Page 182 - Well Logging and Formation Evaluation
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172               Well Logging and Formation Evaluation

          such disturbances may be detected (typically  <15m) and the uncertain
          nature of the magnetization.
            Since standard surveying tools, such as MWD (measurement while
          drilling), now possess accurate magnetometers, there is no need for
          dedicated tools for magnetostatic homing in. However, interpretation
          from such tools is not straightforward. It is hoped that the following will
          provide some useful techniques, as well as a better understanding of mag-
          netic surveying in general.

          12.1.1 Magnetization of Steel Casing/Drillstrings

            As a result of the manufacturing process, or from subsequent magnetic
          inspection or mechanical shocks, the steel used in making casing,
          drillpipe, or accessories (e.g., jars, drill collars, bits) usually acquires a
          degree of magnetization. The simplest model for describing the field due
          to such a magnetization is in terms of a superposition of magnetic point
          monopoles of either north or south polarity. A north monopole is defined
          as one for which the lines of magnetic flux flow symmetrically and spher-
          ically toward the pole; for a south pole, the lines of flux flow similarly
          away from the pole.  Although free monopoles are never observed in
          nature, in the vicinity of a pole, of which the opposite pole is far removed,
          the field will be dominated by that of the near pole, and the far pole may
          be ignored. When two or more poles are a similar distance from the point
          of measurement, the field is a linear superposition of the monopole field
          due to each of the individual poles. The magnetic field due to a monopole
          in a Cartesian reference system is as follows:

                                  3
                  r M x ( * *
            F x = m *  *   4  p  r )                                (12.1.1)
                                  3
            F y = m *  *   4  p  r )                                (12.1.2)
                  r M y ( * *
                                 3
            F z = m *  *   4  p  r )                                (12.1.3)
                  r M z ( * *
          where:
           r =  ( x 2 +  y 2 + ) , in m
                         z 2
          M = the pole strength, in Webers (Wb)
          F x, F y, F z are the field strengths, in Tesla (T)
          mr is the relative magnetic permeability of the medium
          x, y, z are the distances, in m, from the monopole to the measuring point
          along the x, y, and z axes.
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