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第 42 卷 第 2 期          王佳乐等: 曲线坐标系下孔隙介质圆柱纵向表面波的传播特性                                          433


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             附录A

                                                      [                     ]
                                                                (        )
                                              A + Qη 1  2    2    1    1         2
                                       m 11 =          q − k +       +     q 1 + q ,
                                                        1
                                                                                 1
                                                2N                ρ α  ρ β
                                                      [                     ]
                                                                (        )
                                              A + Qη 2  2    2    1    1         2
                                       m 12 =          q − k +       +     q 2 + q ,
                                                                                 2
                                                        2
                                                2N                ρ α  ρ β
                                               (       2       )
                                                      l 0    1
                                       m 13 = ik s +      −     ,
                                                      2
                                                    4s ρ α  ρ α
                                                (       p 2    1  )
                                       m 21 = 2ik q 1 +  2 1  −   ,
                                                      4q ρ α  ρ α
                                                        1
                                                (       p 2    1  )
                                       m 22 = 2ik q 2 +  2  −     ,
                                                        2
                                                      4q ρ α  ρ α
                                                        2
                                                        (  1   1  )
                                                     2
                                                2
                                       m 23 = −s − k +      −     s,
                                                         ρ α   ρ β
                                                       [                      ]
                                                                 (  1    1  )
                                                              2
                                                         2
                                       m 31 = (Q + Rη 1 ) q − k +     +     q 1 ,
                                                         1
                                                                   ρ α  ρ β
                                                       [                      ]
                                                                 (  1    1  )
                                                              2
                                                         2
                                       m 32 = (Q + Rη 2 ) q − k +     +     q 1 ,
                                                         1
                                                                   ρ α  ρ β
                                       m 33 = 0.
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