Page 253 - Biomedical Engineering and Design Handbook Volume 2, Applications
P. 253

232  DIAGNOSTIC EQUIPMENT DESIGN

                                          B Gz
                                                  z
                                                            y






                                             B G1                      B G2


                                    z                                  x



























                                   FIGURE 8.2 A filamentary, single turn Maxwell coil pair z gradient coil is
                                   illustrated. In addition, a typical unshieled z gradient coil is shown.
                       The portion of Eq. (8.8) following the approximation sign is a Taylor series expansion about z = 0. Note
                                                                                      5
                                     3
                       that if the factor of z were zero, gradient error would be reduced to terms dependent on z . Selecting
                                      3
                       d = 0.5 3  makes the z factor vanish. The remaining relative error from the ideal gradient may be approx-
                       imated by dividing the fifth-order z factor by the first-order z factor:
                                                           176z 4
                                                     Error ≈                               (8.9)
                                                           343a  4
                       Equation (8.9) predicts that, for Maxwell coils, the gradient deviates 10 percent from the ideal linearity
                       at z/a = 0.66. For a = 0.3 m, this deviation takes place at z = 0.2 m (e.g., the field of view would be
                       40 cm if 10 percent deviation from linearity was the maximum desired).
                         The first term in z of the expansion of Eq. (8.8) is the gradient amplitude G for a Maxwell pair.
                       So from Eq. (8.7), the current needed to produce a gradient G may be expressed as
                                                        49 Ga 2  21
                                                     I =                                  (8.10)
                                                         144μ
                                                             0
   248   249   250   251   252   253   254   255   256   257   258