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89                      for              4.14b)   the   of   from   downdip

      Models                  solving   by     (Fig.   graph   slope   the   (V,)   layer   shooting   :  downdip

      Interpretation          determined   be   (V,/Vou)   (Vi/  Vo.)   travel-time   of  inverse   the   refracting   the       (X),  distance   shooting   updip:  shooting


           easy  =  see   V,,,  2a   «)   —  sin (8,   downdip  shooting   updip  shooting   layer  overlying   can  critical  angle   the   sin“   —  sin™'(V,/V2q)   2   sin”!   +  (V,/Voa)   2   the   from  determined   as   (V,)   layer  overlying   of  velocity   the   for       1      arrival  of  direct   slope   Vi       sin®,      horizontal   at  receiver   het   Dy   +  |   when  interface   to   Viti   2   hi,  4"   20s   @,   when  interface   to  distance   te   Vi   =







                                                                               1

                                                                               &


                                         =
                   apparent  velocity   velocity  apparent   of  the  velocity   angle   critical   interface.   the   of   dip   and  interface   of the   simultaneously:   a=   sin”!   i  _   be   can  velocities   the   of  velocity   solving   then   and   Y=   Va       a   to   times   (T,),  are:   ee 0.       L   6.  2h, ae       l  perpendicular  distance   perpendicular



                    Va   Vou   V, =   6, =   =   a   dip   The   V,,   true   The   the  reading   arrival,   Law:   travel   The   updip   and   —   em   =   hy   =   h,

                where:           and   V,,       by   direct   Snell’s   (Ty)        where:












                 the
                  B
          reversed  refraction  the  combination  of surveys  downdip  and  updip  directions   the  source  at  A,   from   traverses   B,   at  the  shot   A.  The   are  in  (b)   the  same.  Apparent   in  (b)  are  different,  rays  emerge  at  different   for  the  downdip  (Fig.  4.13a)  and   is  deeper  beneath  intercept  time  (t,,)  for  updip   when  shooting   as   uti-   refrac-   times




          A    ray   receiver  at   as  a  ray  from   receiver  at   times T,,  and  Ty,   angles.  b)  Superposition  of  travel-time  updip  (Fig.  4.13b)  surveys.  Note  that,   interface   is  greater  than   same   the   is  raypath   if   downdip
          4.14   is   (Fig.  4.13).  a)  A   to  a   therefore  exactly  velocities  V,,  and  V,,   the   the   the   (t,y).   be   verify   reciprocal   the   in
          FIGURE   profile   shooting  in   shooting   same  course   shooting  to  a   reciprocal   because   curves   because   B,   Shot   shooting   downdip   to   has   the   exact   can   one   T,,.   If   shooting

                                                                               however,     B   A,   4.14b),   =   when


             s   oS                                                            B,   at   at  A,  because   at   at   (Fig.   if  T,,   arrival   a)
     Interpretation   city  Velo                                              receiver   a   receiver   equal:   be   Tea   =   Tas   receiver   to   at  A   receiver   to   at B   plot  refraction   determining   will  erroneous.   be   refracted   Vv,  +   in  (0,   =






     Refraction   ——>   App  arent   igh   Hi                                 shot   the   to   A   at   shot   to a   B   at   must   from   time   shot   from   time   shot   reversed   by  interface   below  analysis   velocities   the   for   are:   Vea



     Seismic   Velocity   4                                                   from   time   the   from   time   reciprocal  times   the   =   travel   =   travel   events   a   on   same   the   from   the  same,   apparent   directions



     Chapter4   Low  Apparent                                                 travel   The   travel   the   Thus  lized.   where:   Tg   Tpa   picking   tions   are   the   not   The   and  updip




     88     es                                                                                  In   are
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