (divided   =   pzh,   =   thickness   =   h,’   block
                                   P



                                         =   =   Pratt   expressed   =   p =   i]   both   Pz.   P>-   hy,   a   out   particular   Airy   an   (p,).   Airy   P/g   h,’.h,’,
                                         g   z           P   h =   depth   depth   hy,       density
                                              the   be          In   the           Dividing   s   the   In   density   the   pensation   where:
                                              For   can   where:   at   exact   where:     In   the   For












            deflection  of   to   mountain   for  the   to  expected,  due   the



            Expected  a  plumb  bob  (highly  exaggerated),  due   of  the  mass  of  4   actual  deflection   less  than   and  Airy  models  of   both   by  crustal   planes  at   of  compensation.   of  water.   as

            a)       a  deficiency  of  mass  beneath            horizontal                          viewed
            8.16   Himalayas  was                           Pratt  isostatic  compensation.  In   on   body   a   be
            FIGURE   the  attraction   range.  b)  The   mountains.   8.17   models,  pressure  exerted   is  equal   below  the  depth   within   can  8.18a)
                                                            FIGURE   local   columns   and         point   (Fig.   point


                                                                                                   a
                                                                                                   on   Earth     the
                                                                                                   exerted   the  within   pgz   =   P   Earth   the   above  material





        lsostasy                                                                             of  Compensation   pressure   the   is   depth   to:   within   point   of  the

        and                                                                                        pressure   given   a   the   at   density
        Gravity                  Deflection                                                  Depth   at   pressure,  according   pressure   average


               of              Expected  Deflection                                                Hydrostatic   pressure   =   =
        Chapter 8   =  Angle   Deflection   Plumb  Bob   =   Actual   =                              Similarly,   lithostatic   where:   P   p

               6
                               6
                                 @
                                     i                                    Airy Model   es=
                                 _
        238
                                                                          b)   Sea Level
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