Page 320 - Air and Gas Drilling Manual
P. 320

Chapter 8: Air, Gas, and Unstable Foam Drilling    8-3
                                   In Chapter 6 the basic direct circulation drilling  planning  governing  equations
                               have  been  derived  and  summarized.    In  Chapter  7  the  basic  reverse  circulation
                               drilling  planning governing equations have been derived and summarized.    In  this
                               chapter  only  direct  circulation  illustrative  examples  are  discussed.    Reverse
                               circulation examples are discussed in Chapter 5.
                               8.2  Minimum  Volumetric  Flow  Rate
                                   There are various research groups that over the past three decades have developed
                               several mathematical and empirical models for use in  attempting to  describe the gas
                               flow mechanics of air and gas drilling  operations.   Each  of  the  models  developed
                               over the decades have made a variety of assumptions concerning the specific weight
                               of the gas and rock cuttings mixture created at the bottom of the hole as the drill  bit
                               advances.
                                 8.2.1 Discussion of Theories
                                   In  1957,  R.  R.  Angel  developed  the  first  field  useful  mathematical  and
                               empirical model for  air  and  gas  drilling  operations  [3,  4].    This  initial  work  by
                               Angel was supported by industry (i.e.,  Phillips Petroleum Company) and continues
                               to be useful to drilling supervisors and drilling engineers even today.  This  modeling
                               effort drew heavily from the large body of engineering knowledge related to industrial
                               pneumatic conveying (the transport of solids by flowing air).  Thus,  this  model was
                               developed from the outset to be an engineering tool.  The major air and rock cuttings
                               mixture  assumption  made  in  this  model  was  that  the  rock  cutting  particles  move
                               together from the bottom of the borehole to the surface with the velocity of the local air
                               flow.  Through the decades other researchers have improved on this model [5].
                                   In 1981, interest in air and gas drilling technology found its  way into  academic
                               research  [6,  7].    This  research  was  carried  out  at  University  of  Tulsa  and
                               Pennsylvania State University and was supported by U.  S.  Department  of  Energy.
                               In this effort experimental work was carried out to  ascertain the relationship between
                               the motion of the air and the rock cuttings particles.   This  experimental work found
                               that  the  vertical  drilling  annulus  geometry  with  an  upward  flow  of  air  and  rock
                               cuttings chokes in  much  the  same  way  as  industrial  pneumatic  conveying.    This
                               experimental  work  also  showed  that  under  simulated  practical  drilling  conditions
                               small rock particles flow with a velocity that was near that of the air.   This  research
                               effort resulted in a model that was a variation on the original Angel work.   The slip
                               of the rock cutting particles relative to the air flow was ignored.   The model resulted
                               in a air and rock mixture value that was nearly the same as that given by the original
                               Angel model.
                                   In 1983,  the first  model  was  proposed  that  took  into  account  a  rock  cutting
                               particle velocity that was different from that of the  air  flow  [8].    This  model  can
                               yield an improved air and rock mixture value which can improve the accuracy of the
                               predictions from the model.    The problem  with  this  model  is  that  the  individual
                               average velocities of the particles are difficult to  determine analytically for inclusion
                               in this model.
                                   In  1992,  additional  theoretical  work  was  carried  out  to  further  refine  the
                               inclusion  of  the  effect  of  rock  cuttings  particle  velocities  [9].    This  model  also
                               suffered from the difficulty involved in determining average particle velocities.
   315   316   317   318   319   320   321   322   323   324   325